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<rss version="2.0">
<channel>
<title>ADS (Cites/AR query)</title>
<link>https://ui.adsabs.harvard.edu</link>
<description>The SAO/NASA ADS Abstract service provides a search system for the Astronomy and Physics literature</description>
<image>
<url>http://ads.harvard.edu/figs/ads_icon_144.png</url>
<title>SAO/NASA ADS</title>
<link>https://ui.adsabs.harvard.edu</link>
<width>144</width>
<height>122</height>
</image>

<item>
<title> Operational space weather detection and tracking using small spacecraft</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AcAau.241..245M</link>
<description>One of the greatest challenges facing current space weather monitoring
operations is forecasting the arrival of coronal mass ejections (CMEs)
and solar energetic particles (SEPs). This paper presents a mission
concept for operational detection and monitoring of solar weather events
as a means of forecasting the arrival of potentially hazardous CMEs and
SEPs at Earth-like distances. Foregrounding the operational (rather than
scientific) requirements of the system, this work proposes a high-level
mission design that could provide detection of solar weather events by
tracking associated solar radio bursts, enabling advanced warning of
their arrival at Earth. This work concludes that 35 small spacecraft
equipped with radio spectrometers positioned at the SunEarth Lagrange
points and in Earth-leading/-trailing orbits could be used to provide
this capability, with the &lt;mml:math&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;L&lt;/mml:m
i&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;4&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mat
h&gt; and &lt;mml:math&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;L&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:m
row&gt;&lt;mml:mn&gt;5&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:math&gt; Lagrange points
most advantageous for mission performance. While technical developments
in CubeSat survivability would be required to enable the SURROUND
mission, suitable launch, injection and communication options are
identified, indicating its potential feasibility in the near future.</description>
</item>
<item>
<title> The POEMAS solar radio telescope evaluation without HPC</title>
<link>https://ui.adsabs.harvard.edu/abs/2026A&amp;C....5501053C</link>
<description>The increasing temporal resolution and structural diversity of modern
solar instruments place growing demands on database systems used in
observational astronomy. At the Center for Radio Astronomy and
Astrophysics Mackenzie (CRAAM), this challenge is amplified by the need
to consolidate heterogeneous data streams from multiple telescopes
within a single virtual machine. With only 32GB of RAM available (16GB
allocated to the database), a central design question emerged: when
restricted to a single physical host, can a virtualized sharded cluster
offer practical scalability advantages over a standalone deployment? To
investigate this, we conducted an empirical evaluation of MongoDB using
10ms observations from the POEMAS radiotelescope, tested at volumes of
15M, 150M, and 500M documents. Results show that, although sharding
introduces coordination overhead for selective queries, it provides
substantial gains for global aggregations, achieving speedups above
600&lt;mml:math&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:math&gt; while maintaining compression
ratios near 85%. The analysis identifies an operational threshold of
roughly 150 million documents per collection to sustain stable
performance under the available resources. Based on these findings, the
same single-node configuration used in the benchmarks was employed to
process the full historical POEMAS dataset, totaling 3.3 billion records
and producing approximately 50GB of consolidated FITS products. These
products and their associated metadata are made available to the
community through a cloud-hosted portal with reduced operational cost.
This work documents practical scalability boundaries for astronomical
time-series in resource-constrained environments and supports the
deployment currently operating at CRAAM.</description>
</item>
<item>
<title> Dataset for Recognition and Detection Based on Solar Radio Spectrogram Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2026RAA....26c7001L</link>
<description>With the increasing volume of solar radio spectrogram observation data,
deep learning-based recognition and detection of solar radio bursts have
become a key research direction. However, most studies on meter-wave
solar radio spectrogram recognition and detection rely on proprietary
datasets, and publicly available datasets remain scarce. To address this
issue and facilitate the use of public datasets for deep learning model
validation, thereby promoting the development of automatic detection
methods for meter-wave solar radio spectrogram, we propose a new solar
radio spectrogram dataset. The dataset is constructed from meter-wave
solar spectrogram observation data from the Learmonth Observatory in
Australia and the meter-wavelength observing system of the Chashan Solar
radio Observatory (CSO) of Shandong University. Experimental results
demonstrate that the proposed dataset effectively supports the
recognition and detection of solar radio spectrograms, providing
essential data resources for the intelligent recognition of solar radio
burst features.</description>
</item>
<item>
<title> Large area and long-distance ionospheric D region virtual height determination method using lightning VLF electric field waveforms</title>
<link>https://ui.adsabs.harvard.edu/abs/2026Meas..26320193H</link>
<description>This paper introduces a highly effective method for real-time
determination of the large-scale ionospheric D region virtual height
using lightning electromagnetic pulses (LEMP). Utilizing lightning
location and very low frequency (VLF) electric field waveform data from
the Asia-Pacific Lightning Location Network (APLLN), the method can
cover most regions of China with just 15 LEMP detection sites. It
analyzes the arrival times of ground wave, first-hop, and second-hop sky
waves in the 330 kHz cloud-to-ground lightning return stroke electric
field waveforms to derive ground wave propagation delay and D region
virtual height results. Using these results during Mclass solar flare
events, our analysis shows a linear dependence of D region virtual
height on the logarithm of solar X-ray intensity (0.10.8 nm), with a
height descent rate of 5.97 km/decade and a 12 min ionospheric
response delay. It shows remarkable effectiveness in monitoring the
impact of solar flares on D region virtual height. Its advantages lie in
achieving extensive D region virtual height coverage with fewer
lightning detection stations, offering richer data support for
statistical analysis and potential applications in radio wave
propagation studies.</description>
</item>
<item>
<title> From Blazar to Magnetar and Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...999..246Z</link>
<description>Using Gaussian process methods, we analyzed the light curves of three
extreme solar X-ray flares observed by the RHESSI satellite. Their
variability characteristics were then compared with those of HXMT-HE
X-ray burst (XRB; in SGR 1935+2154) associated with fast radio burst
(FRB) 200428 and blazar -ray giant flares to investigate the origins of
these extreme flaring events. The variability patterns of the solar
X-ray flares follow the stochastically driven damped simple harmonic
oscillator model. The derived timescales t&lt;SUB&gt;B_steep&lt;/SUB&gt; and
t&lt;SUB&gt;B_flat&lt;/SUB&gt; (corresponding to power spectral density breaks) are
in the range of 47 and 1653 s, respectively. The FRB-associated HXMT-
HE burst has a Q value near 0.3, matching those of the solar flares that
occurred on 2002 July 23 (flare 1) and 2003 November 3 (flare 2). By
contrast, blazar -ray giant flares show Q &gt; 0.3, similar to the solar
flare that occurred on 2014 February 25 (flare 3). We proposed that the
critically damped state of the system may be the condition triggering
the association between the XRB in SGR 1935+2154 and the FRB. In this
scenario, the critical damping Q value of the system is around 0.3, not
the theoretical 0.5. The similarity in Q values might imply that the
FRB-associated HXMT-HE XRB and solar X-ray flares 1 and 2 share
comparable dynamic behavior, while blazar -ray flares and solar X-ray
flare 3 exhibit another distinct but similar dynamic behavior. Like
solar X-ray flares, these extreme flares may all be related to the
magnetic reconnection process.</description>
</item>
<item>
<title> Dynamics of the Coronal Magnetic Field in the 2022 October 2 X-class Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...999..179F</link>
<description>Solar flares are driven by the release of free magnetic energy and are
often associated with the restructurization of the magnetic field
topology. Yet, observations of the evolving magnetic field in the
flaring volume are limited to very few cases, including the 2017
September 10 X8.2 limb flare; thus, a verification of whether a similar
evolution takes place in other solar flares is needed. Here, we report
one more: the 2022 October 2 X1.1-class solar flare, seen on the disk,
whose microwave data permit mapping the magnetic field over the flaring
source and tracking the magnetic field evolution over the course of the
flare. We find that the coronal magnetic field shows a prominent decay
with a rate up to 10 G s&lt;SUP&gt;1&lt;/SUP&gt; in several (above the) looptop
locations. The magnetic field is also confidently measured at the loop
legs and the bottom part of the erupting filament. Prominent
acceleration of electrons is detected where the magnetic field decays.
We develop 3D models of the flare, whose magnetic field shows
resemblance to and also deviation from the magnetic field inferred from
the microwave data. This study confirms that the coronal magnetic field
decays during the rise phase of the solar flare. The amount of released
magnetic energy is sufficient to support other components of the flare
energy.</description>
</item>
<item>
<title> Signatures of Large-scale Magnetic Field Disturbances and Switchbacks in Interplanetary Type III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...999..134C</link>
<description>Type III solar radio bursts are driven by nonthermal electron beams
travelling along heliospheric magnetic fields, with the radio emission
frequency drift rate determined by the beam speed and the plasma density
profile. Analyzing beam kinematics inferred from the drift rate reveals
behavior inconsistent with the emitter moving radially through smooth,
monotonically decreasing density. We examine whether these features are
driven by disturbances in the guiding magnetic field direction, such as
switchbacks, rather than plasma inhomogeneities along the beam path.
Using simulations and remote observations of 24 interplanetary type III
bursts observed by Parker Solar Probe, we relate measured drift rate
variations to local field deflections. In 50% of events, we identify
disturbances above a 2 noise level that can be attributed to
perpendicular deflections of the field between (0.7 and 1.7)
R&lt;SUB&gt;&lt;/SUB&gt;, over scales (1.86.4) R&lt;SUB&gt;&lt;/SUB&gt; at heliocentric
distances (930) R&lt;SUB&gt;&lt;/SUB&gt;. The features correspond to either
density changes of (10%30%), or deflections of the field direction by
(2388). Further, beam transport simulations show field direction
perturbations produce additional observational signatures in type III
bursts: delayed emission, intensity breaks, and enhanced emission
resembling stria fine structures. In addition, we identified four bursts
where the observed variations are more plausibly explained by field
deflections, possibly in the form of magnetic switchbacks than by
unrealistically large density changes along the field line. The results
show that variations in type III burst profiles can arise from magnetic
as well as density fluctuations and demonstrate the value of type III
bursts as remote probes of inner-heliospheric structure at kilometric
wavelengths.</description>
</item>
<item>
<title> Herringbone Structures during an X-class Eruptive Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...999...66Z</link>
<description>In this paper, we report quasiperiodic herringbone structures during the
impulsive phase of an X-class flare, coinciding with the distinct
acceleration phase of eruptive prominence ejection on 2023 December 31.
The prominence propagates nonradially in the southeast direction with an
inclination angle of 35.4. The fast coronal mass ejection (CME) at a
speed of 2852 km s&lt;SUP&gt;1&lt;/SUP&gt; drives a shock wave and a coronal
extreme-ultraviolet wave. The herringbone structures lasting for 4
minutes take place at the initial stage of a group of type II radio
bursts. The herringbones in the frequency range 2070 MHz are
characterized by simultaneous forward-drift and reverse-drift bursts
with average durations of 2.5 and 3.1 s. The frequency drift rates of
these bursts fall in a range of 1.39.4 MHz s&lt;SUP&gt;1&lt;/SUP&gt; with average
values of 3.6 and 4.1 MHz s&lt;SUP&gt;1&lt;/SUP&gt;, respectively. The speeds of
electron beams producing the herringbones are estimated to be
0.04c0.41c, with average values of 0.23c and 0.11c for forward-
drifting and reverse-drift bursts, respectively. The heights of particle
acceleration regions are estimated to be 0.640.78 R&lt;SUB&gt;&lt;/SUB&gt; above
the photosphere, which are consistent with the height of the CME front
(0.75 R&lt;SUB&gt;&lt;/SUB&gt;) when the shock forms. Quasiperiodic pulsations
with periods of 17.521.3 s are found in the radio fluxes of
herringbones, suggesting that electrons are accelerated by the CME-
driven shock intermittently.</description>
</item>
<item>
<title> Complexity and scaling descriptors as diagnostic predictors of heliophysical indices across solar-cycle timescales</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.6645S</link>
<description>Heliophysical variability emerges from a coupled, multiscale system in
which changes in the solar atmosphere and heliospheric plasma translate
into measurable signatures in widely used activity indices. Operational
space-weather workflows often summarize this variability through
amplitudes and a small set of bulk solar-wind covariates, yet important
dynamical information may also reside in the evolving morphology of the
signals. We examine whether shape descriptors computed from
heliophysical time series provide information beyond classical amplitude
summaries and standard bulk solar-wind covariates. Using daily OMNIWeb-
era records spanning 19642025, we compute ten sliding-window
descriptors under a past-only convention, designed to capture
complementary aspects of temporal morphology such as irregularity,
roughness, and long-range dependence. The descriptor set combines
entropy measures, fractal-dimension estimators, the Hurst exponent, and
LempelZiv (LZ) complexity, yielding a compact representation of time-
series structure that is not reducible to amplitude alone. The window
length is treated as a methodological hyperparameter and selected
through a target-specific sensitivity analysis that jointly favors
competitive out-of-sample RMSE and stable permutation-importance
rankings across neighboring windows. Two complementary learners,
gradient boosting and a multilayer perceptron, are used as diagnostic
probes to quantify permutation-based feature relevance under
chronological splitting and training-only preprocessing. Across three
targets (F10.7, Sunspot Number, and Dst), shape descriptors consistently
rank among the most informative predictors, often matching or exceeding
the relevance of standard solar-wind inputs. The most robust signals
arise from LZ complexity and a compact subset of entropy/fractal
measures, whose windowed trajectories track solar-cycle phases with
characteristic leadlag behaviour. Correlation analyses on both levels
and standardised first differences expose redundancy within descriptor
families and reduce spurious associations driven by shared
nonstationarity, motivating a family-level interpretation of relevance
rather than causal attribution. Overall, the results indicate that
heliophysical time-series morphology encodes dynamical information
complementary to amplitude- and bulk-plasma descriptions, suggesting
compact, instrument-light features for augmenting future space-weather
modelling pipelines.</description>
</item>
<item>
<title> Statistical investigation of Langmuir waves in Type III and II sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.6530C</link>
<description>Type II and III solar radio bursts involve electron beams driving
Langmuir waves that then couple wave energy into radio emission. These
Langmuir waves can be driven to large enough amplitudes that they
undergo electrostatic (ES) decay into a backward propagating Langmuir
wave and a forward propagating ion acoustic wave. The forward and
backwards propagating Langmuir waves can then "beat" together to produce
characteristic Langmuir waveforms and spectra, plus radio emission.
Stochastic growth theory (SGT) predicts that the probability
distribution of the Langmuir wave electric field strength should be
lognormal, with known modifications if nonlinear processes like ES decay
are occurring at high fields. Other analyses suggest the more general
set of Pearson distributions may be relevant. Here, previous work on
Langmuir waves in type II and III source regions is generalized and
tested by analysing the probability distributions of the waveforms of
Langmuir waves observed by the STEREO spacecraft. The focus is on a set
of published events identified using spectral analyses to have or not
have spectral evidence for ES decay. For events for which spectral
analyses provide evidence of ES decay, &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;92&lt;/m
ml:mn&gt;&lt;mml:mspace&gt;&lt;/mml:mspace&gt;&lt;mml:mo&gt;%&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;
of the probability distributions are consistent with the combination of
SGT and a nonlinear process like ES decay, while &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mm
l:mn&gt;68&lt;/mml:mn&gt;&lt;mml:mspace&gt;&lt;/mml:mspace&gt;&lt;mml:mo&gt;%&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/
mml:math&gt; of those without spectral evidence for ES decay are better
fitted by pure SGT. Better fits with stronger statistical significance
are obtained for pure and nonlinear SGT than for Pearson distributions
in the majority of events (&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:mn
&gt;90&lt;/mml:mn&gt;&lt;mml:mspace&gt;&lt;/mml:mspace&gt;&lt;mml:mo&gt;%&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:
math&gt;). These results provide strong evidence for SGT and ES decay
proceeding in type II and III source regions, particularly type III
source regions.</description>
</item>
<item>
<title> Three-dimensional mapping of coronal magnetic field and plasma parameters in a solar flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2026A&amp;A...707A.158K</link>
<description>Aims. Diagnosing solar flare conditions is essential for understanding
coronal energy release. Using combined microwave and X-ray data, we aim
to reconstruct 3D maps of the magnetic fields and plasma parameters in
the SOL2021-05-07 flare. Methods. We used imaging spectroscopy from the
Expanded Owens Valley Solar Array (EOVSA) to derive spatial maps of the
magnetic field strength, as well as the thermal and nonthermal electron
densities, along with the power-law index of nonthermal electrons via
gyrosynchrotron modeling. Simultaneous X-ray observations from
Hinode/X-Ray Telescope (Hinode/XRT) and Solar Orbiter/Spectrometer
Telescope for Imaging X-rays (SolO/STIX), taken from different vantage
points, enable a stereoscopic reconstruction of the flaring loop. By
correlating the positions of microwave and thermal X-ray sources, we
associated the 3D coordinates with the microwave-derived plasma
parameters. Results. We derived observational 3D maps of magnetic field
strength, Alfvn speed, and plasma beta in a flaring volume, revealing a
magnetically dominated environment. These spatially resolved diagnostics
provide valuable constraints for models of magnetic reconnection and
flare dynamics, representing a step toward a realistic 3D
characterization of energy release in solar eruptive events.</description>
</item>
<item>
<title> How Good Are GOES XRS Temperatures and Emission Measures?</title>
<link>https://ui.adsabs.harvard.edu/abs/2026SoPh..301...28W</link>
<description>The soft X-ray (SXR) measurements made by NOAA's GOES weather satellites
are an important resource for solar physics and space weather. In
particular, they are extensively used to study the energetics of solar
flares via temperatures and emission measures derived from the SXR data.
However, the SXR instruments measure just two channels, 0.5  4  and 1
 8 : with just two data points, it is only possible to represent the
flare plasma with a single temperature component, whereas it is well
known that a flare can display a wide range of temperatures at any given
time. In order to assess how representative the GOES SXR temperatures
and emission measures are, we compare GOES measurements with EUV data
for six spectral lines of Fe that cover the typical temperature range of
flares, 10  20 MK. From a sample of 23 large flares, we find that the
GOES temperatures match the emission-measure-weighted EUV temperatures
surprisingly well, but (assuming photospheric abundances) the GOES
emission measures are smaller than the EUV emission measures by up to
50%, with the discrepancy larger at higher temperatures.</description>
</item>
<item>
<title> Fast variability and circular polarization of the 6.7 GHz methanol maser in G33.641-0.228</title>
<link>https://ui.adsabs.harvard.edu/abs/2026PASJ..tmp...24F</link>
<description>The 6.7 GHz methanol maser in a high-mass star-forming region
G33.6410.228 is known to exhibit burst-like flux variability due to an
unknown mechanism. To investigate the burst mechanism, we conducted
high-cadence flux and circular polarization monitoring observations,
simultaneously using left- and right-hand circular polarizations. We
found that the flux density increased and decreased on a short timescale
of 0.3 d during a burst. We also found strong circular polarization,
reaching up to 20% in the component exhibiting the bursts. Circular
polarization of 0%-20% was continuously observed from 2009 to 2016, even
in the quiescent period. The polarization also varied on timescales of
less than one day. When a burst occurred and the flux density increased,
the circular polarization decreased to zero. To explain the
observational properties of the flux variability and circular
polarization, we propose a model in which an explosive event similar to
a solar radio burst occurs on the line of sight behind the maser cloud,
producing circularly polarized continuum emission due to gyro-
synchrotron or gyro-resonance radiation, which is then amplified by the
maser.</description>
</item>
<item>
<title> Daily Predictions of F10.7 and F30 Solar Indices With Deep Learning</title>
<link>https://ui.adsabs.harvard.edu/abs/2026JGRA..13134868W</link>
<description>The F10.7 and F30 solar indices are the solar radio fluxes measured at
wavelengths of 10.7 and 30 cm, respectively, which are key indicators of
solar activity. F10.7 is valuable for explaining the impact of solar
ultraviolet (UV) radiation on the upper atmosphere of Earth, while F30
is more sensitive and could improve the reaction of thermospheric
density to solar stimulation. In this study, we present a new deep
learning model, named the Solar Index Network, or SINet for short, to
predict daily values of the F10.7 and F30 solar indices. The SINet model
is designed to make medium-term predictions of the index values (160
days in advance). The observed data used for SINet training were taken
from the National Oceanic and Atmospheric Administration as well as
Toyokawa and Nobeyama facilities. Our experimental results show that
SINet performs better than five closely related statistical and deep
learning methods for the prediction of F10.7. Furthermore, to our
knowledge, this is the first time deep learning has been used to predict
the F30 solar index.</description>
</item>
<item>
<title> Solar radio bursts and their applications in space weather forecasting</title>
<link>https://ui.adsabs.harvard.edu/abs/2026FrASS..1388006Z</link>
<description>Not Available</description>
</item>
<item>
<title> Modeling Metric Gyrosynchrotron Radio Emission From the Quiet Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2026BlgAJ..44...28K</link>
<description>The radio emission of the quiet Sun in the metric and decametric bands
has not been well studied historically due to limitations of existing
instruments. It is nominally dominated by thermal brehmsstrahlung of the
solar corona, but may also include significant gyrosynchrotron emission,
usually assumed to be weak under quiet conditions. In this work, we
investigate the expected gyrosynchrotron contribution to solar radio
emission in the lowest radio frequencies observable by ground
instruments, for different regions of the low and middle corona. We
approximate the coronal conditions by a synoptic magnetohydrodynamic
(MHD) model. The thermal emission is estimated from a forward model
based on the simulated corona. We calculate the expected gyrosynchrotron
emission with the Fast Gyrosynchrotron Codes framework by
\cite{Fleishman:2010}. The model emissions of different coronal regions
are compared with quiet-time observations between 20-90 MHz by the LOw
Frequency ARray (LOFAR;\cite{vanHaarlem:2013}) radio telescope. The
contribution of gyrosynchrotron radiation to low frequency solar radio
emission may shed light on effects such as the hitherto unexplained
brightness variation observed in decametric coronal hole emission, and
help constrain measurements of the coronal magnetic fields. It can also
improve our understanding of electron populations in the middle corona
and their relation to the formation of the solar wind.</description>
</item>
<item>
<title> A TimesNet-based Real-time Forecasting System for the F10.7 Index Using DRAO and Chinese Langfang Datasets</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJS..282...52L</link>
<description>In this paper, we construct the DRAO univariate dataset, the DRAO
multivariate dataset, and the Chinese Langfang dataset. We develop and
compare five deep learning models (TimesNet, iTransformer, PatchTST,
N-Beats, BiGRU) and a benchmark artificial neural network (ANN) model to
predict the F10.7 index. We study the impact of different feature
combinations on the performance of the recommended TimesNet model.
Furthermore, we develop a real-time forecasting system for the F10.7
index, incorporating both univariate and multivariate TimesNet models.
During the same period, we compare F10.7 prediction performance between
our system and that of four foreign institutions (British Geological
Survey (BGS), SWPC, Collecte Localisation Satellites (CLS), DRAO). We
conduct daily averaged and hourly resolution forecasting using the
Langfang dataset. To our knowledge, we establish the first TimesNet-
based framework for F10.7 prediction, advancing hourly resolution F10.7
forecasting for the first time. The main results are as follows. (1) The
univariate TimesNet model achieves superior prediction performance on
the first to the 27th day of forecasting, outperforming both four deep
learning models and the ANN model. With the increase in the prediction
days, the prediction performance of the six models all shows a downward
trend. (2) The multivariate TimesNet-FIAC model, using optimal feature
combinations, outperforms the univariate TimesNet-F model. (3) In short-
term prediction, TimesNet-FIAC within our system surpasses four foreign
institutions. On the first forecasting day, its root mean square error,
mean absolute error, and mean absolute percentage error decrease by
15.06%, 18.54%, and 20.90% compared to BGS, and by 3.54%, 10.21%, and
14.94% compared to CLS. (4) On the Langfang dataset, TimesNet-F
demonstrates superior generalization in daily averaged short-term
forecasting, and maintains good and stable performance in hourly
resolution short-term prediction.</description>
</item>
<item>
<title> First Detailed MeerKAT Imaging Spectroscopy of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...998L..46L</link>
<description>Radio observations provide powerful diagnostics of energy release,
particle acceleration, and transport processes in solar flares. However,
despite recent progress in radio interferometric imaging spectroscopy,
current instruments still face limitations in image fidelity and
resolution, restricting detailed spectroscopic studies of flaring
regions. Here we present high-fidelity imaging spectroscopy of an M1.3
GOES class flare with MeerKAT, a precursor to the future-generation
array SKA-Mid. Radio emissions at the observed frequencies typically
originate in the low corona, offering valuable insights into magnetic
reconnection and primary energy-release sites. The obtained images
achieve an unprecedented dynamic range exceeding 10&lt;SUP&gt;3&lt;/SUP&gt;,
enabling simultaneous analysis of bright coherent bursts and faint
incoherent emission from the active region. Multiple spatially distinct
coherent sources are identified, implying contributions from different
populations of accelerated electrons. The incoherent emission extends
beyond Atmospheric Imaging Assembly structures, highlighting MeerKAT's
ability to detect dilute but hot plasma invisible to extreme-ultraviolet
instruments. Combined with cotemporal hard X-ray images and magnetic
field extrapolations, the radio sources are located within distinct
magnetic structures, further revealing their association with different
populations of accelerated electrons. These results demonstrate MeerKAT
imaging spectroscopy as a powerful diagnostic of solar flares and pave
the way for future solar flare studies with SKA-Mid.</description>
</item>
<item>
<title> The Spectral Features of Single-band Type III-like Radio Bursts Observed by PSP during Its First Nine Orbital Encounters</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...998..316M</link>
<description>The spectral features of 1122 single-band type III-like radio bursts
were analyzed statistically using data from the Parker Solar Probe (PSP)
during the first nine orbital encounters. After excluding overlapping
events, 923 bursts were classified into 706 complete-spectrum (CS)
bursts and 217 incomplete-spectrum (IS) bursts depending on radiation
completeness. The distribution of start frequency f&lt;SUB&gt;st&lt;/SUB&gt; for IS
events (2054 MHz) was predicted by a lognormal fit. The higher cutoff
frequency (f&lt;SUB&gt;lo&lt;/SUB&gt;  1.21.6 MHz) than previous results may be
attributed to the limitation of exciting conditions or the radial
expansion of guiding magnetic flux tubes. Short durations (14 minutes)
and low peak fluxes (10&lt;SUP&gt;3&lt;/SUP&gt; sfu) indicate that most events are
short-time weak bursts. The spectral index of duration versus frequency
is near 1, which reflects the influence of velocity dispersion and
radio-wave scattering. For the denoised spectra of CS events, the peak
frequency of maximal flux (4.5 MHz) is obviously higher than those from
STEREO (1 MHz) and WIND ( 2 MHz). This implies that the radiation may
be the second or third harmonic wave rather than the fundamental wave.
Statistical frequency drift rates follow the classical power-law
relation (D&lt;SUB&gt;abs&lt;/SUB&gt;  f&lt;SUP&gt;1.84&lt;/SUP&gt;) and are consistent with
simulation results of typical type III radio bursts. CS and IS bursts
show similarities in f&lt;SUB&gt;lo&lt;/SUB&gt;, duration, and drift features, but
obviously differ in the peak frequency of maximal flux. These results
can provide a useful reference for further exploring the emission
mechanisms of single-band type III-like radio bursts and the associated
energetic electron acceleration processes.</description>
</item>
<item>
<title> Comparisons of Intervals with and without Type III Storms</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...997..333C</link>
<description>Solar p-modes are 5 minute acoustic waves, which can be used as
helioseismological diagnostics of the Sun's subsurface. Recent studies
relate them to quasiperiodic pulsations (QPPs) identified in X-rays,
radio waves, and extreme ultraviolet (EUV) emission. QPPs with 5 minute
periods have been simultaneously observed in Solar Dynamics Observatory
(SDO) EUV measurements and Parker Solar Probe (PSP) observations of Type
III radio storms, suggesting a link between p-modes and electron
acceleration. Using examples when potential field source surface mapping
indicated that PSP and SDO were magnetically connected, we compared
periodicities in intervals with ("loud") or without ("quiet") coincident
Type III radio storms, and looked for small jets (jetlets), as
indicators of open field lines enabling electrons to escape and produce
radio waves. QPPs of 310 minutes occurred in EUV and Helioseismic and
Magnetic Imager (HMI) data in all intervals. Whereas the p-mode
amplitudes in photospheric EUV and HMI data were similar in "quiet" and
"loud" events, amplitudes in coronal EUV waves were approximately an
order of magnitude larger during "loud" intervals. The jetlet rate was
comparably higher during "loud" times, consistent with the low corona as
the source of electron beams producing Type III waves. The larger EUV
amplitudes and higher jetlet rates during "loud" intervals indicate that
the presence of electron acceleration along open field lines depends
strongly on QPP magnitude and the associated magnetic field
configuration. These findings provide new insights into the conditions
under which p-mode energy can leak from the photosphere into the corona.</description>
</item>
<item>
<title> Longitudinal variation in the ionospheric responses to two successive geomagnetic storms in early Solar Cycle 25</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.5222N</link>
<description>This study examines the ionospheric response over different longitude
sectors to two consecutive minor to moderate storms of Solar Cycle 25
that occurred on 34 November 2022 and 78 November 2022, using Total
Electron Content (TEC) measurements from the SWARM-A satellite. The
first storm, occurring on 34 November, was driven by a Corotating
Interaction Region (CIR) and characterized by a gradual commencement,
while the second storm on 78 November was driven by a Coronal Mass
Ejection (CME). On 7 November 2022 at 00.11 UT, a powerful impulsive
M5-class solar flare erupted from Sunspot AR3141, resulting in
significant ionization of the upper atmosphere and triggering a
shortwave radio blackout across the South Pacific region, including
parts of Australia and all of New Zealand. The initial storm led to
widespread positive ionospheric storm effects globally during both dawn-
side and dusk-side hours. The subsequent storm exhibited cumulative
effects, producing pronounced positive storm conditions, particularly
over the East Pacific, Asia-Pacific, and Australian sectors. Over the
American sector, the second storm also produced a notable hemispheric
asymmetry in the SWARM-TEC distribution during the morning hours, with
enhanced TEC in the Southern Hemisphere and a flattened profile in the
Northern Hemisphere. This asymmetry is attributed to storm-time
equatorward winds and composition-driven differences in electron density
loss. Compositional changes during these geomagnetic storms were
investigated using O/N&lt;SUB&gt;2&lt;/SUB&gt; ratio observations from TIMED/GUVI,
highlighting thermospheric responses to solar and geomagnetic
disturbances. Additionally, temporal variations in the Equatorial
Electric Field (EEF), derived from real-time modelling, were analysed to
evaluate fluctuations in the equatorial eastward electric field across
the studied longitude sectors, providing insights into the
electrodynamic processes driving the observed ionospheric variability.
The occurrence of two closely spaced geomagnetic storms allowed us to
uniquely quantify the cumulative impact of successive solar disturbances
on global TEC variability, revealing pronounced longitudinal and
hemispheric asymmetries not previously characterized in detail for Solar
Cycle 25.</description>
</item>
<item>
<title> CLEAN and multiscale CLEAN for STIX in Solar Orbiter</title>
<link>https://ui.adsabs.harvard.edu/abs/2026A&amp;A...706A.360C</link>
<description>CLEAN is a well-established deconvolution approach to Fourier imaging at
radio wavelengths and hard X-ray energies. One of the main limitations
of CLEAN for hard X-ray imaging is that it requires a final convolution
step by means of a convolution kernel whose width is strongly user
dependent, and moreover, under-resolution effects are often introduced.
This paper describes a multiscale version of CLEAN that is specifically
tailored to the reconstruction of images from measurements observed by
the Spectrometer/Telescope for Imaging X-rays (STIX) on board Solar
Orbiter. Using synthetic STIX data, this study shows that multiscale
CLEAN might represent a reliable solution to the two CLEAN limitations
described above. Further, we show the performances of CLEAN and its
multiscale release in reconstructing experimental real scenarios
characterized by complex emission morphologies.</description>
</item>
<item>
<title> A solar jet-induced perturbation propagating through coronal loops and in-loop electron beam transport as indicated by type II and type N radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2026A&amp;A...706A.197C</link>
<description>Aims. Solar type II radio bursts are commonly attributed to coronal
shocks driven by coronal mass ejections (CMEs). However, some metric
type II bursts have occasionally been reported to occur in the absence
of a CME and to be associated with weak solar activity. The aim of this
study is to identify the driver of the coronal shock in this kind of
type II event. Methods. We investigated a high-frequency metric type II
burst with clear band splitting, observed simultaneously by the Chashan
Broadband Solar radio spectrograph and the Nanay Radioheliograph. It is
associated with a C3.1-class flare and a small-scale jet, but without a
detectable CME in the coronagraphs. Results. The type II burst is
preceded by multiple type III bursts, one of which exhibits
characteristics of a type N burst. The type II burst source is
associated with the jet-induced perturbation front propagating through
nearby closed loops at a speed of 880 km s&lt;SUP&gt;1&lt;/SUP&gt;, rather than
the much slower jet front. This suggests that the disturbance initiated
by the jet can convert to a shock wave within low Alfvnic coronal
loops, providing the necessary conditions for electron acceleration and
subsequent radio emission. Our findings offer new insights into the
formation mechanism of high-frequency type II bursts associated with
weak flares and jets.</description>
</item>
<item>
<title> Radio, X-ray, and extreme ultraviolet signatures of internal and external reconnection of an erupting flux rope</title>
<link>https://ui.adsabs.harvard.edu/abs/2026A&amp;A...706A.143K</link>
<description>Aims. We aim to interpret and relate features observed in gigahertz
radio, extreme UV (EUV), and X-ray emissions during a filament eruption
at the start of a solar flare on 2 April 2022. Methods. We analysed
imaging (EUV, X-ray) and spectral (radio, X-ray) data obtained by
ground-based and space instruments on board space missions both on Earth
(Fermi, Hinode, Solar Dynamics Observatory) and in solar orbits (Solar
Orbiter, STEREO-A), thus providing a multi-directional view on the same
event. Results. The combination of EUV and X-ray images and X-ray
spectra allowed us to identify hot loops in the vicinity of the filament
before its eruption. We interpreted their interaction with the rising
filament as a signature of an arcade-to-rope reconnection geometry. The
subsequent EUV brightening within the filament revealed a helical
structure of the erupting rope. We explain co-temporal radio slowly
positively drifting bursts as being a result of beam acceleration within
the magnetic rope and propagation along the helical structure. The
corresponding X-ray spectra are consistent with a thermal origin. The
filament rising was accompanied by co-temporal normal and reverse drift
type III radio bursts. We interpret them as a signature of a
reconnection event and estimated the electron density at the
reconnection site. Further untwisting of the helical structure led to
formation of a quasi-circular EUV structure seen from Earth and
STEREO-A. Its occurrence was co-temporal with a unique tangle of radio
U- and inverse U-bursts. We propose that several accelerated beams
propagate within that complex structure and generate the burst tangle.
During the start of the flare, hard X-ray emission was concentrated near
the filament leg only, suggesting predominant propagation of the beams
towards its rooting. Conclusions. We collected multi-wavelength
observations indicating interaction of the erupting magnetic flux rope
with the overlying arcade and internal magnetic reconnection inside the
rising flux rope.</description>
</item>
<item>
<title> The Chinese Radio Telescope Array for Interplanetary Scintillation Monitoring</title>
<link>https://ui.adsabs.harvard.edu/abs/2026SpWea..2404593Y</link>
<description>Solar flares, coronal mass ejections (CMEs) and enegertic particles,
etc., are the driving sources that may cause catastrophic space
weathers. It is desirable to obtain information of solar eruptions like
flares and CMEs, etc., propagating from the Sun to the near-Earth space.
The Chinese Meridian Project includes the interplanetary scintillation
(IPS) telescopes to investigate the structures and properties of the
solar wind throughout the inner heliosphere. From IPS observations one
can obtain disturbance information on CME speeds and thus on CME arrival
times well off the Sun-Earth line. When combined with modeling
techniques and/or in situ data, other parameters such as CME masses can
also be obtained, along with CME propagation directions and arrival
times. Therefore, a radio telescope array with three 140 m ${\times} $
40 m parabolic cylinder antennas at the main site and two ${\Phi }$30 m
antennas at two subsites about 200 km away from each other, featuring a
multi-site array with the highest sensitivity dedicated to IPS
observations in the world, has been supported as a major facility of the
Chinese Meridian Project. The detailed description of the final
optimized design and implementation of this IPS radio telescope array is
introduced. The antennas and array configuration, the analog and digital
receiving systems for the main site and subsites, the calibration of the
IPS telescope array and data processing are described. Finally the
overall performance of the IPS telescope array is provided. The detailed
information on the IPS radio telescope array will facilitate the use of
its data serving space weather research and applications.</description>
</item>
<item>
<title> Shock Signatures of the Successive Type-II Solar Radio Bursts at Meter Wavelength</title>
<link>https://ui.adsabs.harvard.edu/abs/2026SoPh..301...20V</link>
<description>The successive type-II solar radio bursts observed on 31 July 2012 by
the Bruny Island Radio Spectrometer (BIRS) in the frequency range
between 62  6 MHz is reported and analyzed. The first type-II radio
burst shows clear fundamental and harmonic band structures, while only
one band is observed for the second type-II radio burst and is
considered as the harmonic band. The first type-II radio burst is
observed in the frequency range of 57  27 MHz between 00:03  00:09 UT
at the harmonic band. The second type-II burst is observed between 00:18
 00:27 UT in the frequency range of 43  17 MHz. The type-II radio
bursts are associated with a C6 class flare located at the southeastern
limb (S24E87) and a CME observed from STEREO and LASCO observations. The
EUVI signatures of the CME are observed in the STB EUVI FOV between
23:56 (on 30 July 2012) to 00:06 UT (on 31 July 2012), and in the ST-B
COR1 FOV between 00:10  00:35 UT moving within an average speed of 725
 101 km s&lt;SUP&gt;1&lt;/SUP&gt;. The CME is observed in the LASCO C2 FOV after
00:12 UT as a partial halo CME moving with an average speed of 486 km
s&lt;SUP&gt;1&lt;/SUP&gt;. The height-time plot shows that the first type-II radio
burst was formed by the CME-shock along the shock front and the second
type-II radio burst along the shock-dip structure, probably the dip
structure results from the shock transiting across the high dense
streamer structure. The successive type-II bursts are most likely
produced by the single CME shock and their interactions with the
streamer structures. The first type-II radio burst by the CME shock and
the second type-II radio burst by the CME shockstreamer interactions.</description>
</item>
<item>
<title> Investigating the interplanetary causes of severe geomagnetic storms during solar cycle 23 using SYM-H and OMNI data</title>
<link>https://ui.adsabs.harvard.edu/abs/2026RLSFN.tmp....1K</link>
<description>During Solar Cycle 23, a detailed analysis was conducted to identify the
interplanetary drivers of severe geomagnetic storms (Dst  - 150 nT) and
to investigate their dependence on solar cycle phases. All such storms
were associated with prolonged intervals of southward interplanetary
magnetic field (IMF Bz), emphasizing magnetic reconnection as the
dominant triggering mechanism. Using OMNI data, key interplanetary
parameters (B, Bz, Vsw, Dsw, Tsw) and geomagnetic indices (Kp, Ap,
SYM-H) were examined, along with solar proxies (Sunspot Number, SSN; and
solar radio flux, F10.7). The results indicate that most severe storms
were driven by four primary interplanetary structures: magnetic clouds
with shocks (sMC, 30.4%), sheath fields (Sh, 30.4%), combined sheath-
magnetic cloud events (Sh + MC, 17.4%), and non-magnetic cloud ICMEs
(non-MC, 17.4%), with complex structures contributing only 4.3%.
Together, these accounted for roughly 75% of all severe storms during
Solar Cycle 23. In terms of solar cycle dependence, sMCs and sheaths
were the most frequent drivers during the rising phase, sheath fields
dominated during solar maximum, and sMCs, sheaths, and CIRs were the
primary contributors during the declining phase. The analysis further
confirms that interplanetary magnetic field strength (B, Bz) and solar
wind conditions (Vsw, Dsw, Tsw) are more directly responsible for storm
intensity than solar proxies (SSN, F10.7), reinforcing the importance of
interplanetary monitoring for space weather forecasting.</description>
</item>
<item>
<title> Design of a New Solar Radio Observing System Working in 36 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2026PASP..138a4504Y</link>
<description>Solar radio bursts from decimeter to centimeter wavelength originate
from radiations from coherent to incoherent mechanism. This spectral
domain hosts a rich variety of fine structures that encode critical
information about energetic electron beams, coronal magnetic fields, and
ambient plasma conditionskey elements for understanding particle
acceleration and energy release during solar flares. To exploit this
diagnostic potential, a broadband observing system with high time and
frequency resolution is essential. In this study, we designed and
developed the Chashan Broadband Solar Decimetric Spectrometer (CBSdm),
which enables high-precision observation of solar radio bursts in the
36 GHz frequency band. The system employs a 6 m parabolic antenna with
a log-periodic dipole array feed, and utilizes nanosecond-level
microwave switching technology to construct a dual-channel analog
receiving chain (3.14.4 GHz/4.65.9 GHz). Real-time spectral processing
is achieved via a 14-bit 3 GSPS analog-to-digital converter and an Field
Programmable Gate Array-based digital backend. Key performance metrics
include a noise figure of 2 dB, sensitivity of 77.9 dBm@2.6 GHz, and
system linearity better than 0.998. Relative calibration was performed
and cross-validated with data from the Learmonth Observatory. Since its
deployment in 2023 October, the system has successfully captured X-class
flare events, with dynamic spectra exhibiting typical continuum features
and multi-frequency synchronous evolution. The coordinated observations
of CBSdm (36 GHz) and CBScm (615 GHz) provide continuous
gyrosynchrotron spectra covering the optically thick to thin transition,
enabling diagnostics of flare magnetic fields and nonthermal electron
distributions.</description>
</item>
<item>
<title> A real-time triggering framework using Yamagawa solar spectrograph for active solar emission observations with the MWA</title>
<link>https://ui.adsabs.harvard.edu/abs/2026PASA...43...11P</link>
<description>Some of the most interesting insights into solar physics and space
weather come from studying radio emissions associated with solar
activity, which remain inherently unpredictable. Hence, a real-time
triggering system is needed for solar observations with the versatile
new-generation radio telescopes to efficiently capture these episodes of
solar activity with the precious and limited solar observing time. We
have developed such a system, Solar Triggered Observations of Radio
bursts using MWA and Yamagawa (STORMY) for the Murchison Widefield Array
(MWA), the precursor for the low frequency telescope of upcoming Square
Kilometre Array Observatory (SKAO). It is based on near-real-time data
from the Yamagawa solar spectrograph, located at a similar longitude to
the MWA. We have devised, implemented, and tested algorithms to perform
an effective denoising of the data to identify signatures of solar
activity in the Yamagawa data in near real time. End-to-end tests of
triggered observations have been successfully carried out at the MWA.
STORMY is operational at the MWA for the routine solar observations, a
timely development in the view of the ongoing solar maximum. We present
this new observing framework and discuss how it can enable efficient
capturing of event-rich solar data with existing instruments, like the
LOw Frequency ARray (LOFAR), Owens Valley Radio Observatory  Long
Wavelength Array (OVRO-LWA), etc., and pave the way for triggered
observing with the SKAO, especially the SKA-Low.</description>
</item>
<item>
<title> Correlation between active regions' spectra at high radio frequencies and solar flare occurrences</title>
<link>https://ui.adsabs.harvard.edu/abs/2026NatSR..1544237M</link>
<description>High radio frequencies observations with the Italian network of large
single-dish radio telescopes resulted in 450 solar images between 2018
and 2023 in K-band frequency range (1826 GHz). Solar radio mapping at
these frequencies allows the probing of the Active Regions (ARs)
chromospheric magnetic field close to the Transition Region, where
strong flares and coronal mass ejection events occur. Enhanced magnetic
fields up to 15002000 G determine anomalous spectra in the ARs
brightness compared to pure free-free emission, due to the addition of a
steeper gyro-resonance component also associated with circular
polarisation up to 40%. When a significant AR spectral flattening is
detected, the probability of a strong flare occurrence within 30 hours
is high (89% in terms of statistical precision). Despite an approximate
weekly cadence of our observations, only 12% of strong flares are
missed/unpredicted within this time interval. Through a correlation
analysis, we assess the trade-off on the sensitivity and the robustness
of this physics-based flare forecast method.</description>
</item>
<item>
<title> Automatic detection of equatorial plasma bubbles using deep neural networks</title>
<link>https://ui.adsabs.harvard.edu/abs/2026JASTP.27806687Z</link>
<description>The equatorial plasma bubble (EPB) is one of the most important
phenomena in the Earth's ionosphere. In this paper, we propose a method
for the EPB image data processing and automatic labeling, utilizing the
Global-scale Observations of the Limb and Disk (GOLD) 135.6 nm nightglow
data. The method extracts the central position of EPBs, significantly
reducing the workload of manual labeling. Through manual analysis, a
dataset of 1,380 image samples was established. Based on the unique
features of EPB images, a deep learning model was developed to improve
detection accuracy. After optimization and validation, the YOLO-LessHead
model achieved a mean Average Precision (mAP@0.5) of 78.39 %, enabling
automatic and accurate identification of EPB images. We used the
developed model to identify and statistically analyze the GOLD airglow
image data from October 2018 to December 2024. The results indicate that
EPB occurrence rates show strong seasonal and longitudinal variability,
with distinct seasonal patterns across different longitudes. The zonal
drift velocities of EPBs increase with enhanced solar radio flux (F10.7)
and decrease as geomagnetic activity (Ap index) intensifies. Drift
speeds are generally higher and more variable at the magnetic equator,
while the northern and southern EIA regions exhibit similar values and
trends.</description>
</item>
<item>
<title> Comparative Analysis of Ground-level Enhancement (GLE) Events and Non-GLE Solar Energetic Particle Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJS..282....1L</link>
<description>This study explores the acceleration origins of solar energetic
particles (SEPs) by analyzing the energy spectral characteristics of
particles in ground-level enhancement (GLE) events and common SEP (non-
GLE) events, as well as the correlations of the peak intensities of
energetic particles with flare and coronal mass ejection (CME)
diagnostic parameters. By examining the peak energy spectra of protons,
for protons with energies &gt;66 MeV, the peak intensities in most GLE
events are significantly higher than those in SEP events, establishing
an energy threshold distinguishing GLE from non-GLE events. Given the
strong correlation between energetic electrons and protons, radio bursts
and soft X-rays (SXRs) produced by energetic electrons can be used to
study acceleration regions of GLE. Based on data from solar cycles 23
and 24, multifrequency radio data (5, 8.8, and 15.4 GHz) and SXR
intensity analysis reveal the heights of particle acceleration. The
results indicate that protons with energies &gt;66 MeV in GLE events are
closely associated with flare-related acceleration in the low corona,
although a contribution from CME-driven shock acceleration cannot be
excluded. In contrast, lower-energy protons (&lt;10 MeV) are primarily
accelerated by CME-driven shocks. Moreover, SEPs at intermediate
energies exhibit a mixed origin, which includes particles accelerated by
both flares and CME-driven shocks. These findings provide key insights
into the mechanisms of particle acceleration in solar events.</description>
</item>
<item>
<title> Improving Hard X-Ray and EUV Diagnostics</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...996...58L</link>
<description>Solar flares effectively accelerate particles to nonthermal energies.
These accelerated electrons are responsible for energy transport and
subsequent emissions in hard X-ray (HXR), radio, and UV/EUV radiation.
Due to the steeply decreasing electron spectrum, the electron population
and consequently the overall flare energetics are predominantly
influenced by low-energy nonthermal electrons. However, deducing the
electron distribution in this energy-containing range remains a
significant challenge. In this study, we apply the warm-target HXR
emission model with kappa-form injected electrons to two well-observed
GOES M-class flares. Moreover, we utilize EUV observations to constrain
the flaring plasma properties, which enables us to determine the
characteristics of accelerated electrons across a range from a few keV
to tens of keV. We demonstrate that the warm-target model (WTM) reliably
constrains the properties of flare-associated electrons, even accounting
for the uncertainties that had previously been unaddressed. The
application of a kappa distribution for the accelerated electrons allows
for meaningful comparisons with electron distributions inferred from EUV
observations, specifically for energy ranges below the detection
threshold of RHESSI. Our results indicate that the accelerated electrons
constitute only a small fraction of the total electron population within
the flaring region. Moreover, the physical parameters, such as electron
escape time and acceleration timescale, inferred from both the WTM and
the EUV observations further support the scenario in which electrons
undergo thermalization within the corona. This study highlights the
effectiveness of integrating the WTM with EUV observations to accurately
characterize energy-containing electrons and their associated
acceleration and transport processes.</description>
</item>
<item>
<title> Microwave Bright Points with Multiple Periodic Oscillations in the Solar Polar Coronal Hole during Solar Cycle Minimum</title>
<link>https://ui.adsabs.harvard.edu/abs/2026ApJ...996...55H</link>
<description>During solar cycle minimum, polar coronal holes show a prominent radio
brightening cap. The analysis of polar microwave enhanced radiation in
polar coronal holes is helpful for understanding the magnetic field
characteristics and the origin of the solar wind. Using the Koshix
synthesis method on Nobeyama Radioheliograph data, we identified
microwave bright points (BPs) superposed on the microwave brightening
cap of the northern polar coronal hole. These microwave BPs manifested
intermittently at fixed locations, with their radiation intensities
displaying multiperiodic oscillations (20 s, 50 s, and 2.5 minutes).
Multiwavelength analysis revealed that nearly all BPs were adjacent to
or coincide with 171  open structures, indicating a strong correlation
between microwave BPs and solar wind, propagating along the open field
lines. At lower layers, BPs were associated with bright ribbons in the
chromosphere and local enhanced magnetic structures in photosphere. The
20 s lifetime of microwave BP enhancement corresponds to their shortest
oscillation period, which, in the temporal characteristics of Alfvn
waves, implies a localized heating or a small-scale magnetic
reconnection process modulated by Alfvn waves at the root of open
magnetic field lines. The microwave 2.5 minute and 171  5 minute
oscillations likely stem from chromospheric and photospheric oscillation
leakage/propagation, respectively. And longer-period (12 minute)
oscillations in 171  open structures may link to large-scale coronal
hole evolution. The multiperiod oscillatory processes in the polar
coronal hole imply complex plasma dynamics inside, which contributes to
our understanding of the origin and propagation of solar wind along the
open structures in the coronal hole.</description>
</item>
<item>
<title> Siberian Radioheliograph image classification using ensemble of CLIP, EfficientNet and CatBoost models</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.2723E</link>
<description>The Siberian Radioheliograph (SRH) is a ground-based radio
interferometer in Irkutsk, Russia, designed for high-resolution solar
observations in the microwave range. It can observe dynamic solar events
with spatial resolutions of 730 arcseconds and temporal resolution up
to 0.1 s. Generating solar radio images from the Siberian
Radioheliograph (SRH) is a multi-step calibration process that corrects
instrumental and atmospheric distortions, using redundancy-based
calibration with both adjacent and non-adjacent antenna pairs to address
phase and amplitude errors in visibility data. The CLEAN algorithm is
then applied to deconvolve the point spread function, reduce sidelobes,
and enhance the visibility of solar features, resulting in higher
quality and more reliable images. While the calibration process
generally improves image quality, it can sometimes result in noisy or
spatially shifted images that are not suitable for scientific use. We
developed a deep learning approach for automatic image quality
classification. The training dataset was prepared using a zero-shot CLIP
model and further validated manually. We evaluated four different
models: a fine-tuned EfficientNet, two CatBoost variants using
embeddings from CLIP and EfficientNet, and an Ensemble model that
combined predictions from all three individual models. The ensemble
model delivered the highest performance and is now used for daily SRH
image classification in the web service.</description>
</item>
<item>
<title> Performance evaluation of NTCM ionospheric model variants (NTCM-GL, NTCM-BC, NTCM-Klobpar and NTCM-GlAzpar) during the 25th solar cycle</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.2588Z</link>
<description>In GNSS navigation and positioning applications, single-frequency users
typically require additional ionospheric Total Electron Content (TEC)
information to correct for signal propagation delays and mitigate
ranging errors. The Global Neustrelitz TEC Model (NTCM-GL), an empirical
model for estimating TEC, has been adapted into three variants through
parameter reduction or driver parameter modification: the Neustrelitz
TEC broadcast model (NTCM-BC), the NTCM driven by GPS Klobuchar
parameters (NTCM-Klobpar), and the NTCM driven by Galileo broadcast
parameters (NTCM-GlAzpar). This study evaluates the performance of these
four NTCM variants both in the TEC domain (assessing the precision of
their TEC calculations) and in the positioning domain (assessing their
improvement in single-frequency, single-point positioning (SPP) during
the 25th solar cycle. Using Global Ionospheric Map (GIM) product from
the International GNSS Service (IGS) as a reference, the global
ionospheric TEC correction percentage is 48.24 % for NTCM-BC, 71.16 %
for NTCM-GlAzpar, 56.14 % for NTCM-Klobpar, and 62.93 % for NTCM-GL.
Furthermore, SPP results from 32 globally distributed GNSS stations show
percentage improvements in 3D positioning accuracy compared to the
uncorrected solution: On low solar activity days in 2020, improvements
reached 38.37 % (NTCM-BC), 46.15 % (NTCM-GlAzpar), 39.48 % (NTCM-
Klobpar), and 45.16 % (NTCM-GL). For high solar activity days in 2023,
the corresponding values were 42.42 %, 53.79 %, 36.98 %, and 52.33 %,
respectively. Among the evaluated models, NTCM-GL and NTCM-Klobpar
demonstrate the highest sensitivity to solar activity, with their root
mean square (RMS) errors closely correlating with variations in the 10.7
cm solar radio flux (F10.7) index. Conversely, NTCM-GlAzpar exhibits the
least sensitivity, maintaining stable performance across varying solar
flux conditions.</description>
</item>
<item>
<title> Ionospheric topside sounding revival</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.2574P</link>
<description>Although satellite sounding of the upper ionosphere yielded impressive
results and enabled numerous important discoveries across different
nations, its application halted in 1999 following the deployment of the
last topside sounder aboard the Russian space station Mir. During the
last decades monitoring of the upper ionosphere traditionally relied on
total electron content (TEC) measurements obtained from ground- and
space-based Global Navigation Satellite Systems (GNSS) receivers.
However, this methodology struggles to resolve the internal structure of
the ionosphere effectively, particularly in scenarios involving steep
horizontal gradients of plasma density. Alternative techniques, such as
GNSS occultation experiments, although widely adopted, suffer from
similar limitations when confronted with strong gradient conditions.
Meanwhile, ground-based tomographic imaging, dependent on empirical
models like IRI and NeQuick, fails to reconstruct sharply layered
ionospheric structures reliably. Addressing these gaps, the pioneering
launch of two LAERT topside sounders on November 5, 2024, aboard the
Ionosfera-M1 and Ionosfera-M2 satellites marked a turning point to
direct ionospheric sensing after a hiatus of 25 years. Deployed into a
sun-synchronous orbit at an altitude of 820 km, the new-generation LAERT
sounders introduced multifunctionality, combining traditional vertical
sounding with advanced techniques such as HF radio spectrometry and
relaxation sounding. Retaining the capability to deliver precise
vertical profiles of plasma density, these innovations allow for a more
nuanced exploration of plasma dynamics near the spacecraft,
magnetospheric interactions, and extraterrestrial phenomena like solar
radio bursts.</description>
</item>
<item>
<title> Band splitting in m-Type II radio bursts and their role in coronal parameter diagnostics</title>
<link>https://ui.adsabs.harvard.edu/abs/2026AdSpR..77.1349D</link>
<description>Type II radio bursts are signatures of shock waves generated by solar
eruptions, observed at radio wavelengths. While metric (m) type II
bursts originate in the lower corona, their longer-wavelength (up to
kilometers) counterparts extend into interplanetary space. A rare but
valuable feature observed in some type II bursts is band splitting in
their dynamic spectra, which provides crucial insights into physical
parameters such as shock speed, Alfvn Mach number, Alfvn speed, and
coronal magnetic field strength (B). In this study, we investigate band-
splitting in 44 m-type II radio bursts observed by the Radio Solar
Telescope Network during solar cycle 24 (20092019). These events
exhibit splitting in both fundamental and harmonic bands and are
analyzed under both perpendicular and parallel shocks. All events are
associated to solar flares and 41 (93 %) with the coronal mass
ejections. Shock speeds, derived using a hybrid coronal density model
proposed by Vrnak et al. (2004), range from
&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; 350 to 1727
km s&lt;SUP&gt;1&lt;/SUP&gt;. The relative bandwidth (BDW) of the split bands
remains constant with frequency and height. Alfvn Mach numbers indicate
moderate shock strength (1.063.38), while Alfvn speeds and B vary from
&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; 2301294 km
s&lt;SUP&gt;1&lt;/SUP&gt;and
&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; 0.487.13
G, respectively. Power-law relationships are established as &lt;mml:math&gt;&lt;m
ml:mrow&gt;&lt;mml:mi&gt;BDW&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:msubsup&gt;&lt;mml:mrow&gt;&lt;mm
l:mi&gt;f&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;L&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mr
ow&gt;&lt;mml:mo&gt;-&lt;/mml:mo&gt;&lt;mml:mn&gt;0.4&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msubsup&gt;&lt;/mml:
mrow&gt;&lt;/mml:math&gt; and &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;BDW&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/
mml:mo&gt;&lt;mml:msup&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;R&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:m
o&gt;&lt;/mml:mo&gt;&lt;mml:mn&gt;1&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msup&gt;&lt;/mml:mrow&gt;&lt;/mml:mat
h&gt;, while the coronal magnetic field decreases with height as &lt;mml:math&gt;
&lt;mml:mrow&gt;&lt;mml:mi&gt;B&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:msup&gt;&lt;mml:mrow&gt;&lt;mml:m
i&gt;R&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:mo&gt;-&lt;/mml:mo&gt;&lt;mm
l:mn&gt;3&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msup&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;. These
results enhance our understanding of shock dynamics and magnetic field
structures in the solar corona.</description>
</item>
<item>
<title> A Global TEC Spatiotemporal Prediction Model Based on Multisource Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SpWea..2304484L</link>
<description>The accurate prediction of Total Electron Content (TEC) is crucial for
ensuring the safety of space missions and enhancing the stability of
satellite navigation. Combining the advantages of Convolutional Neural
Networks (CNN) in local feature extraction with the Transformer self-
attention mechanism's ability to capture global dependencies, this paper
proposes a spatiotemporal prediction model based on an encoder-decoder
structureED-ST-Transformer, aimed at improving TEC prediction accuracy.
Given the close relationship between TEC, solar activity, and
geomagnetic disturbances, this study incorporates auxiliary inputs
including the disturbance storm time index (Dst), planetary K-index
(Kp), 10.7 cm solar radio flux (F10.7), and sunspot number. Using multi-
source data from the preceding 24 hr (with a temporal resolution of 2
hr), the model is constructed to forecast global TEC maps for the
subsequent 24 hr. To evaluate the performance of the ED-ST-Transformer
model, this study compares it with the C1PG, ED-ConvLSTM, and ED-
BiConvLSTM models in terms of overall prediction accuracy, error
distribution, visualization effects, and performance in different months
and latitude regions under various solar activity years. Additionally,
the prediction performance of the model during geomagnetic storms is
also analyzed. This outcome demonstrates that ED-ST-Transformer provides
the most stable and accurate predictions under all conditions,
outperforming the other models.</description>
</item>
<item>
<title> Type II and Type III Solar Radio Burst Classification Using Transfer Learning</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..179L</link>
<description>The Sun periodically emits intense bursts of radio emission known as
solar radio bursts (SRBs). These bursts can disrupt radio communications
and be indicative of large solar events that can disrupt technological
infrastructure on Earth and in space. The risks posed by these events
highlight the need for automated SRB classification, providing the
potential to improve event detection and real-time monitoring. This
would advance the techniques used to study space weather and related
phenomena. A dataset containing images of radio spectra was created
using data recorded by the Compound Astronomical Low frequency Low cost
Instrument for Spectroscopy and Transportable Observatory (e-Callisto)
network. This dataset comprises three categories: empty spectrograms;
spectrograms containing Type II SRBs; and spectrograms containing Type
III SRBs. These images were used to fine-tune several popular pre-
trained deep-learning models for classifying Type II and Type III SRBs.
The evaluated models included VGGnet-19, MobileNet, ResNet-152,
DenseNet-201, and YOLOv8. Testing the models on the test set produced F1
scores ranging from 87% to 92%. YOLOv8 emerged as the best-performing
model among them, demonstrating that using pre-trained models for event
classification can provide an automated solution for SRB classification.
This approach provides a practical solution to the limited number of
data samples available for Type II SRBs.</description>
</item>
<item>
<title> Three-Dimensional Characterization of Coronal Loops Using Combined Radio and EUV Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..175F</link>
<description>Coronal arcade loops play a key role in our understanding of solar
activity because they contain plasma within closed magnetic field lines.
Although these structures have been extensively studied using various
observational techniques, combining radio and extreme ultraviolet (EUV)
observations provides a unique opportunity to analyse their properties
more comprehensively. In this study, we present the first three-
dimensional characterisation of coronal loops by analysing simultaneous
observations of type J solar radio bursts and EUV imaging. Data were
collected from the Observations Radiospectrographiques pour FEDOME et
l'tude des ruptions Solaires, the Nanay Radioheliograph, and the
Solar Dynamics Observatory/Atmospheric Imaging Assembly instruments
during an event on 6 March 2014. Our results reveal a direct spatial
correlation between the sources of type J bursts and visible coronal
loops. Using a new methodology combining radio polarisation measurements
and EUV-based three-dimensional loop reconstruction, we determined
several key physical parameters: a temperature of approximately 0.82 MK,
an electron density distribution ranging from around 109 cm3 at the
foot of the loop to around 107 cm3 at the top, and a magnetic field
strength varying from around 850 Gauss at the footpoint to around 5
Gauss at the top. Our results confirm the validity of hydrostatic
equilibrium and dipole field models for coronal loops while providing
unprecedented insights into their three-dimensional structure and
physical properties. This research introduces a new diagnostic technique
for studying coronal loop dynamics and their role in solar eruptions.</description>
</item>
<item>
<title> Relevance to PSP and other solar wind observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PhPl...32l2903S</link>
<description>Based on the linearized Maxwell-fluid equations, this paper investigates
how an electronion plasma responds to a short-term current variation
with respect to the generation of electromagnetic waves. It is shown
that Langmuir waves can be triggered in the high-frequency range, the
direct conversion of which is directly associated with the generation of
type III radiation. In contrast to the classical approach of Ginzburg
and Zhelezniakov ["On the possible mechanisms of sporadic solar radio
emission (radiation in an isotropic plasma)," Sov. Astron. 2, 653
(1958)], after which beam-excited Langmuir waves in a two-step process
are converted into electromagnetic radiation, the presented mechanism
works without any parametric decay and wave coalescence. Rather,
electric field oscillations at the electron plasma frequency can be
triggered by different pulses of the driving current, e.g., by the
sudden (uncompensated) net current onset of the strahl at t = 0 in a
core-strahl plasma or by given temporal current variations, which may
occur as transient phenomena if the solar wind is disturbed by shocks,
magnetic switch-backs or other discontinuities. The application of
current pulses that imitate the beamplasma instability may generate
type III radiation with double-peak frequency spectra, often observed on
satellites. Moreover, suitable current profiles enable the simultaneous
excitation of type III emission and whistler waves. Measurements of
Langmuir waves, type III radiation, and whistler waves on board various
satellites in the solar wind, and in particular some of the recent
results of the Parker Solar Probe, are interpreted in the light of the
theoretical model. The fluid approach is confirmed by the results of
fully kinetic particle-in-cell simulations, presented in the Appendix.</description>
</item>
<item>
<title> A type II solar radio burst without a coronal mass ejection association</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JApA...46...90K</link>
<description>Type II solar radio bursts are commonly associated with shocks generated
by coronal mass ejections (CMEs), where plasma waves are excited by
magnetohydrodynamic (MHD) processes and converted into radio waves at
the local plasma frequency or its harmonics. However, there are
instances where type II bursts occur in the absence of whitelight CMEs.
We analysed one such metric type II radio burst observed on 2 November
2023, characterized by split band features and fundamental-harmonic
lanes. Notably, no CME was detected with space-based coronagraphs during
this event. However, an intense M1.6 class flare was observed just
before the type II burst and an extreme ultraviolet (EUV) disturbance
was observed expanding into surrounding regions. The absence of any
whitelight CME seen in any coronagraph field of view, even though the
EUV shock had a moderate speed of 500 km s-1, which was close to the
shock speed derived from radio observations. These observations indicate
that the shock in the inner corona was most likely driven by the EUV
ejecta seen in the lower corona, but the ejecta did not survive as a CME
in the coronagraph field of view.</description>
</item>
<item>
<title> Environmental and cosmic drivers</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JASTP.27706667A</link>
<description>This study employs Lomb periodogram analysis to investigate the spectral
characteristics of atmospheric gases (NH&lt;SUB&gt;3&lt;/SUB&gt;, O&lt;SUB&gt;3&lt;/SUB&gt;,
NOx, NO&lt;SUB&gt;1&lt;/SUB&gt;, NO&lt;SUB&gt;2&lt;/SUB&gt;, NMHC), solar radio flux (F10.7),
and cosmic rays (CR) in Riyadh from 1999 to 2007. Significant
periodicities ranging from 10 days to 1.6 years were identified, with
prominent cycles for gases at 454584 days, 291293 days, 215 days,
155171 days, 113 days, 97 days, 39 days, 1517 days, and 10 days; for
F10.7 at 467 days, 255 days, 172 days, and 17 days; and for CR at 489
days, 273 days, 140 days, and 32 days. The 215-day semi-annual and
39-day synoptic cycles, prevalent across multiple gases, alongside the
155171-day cycle strongly linked to F10.7 and CR, highlight robust
seasonal, synoptic, and heliospheric influences. Cross-spectral
analyses, along with zero-order and partial correlation analyses, were
conducted and confirmed that, while variations in atmospheric gases are
subject to terrestrial factors such as meteorological conditions
(temperature, humidity, wind), extraterrestrial factors, including solar
activity and CR, play a significant role in their variations, with
common periodicities validating these influences. Solar activity
enhances NOx and NMHC photochemistry, while CR ionization significantly
affects O&lt;SUB&gt;3&lt;/SUB&gt; and reduces NOx. These extraterrestrial impacts,
which warrant further investigation, are critically modulated by
meteorological factors. These findings are vital for addressing Riyadh's
environmental challenges, supporting sustainable urban development, and
enhancing understanding of extraterrestrial influences on climate,
atmospheric processes, and environmental sciences.</description>
</item>
<item>
<title> Comparative Assessment of Solar and Geophysical Parameters during the Initial Six Years of Solar Cycles 24 and 25</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Ge&amp;Ae..65..123A</link>
<description>This study presents a comparative statistical analysis of solar activity
during the first six years of Solar Cycles 24 (20082013) and 25
(20192024). The analysis focuses on key solar and geophysical
parameters, including sunspot numbers, halo coronal mass ejections
(CMEs), solar radio flux at 10.7 cm (F10.7), and geomagnetic storms, to
assess differences in solar behavior between the two cycles. Sunspot
numbers varied between 0 and 139.1 in Solar Cycle 24, whereas they
ranged from 0.2 to 216 during the corresponding period of Solar Cycle
25. Similarly, the F10.7 cm radio flux fluctuated between 65.7 and 153.5
in solar flux unit (s.f.u.) during 20082013, and between 67.05 and
245.6 s.f.u. from 2019 to 2024, reflecting an overall increase in solar
output. The study also includes an analysis of halo CMEs, with 192
events observed during Solar Cycle 24 and 227 during Solar Cycle 25,
both characterized by an angular width of 360. Geomagnetic activity was
assessed using 104 events from Cycle 24 and 179 from Cycle 25, with
disturbance storm time (Dst) index values ranging from 50 to 350 nT.
The results indicate a significant increase in solar activity during the
early phase of Solar Cycle 25 compared to Solar Cycle 24. This suggests
a more intense and dynamic space weather environment in the current
solar cycle, which may have important implications for space weather
forecasting and satellite operations.</description>
</item>
<item>
<title> The 27-Day Oscillation in Ionospheric Total Electron Content Observed by GNSS</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Atmos..16.1384H</link>
<description>The 27-day oscillation in total electron content (TEC) is analysed by
means of world maps of TEC. The TEC maps are derived from measurements
of the ground receiver network of the Global Navigation Satellite System
(GNSS) and are provided by the International GNSS Service (IGS). The
observed 27-day oscillation in TEC is mainly due to the 27-day solar
rotation period, which induces a 27-day oscillation in extreme
ultraviolet radiation (EUV) of the Sun. Analysing the time interval from
2003 to 2020, cross-correlation of the 27-day oscillation of the solar
MgII-index of the Solar Radiation and Climate Experiment (SORCE) and the
27-day oscillation in TEC shows an average time delay of about 1.1 days
for the ionospheric response with respect to the solar EUV variation.
The average correlation coefficient of the solar and the ionospheric
variation is 0.85. The cross-correlation of the 27-day oscillation in
solar radio flux F10.7 and the 27-day oscillation in TEC gives a time
lag of about 1.3 days and an average correlation coefficient of 0.78.
The world maps of the amplitude of the 27-day oscillation in TEC are
discussed for the TEC data from 1998 to 2024. Finally, TEC composites
are derived for F10.7 enhancement events and geomagnetic storms.</description>
</item>
<item>
<title> Reconnection-driven Decaying Pulsations Modulated by Slow Magnetoacoustic Waves</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..281...46L</link>
<description>Decaying pulsations have been simultaneously detected in the low-energy
X-rays of solar/stellar flares, which are supposed to be associated with
standing slow magnetoacoustic or kink-mode waves. The physical mechanism
behind rapid decay remains unknown. We present the detection of
quasiperiodic pulsations (QPPs) with rapid decay in high-energy
emissions produced in two major flares on 2024 January 10 and May 14.
Using empirical mode decomposition, decaying QPPs are identified in hard
X-ray and microwave emissions during the flare-impulsive phase,
suggesting a process of oscillatory magnetic reconnection. The quasi-
periods and decay times are determined by a damped harmonic function,
which are approximately 177  8 s (249  25 s) and 118  4 s (124  5
s), respectively. The restructured X-ray images reveal double footpoints
connected by hot flare loops. Their phase speeds are estimated to be
about 400 and 670 km s&lt;SUP&gt;1&lt;/SUP&gt;, both below the local sound speed in
high-temperature plasmas, indicating the presence of slow-mode waves in
hot flare loops. We perform coronal diagnostics based on standing slow-
mode waves and derive key physical parameters, including the polytropic
index, the thermal ratio, viscous ratio and radiation ratio, which are
consistent with previous results. Our observations support the
conclusion that decaying QPPs are triggered by oscillatory magnetic
reconnection that is modulated by standing slow magnetoacoustic waves,
with their rapid decay attributable to a coeffect of viscous damping and
localized magnetic reconnection rate.</description>
</item>
<item>
<title> "Ab-initio General-relativistic Neutrino-radiation Hydrodynamics Simulations of Long-lived Neutron Star Merger Remnants to Neutrino Cooling Timescales" (2023, ApJ, 959, 46)</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...995..229R</link>
<description>Not Available</description>
</item>
<item>
<title> Spatially Resolved Transport Parameters in Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...995..210O</link>
<description>The time profile of solar flare radio emission is often modeled as an
injection of energetic particles onto a closed magnetic loop, where they
may be trapped by the pinching of field lines and remain for a time
before decaying through loss of energy to the background or escaping to
the solar surface through the bottom of the loop. These injection,
trapping, and precipitation models for energetic particle transport have
often been used to explain the characteristics of spatially integrated
microwave emissions in solar flares. With the high-cadence imaging
spectroscopy capabilities of modern radio instruments, these ideas can
be probed with new depth. Radio imaging allows for the selection of
particular regions of flares to spatially and temporally isolate
individual injections and determine individual decay parameters that
could be confused in spatially integrated spectra. Simultaneous
spectroscopy allows the fitting of light curves versus frequency for
insight into the evolution of the particle energy spectrum and a deeper
physical understanding of the decay process. Using currently available
time resolution and data quality, injections and decays can be fit
simultaneously to the order of 1 s. These considerations motivate the
creation of the Pulsed-Injection-Precipitation Decomposition Fitter
(PIP_Decomp), which implements an automated method for fitting a series
of light curves with injection functions convolved with exponential
decays to produce spectrally resolved fit parameters. Herein, PIP_Decomp
is introduced and tested by applying it to model flares. Then,
PIP_Decomp is used to investigate two relatively simple flares observed
by the Expanded Owens Valley Solar Array.</description>
</item>
<item>
<title> Enigmatic Centi-SFU and mSFU Nonthermal Radio Transients Detected in the Middle Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...994..254M</link>
<description>Decades of solar coronal observations have provided substantial evidence
for accelerated particles in the corona. In most cases, the location of
particle acceleration can be roughly identified by combining high
spatial and temporal resolution data from multiple instruments across a
broad frequency range. In almost all cases, these nonthermal particles
are associated with quiescent active regions, flares, and coronal mass
ejections (CMEs). Only recently, some evidence of the existence of
nonthermal electrons at locations outside these well-accepted regions
has been found. Here, we report for the first time multiple cases of
transient nonthermal emissions, in the heliocentric range of
37R&lt;SUB&gt;&lt;/SUB&gt;, which do not have any obvious counterparts in other
wave bands, like white-light and extreme ultraviolet. These detections
were made possible by the regular availability of high dynamic-range
low-frequency radio images from the Owens Valley Radio Observatory's
Long Wavelength Array. While earlier detections of nonthermal emissions
at these high heliocentric distances often had comparable extensions in
the plane of sky, they were primarily associated with radio CMEs, unlike
the cases reported here. Thus, these results add on to the evidence that
the middle corona is extremely dynamic and contains a population of
nonthermal electrons, which is only becoming visible with high dynamic-
range low-frequency radio images.</description>
</item>
<item>
<title> Solar Eruption Onset and Particle Acceleration in Nested-null Topologies</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...994..180K</link>
<description>The magnetic breakout model explains a variety of solar eruptions,
ranging from small-scale jets to large-scale coronal mass ejections
(CMEs). Most of our previous studies are focused on jets and CMEs in
single null-point topologies. Here, we investigate the initiation of
CMEs and associated particle acceleration in a double null-point (or
nested fan-spine) topology during multiple homologous M- and X-class
flares from an active region. The initiation of the flare and associated
eruption begins with inflow structures moving toward the inner null of
the closed fan-spine topology. Simultaneous slow flare reconnection
below a small filament formed a hot flux rope along with expansion of
the overlying flux during slow breakout reconnection at the inner null.
The first explosive breakout reconnection of the flux rope at the inner
null produced a circular and a remote ribbon along with successful
eruption of the flux rope and associated fast EUV (shock) wave.
Simultaneous flare reconnection beneath the erupting flux rope produced
a typical two-ribbon flare along with two hard X-ray footpoint sources.
When the flux rope (with shock) reaches the outer null, a second
explosive breakout reconnection produces another large-scale remote
ribbon. The radio observations reveal quasiperiodic Type III bursts
(period = 100 s) and a Type II burst during the breakout reconnection
near the inner and outer nulls, along with gradual solar energetic
particles observed at 1 au for magnetically connected events. This study
highlight the importance of two successive breakout reconnections in the
initiation of CMEs in nested-null topologies and associated particle
acceleration and release into the interplanetary medium. The particles
are accelerated by the shock ahead of the flux rope, which formed during
the inner breakout reconnection. These findings have significant
implications for particle acceleration and escape processes in
multiscale null-point topologies that produce jets and CMEs.</description>
</item>
<item>
<title> Effects in the upper atmosphere and ionosphere in the subauroral region during Victory Day 2024 Geomagnetic Storm (May 1012, 2024)</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.7325C</link>
<description>This study provides a detailed analysis of the impact of the magnetic
storm (referred to as the Victory Day Storm, as the solar flares
occurred on May 89, 2024), which took place from May 10 to 12, 2024,
and has become the most significant geomagnetic event of the 21st
century to date, on the subauroral and mid-latitude ionosphere using a
variety of instruments and observation methods. The research is based on
data from satellite systems (Swarm, DMSP, TIMED), ground-based
magnetometers, ionosondes, VLF (very low frequency) signals, GNSS
(global navigation satellite system) receivers, and all-sky cameras. The
solar flares and powerful coronal mass ejection (CME) from the Sun
caused intense geomagnetic disturbances, leading to significant changes
in the density, structure, and dynamics of the ionospheric plasma at
subauroral and mid-latitudes. In particular, auroras were observed at
these latitudes, which is a rare phenomenon for these regions. Satellite
observations, SUSSI data (allowing for measurements of auroral emissions
in the ionosphere) from the DMSP satellite, and all-sky cameras provided
detailed information on the spatial development of storm phenomena in
the ionosphere. The cooling flux of nitrogen oxide during geomagnetic
activity was studied using TIMED/SABER data, as well as latitudinal
profiles of the integral O/N2 ratio from TIMED/GUVI data. Measurements
from magnetometers and ionosondes revealed significant changes in the
magnetic field and ionospheric plasma density, while VLF (very low
frequency) stations and GNSS receivers recorded substantial disruptions
in radio communication and navigation during the Victory Day Geomagnetic
Storm. The study emphasizes the need for integrating various data to
deeply understand and predict the impact of extreme magnetic storms on
the ionosphere, upper atmosphere, and related technological systems.</description>
</item>
<item>
<title> A case study of Mother's Day solar storm (1015 May 2024)</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.7308B</link>
<description>The strongest geomagnetic storm of solar cycle 25 (SYM-H &lt; 518 nT),
referred to as the "Mother's Day Storm", occurred between 10 and 15 May
2024. Its source traces back to a solar event on 8 May 2024, when the
solar Active Region 13,664 produced multiple solar flares and launched
several Earth-directed coronal mass ejections (CMEs). Classified as a G5
geomagnetic storm, it was the most intense one of the space age since
March 1989 storm (SYM-H &lt; 720 nT). The storm's impact on Earth's
ionosphere-magnetosphere system, particularly the significant variations
in electron density, degraded radio wave propagation, disrupted Global
Navigation Satellite System (GNSS) operations and communication
services. These disruptions pose challenges to the integrity and
accuracy of GNSS-based high-precision positioning methods, such as
Precise Point Positioning (PPP). This study evaluates the performance of
multi-GNSS dual-frequency PPP (DF-PPP) during both the quiet pre-storm
period (89 May 2024) and the Mother's Day storm (1011 May 2024). Using
a robust dataset from over 1,800 globally distributed GNSS stations, the
analysis investigates the correlation between PPP errors and the rate of
Total Electron Content (TEC) index (ROTI), a widely used metric for
characterizing ionospheric plasma irregularities. The results reveal
three critical findings: first, positioning errors showed strong
latitudinal dependence, with high-latitude stations suffering the most
severe degradation  median errors rising from 2.4 cm (quiet-time) to
9.0 cm (275 % increase) due to intense ionospheric irregularities within
the auroral oval. Mid-latitude stations experienced moderate degradation
(25 % median error increase) associated with expanded Equatorial Plasma
Bubbles (EPBs), while low-latitude regions showed more stable but
inherently higher positioning errors. Second, the elevation-weighted
ROTI (&lt;mml:math&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;R&lt;/mml:mi&gt;&lt;mml:mi&gt;O&lt;/mml:mi&gt;
&lt;mml:mi&gt;T&lt;/mml:mi&gt;&lt;mml:mi&gt;I&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;e&lt;/mml:
mi&gt;&lt;mml:mi&gt;l&lt;/mml:mi&gt;&lt;mml:mi&gt;e&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:math&gt;
) exhibited strong correlations with PPP errors
(&lt;mml:math&gt;&lt;mml:mi&gt;r&lt;/mml:mi&gt;&lt;/mml:math&gt; = 0.78 at high latitudes),
validating its utility for global storm-impact assessments. Third,
multi-GNSS combinations (GPS + GLONASS + Galileo) reduced errors by
4152 % compared to GPS-only solutions, with Galileo's signals showing
particular robustness. Collectively, these findings establish multi-GNSS
PPP as a critical tool for space weather monitoring, thereby advancing
global understanding of ionospheric impacts during extreme geomagnetic
events.</description>
</item>
<item>
<title> Comparative assessment of GNSS ionospheric broadcast models during the May 10, 2024 geomagnetic storm event</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.7272C</link>
<description>The Single-Frequency GNSS ionospheric corrections models play a vital
role in improving the positional accuracy of GNSS users, satellite orbit
determination, Radio Occultation for atmospheric profiling, and remote
sensing satellite data analysis. Ionospheric correction models such as
GNSS Klobuchar, NeQuick G, BDGIM, and USRG can be investigated to
understand space weather effects like geomagnetic storms and solar
flares in low-latitude regions. In this paper, the performance of four
ionospheric Total Electron Content models, BDGIM, USRG, NeQuick G, and
Klobuchar, are evaluated for geomagnetic storm events that occurred on
10 May 2024 over the Indian region, a low-latitude area profoundly
influenced by the Equatorial Ionization Anomaly (EIA). The results
indicate that the BDIGM model outperformed the RMSE of 7.7TECU over the
NeQuick G (11.16TECU) and Klobuchar (25.38TECU) models on main and
geomagnetic storm days. The season variability of the BDGIM model is
also well predicted as compared to other single-frequency ionospheric
models. The BDGIM TEC models are closer to dual frequency GNSS TEC
estimations than Klobuchar and NeQuick G at eight GNSS stations in the
Indian region. Further, the positional accuracy analysis of single-
frequency ionospheric correction models with the GLAB GNSS data
processing tool for Bengaluru GNSS station TEC data. The BDGIM model
static positioning errors are minimal compared to Klobuchar and NeQuick
G over low-latitude GNSS stations under geomagnetic storm conditions.
The outcome of this research work would be beneficial for identifying
suitable single-frequency GNSS ionospheric corrections models over the
low and equatorial latitude conditions for aviation, maritime, and
remote sensing data applications.</description>
</item>
<item>
<title> a challenge to the coronal mass ejection origin of long-duration gamma-ray flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...704A.140B</link>
<description>We present a multi-spacecraft analysis of the 2024 July 16 long-duration
gamma-ray flare (LDGRF) detected by the Large Area Telescope on the
Fermi satellite. The measured &gt; 100 MeV -ray emission persisted for
over seven hours after the flare impulsive phase, and was characterized
by photon energies exceeding 1 GeV and a remarkably hard parent-proton
spectrum. In contrast, the phenomena related to the coronal mass
ejection (CME)-driven shock linked to this eruption were modest,
suggesting an inefficient proton acceleration unlikely to achieve
energies well above the 300 MeV pion-production threshold to account for
the observed -ray emission. Specifically, the CME was relatively slow
(600 km/s) and the accompanying interplanetary type-II/III radio bursts
were faint and short-lived, unlike those typically detected during large
events. In particular, the type-II emission did not extend to kilohertz
frequencies and disappeared 5.5 hours prior to the LDGRF end time.
Furthermore, the associated solar energetic particle (SEP) event was
very weak, short-duration, and limited to a few tens of MeV, even at
magnetically well-connected spacecraft. These findings demonstrate that
a very fast CME resulting in a high-energy SEP event is not a necessary
condition for the occurrence of LDGRFs, challenging the idea that the
high-energy -ray emission is produced by the back-precipitation of
shock-accelerated ions into the solar surface. The alternative origin
scenario based on local particle trapping and acceleration in large-
scale coronal loops is instead favored by the observation of giant arch-
like structures of hot plasma over the source region that persisted for
the entire duration of this LDGRF.</description>
</item>
<item>
<title> Insights from radio and in situ observations, and EUHFORIA modeling</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...704A..95D</link>
<description>Context. The distribution of the coronal electron density at different
distances from the Sun strongly influences the physical processes in the
solar corona, and it is therefore a very important topic in solar
physics. The majority of the methods used to estimate coronal electron
density, including radio observations, were up to now not fully
validated due to the absence of in situ observations closer to the Sun.
Consequently, space weather forecasting models that simulate coronal
density lacked proper validation. Newly available Parker Solar Probe
(PSP) in situ observations at distances close to the Sun provide an
opportunity to study the properties of plasma near the Sun and to
compare observational and modeling results. Aims. The focus of this work
is to study type III radio bursts, estimate their propagation path, and
validate the coronal electron density obtained from in situ radio
observations and modeling with the EUropean Heliospheric FORecasting
Information Asset (EUHFORIA). Methods. In this study of type III radio
bursts observed during the second PSP perihelion, we employ radio
triangulation and modeling to analyze coronal electron density. Using
the radio triangulation method, we determined the 3D positions of the
radio sources. Additionally, we utilized the state-of-the-art EUHFORIA
model to estimate electron densities at various locations. The electron
densities derived from radio observations and EUHFORIA modeling were
then inter-validated with in situ measurements from PSP. Results. We
studied 11 type III radio bursts during the second PSP perihelion, with
radio triangulation showing their propagation path in the southward
direction from the solar ecliptic plane. The obtained radio source sizes
ranged from 0.5 to 40 deg (0.525 R&lt;SUB&gt;&lt;/SUB&gt;), showing no clear
frequency dependence. This indicates that scattering of radio waves was
not very significant for the studied events and in this frequency range.
A comparison of electron densities derived from radio triangulation, in
situ PSP data, and EUHFORIA modeling showed a large range of obtained
values. This result is influenced by the different propagation paths
across different coronal structures and model limitations. Despite these
variations, EUHFORIA successfully identified high-density regions along
type III burst paths, demonstrating its capability to capture large-
scale density structures. Conclusions. Our study emphasizes that type
III bursts do not always follow the Parker spiral but instead trace
distinct magnetic field lines that can be very differently oriented. The
study shows constant radio source sizes and confirms that small-scale
density fluctuations in PSP data remain relatively low. These two
characteristics indicate that scattering effects do not significantly
change observed radio source positions within the studied distances.</description>
</item>
<item>
<title> Solar Radio Wide-Band Spectroscopy and Imaging Facilities of the Chinese Meridian Project Phase II</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SpWea..2304595Y</link>
<description>Solar eruptions, including flares and coronal mass ejections, are the
most energetic phenomena in the solar system. These explosive events
accelerate high-energy particles and generate electromagnetic radiation
from radio to gamma-ray wavelengths, producing heliospheric disturbances
and acting as primary drivers of space weather hazards. Wide-band solar
radio observations, spanning decameter to centimeter wavelengths,
constitute a key component of the Chinese Meridian Project (CMP) for
tracking and monitoring solar eruptions from the Sun's atmosphere into
interplanetary space. The technique of solar radio imaging spectroscopy
is still challenging and new. The Mingantu Spectral Radioheliograph
(MUSER) with three arrays at low (30400 MHz), intermediate (400 MHz2
GHz), and high (215 GHz) frequency bands images the solar atmosphere in
3D from the top-chromosphere up into the mid-corona. The solar radio
spectrometers include a Metric Wavelength Solar Radio Spectrometer
(90600 MHz) at Chashan in Shandong province, together with the three
Decameter-Metric to Centimetric Wavelength Solar Radio Spectrometers at
the MUSER site, offering spectrum monitoring ability across a super wide
band from 30 MHz up to 15 GHz. The overall design, some technical
details, calibration method, and performance with some preliminary data
of these facilities are described.</description>
</item>
<item>
<title> Detection of Various Solar Radio Bursts Based on Stable Diffusion and Self-Supervised Pretraining</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..171Z</link>
<description>Accurate identification of solar radio bursts (SRBs) is of great
significance for solar physics research and space-weather forecasting.
Most existing studies focus on the mere detection of SRB occurrence or
the identification of a single class (e.g., Type III bursts), which
fails to meet the demand for precise detections of various solar radio
bursts. Additionally, current mainstream SRBs detection models often
employ complex architectures and redundant parameters, resulting in low
computational efficiency. To address these limitations, we constructed a
spectrogram dataset based on the e-CALLISTO platform, comprising Type
II, Type III, Type IV, and Type V bursts. The dataset contains 8752
images with 10,822 annotated instances, where samples of types IV and V
are incredibly scarce. To overcome the challenge of pretraining with
few-shot classes, this paper proposes a pretraining method that
integrates a stable diffusion generative model with a self-supervised
learning strategy, effectively enhancing the model's learning capability
for few-shot classes. Building on this, this paper presents a detection
model for various solar radio bursts, VitDet-SRBs (Vision Transformer
Detector for Solar Radio Bursts), which incorporates a channel attention
mechanism into the feature fusion module to enhance performance while
controlling model complexity. Experimental results show that VitDet-SRBs
achieve an average precision at a single Intersection-over-Union
threshold of 0.50 (AP@50, AP with IoU = 0.50) of 81.2% on the SRBs
dataset, outperforming existing mainstream methods in both precision and
recall. This study not only provides a novel approach for efficient
detections of various solar radio bursts but also offers a feasible
solution for other few-shot astronomical data processing problems, with
broad application prospects.</description>
</item>
<item>
<title> Relative Strengths of Fundamental and Harmonic Emissions of Solar Radio Type II Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..168J</link>
<description>Solar radio type II bursts are slow-drifting bursts that exhibit various
distinct features such as Fundamental (F) and Harmonic (H) emissions,
band-splitting, and discrete fine structures in the dynamic spectra.
Observationally, it has been found that in some cases the F emission is
stronger than the H emission, and vice versa. The reason for such
behavior has not been thoroughly investigated. To investigate this, we
studied 58 meter wave (20  500 MHz) type II solar radio bursts showing
both F and H emissions, observed during the period from 13 June 2010 to
25 December 2024, using data obtained with the Compound Astronomical Low
frequency Low cost Instrument for Spectroscopy and Transportable
Observatory (CALLISTO) spectrometers at different locations and
Gauribidanur LOw-frequency Solar Spectrograph (GLOSS). We examined the
intensity ratios of the H (IH) and F (IF) emissions and analyzed their
variation with heliographic longitude. We found that 14 out of 19 bursts
originating from heliographic longitudes beyond 75 exhibited an IH/IF
ratio greater than unity. In contrast, 32 out of 39 bursts originating
from longitudes within 75 showed a intensity ratio less than unity.
From these results, we conclude that the relative strength of the F and
H emissions can be influenced by refraction due to density gradient in
the solar corona, directivity and viewing angle of the bursts.</description>
</item>
<item>
<title> Sources of a Stationary Type II Radio Burst on the Associated Coronal Mass Ejection Driven-Shocks</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..164F</link>
<description>Solar type II radio bursts are associated with shock waves driven by
coronal mass ejection (CME). Their shapes in the solar radio dynamic
spectrum depend on the shock velocity and the electron density traversed
by their radio sources. This study examines a stationary type II radio
burst. By analyzing observations from the Daocheng Solar Radio Telescope
and the Solar Dynamics Observatory/Atmospheric Imaging Assembly, we aim
to determine the spatial relationship between type II burst sources and
shock fronts. Observations suggest that the radio sources are located in
the interaction region between the CME shocks and the coronal streamer.
Extensive analysis of their fine structures, particularly the type II
herringbones, shows that the radio sources are generally distributed in
a frequency order from downstream to upstream regions of the shocks, or
only in the upstream region. The observations confirm the existence of
type II bursts and associated energetic electrons in the regions
upstream and downstream of a shock wave.</description>
</item>
<item>
<title> The Bimodal Solar Corona Revisited</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..160W</link>
<description>During Solar Cycle 24, several groups independently noticed that a sharp
transition in coronal activity occurred early in 2011. The transition
took the form of a sudden jump in the intensity of ("hot") EUV lines
formed at temperatures above about log(T) = 6.1, whereas ("cool") lines
formed below log(T) = 6.0 showed little change. This led to the
suggestion of bimodal behavior in the corona, and has been linked to the
timing of the "terminator" of the previous solar cycle. An obvious
question is whether this behavior is typical of solar cycle onsets in
the corona. In this brief article we investigate whether the corona
showed similar behavior at the onset of Solar Cycle 25, using data from
the EUV Variability Experiment (EVE) on the Solar Dynamics Observatory
(SDO) satellite. Previous observations have shown that hot coronal lines
vary by orders of magnitude over the solar cycle while cool lines show
very little variation. EVE has measurements of a number of strong
coronal lines, and here we compare the onsets to Cycles 24 and 25 in the
hot Si XII 499  line and the cool Ne VIII 770  line. We find that, in
contrast to Cycle 24, the onset of emission in the higher temperature
lines during Cycle 25 is relatively gradual, with no clear indication of
bimodal behavior, suggesting that sharp onsets of coronal activity are
not a recurrent feature of the solar cycle.</description>
</item>
<item>
<title> Entropy transfer from solar radio bursts to energetic particles</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SciA...11z7419L</link>
<description>Space plasma thermodynamics is thought to be affected by wave activity.
Here, we show that solar radio bursts (SRBs) can transfer entropy to
solar energetic protons (SEPs), affecting their thermodynamics. In
particular, our analysis (i) detects the statistically significant SEP
density fluctuations, associated with SRB activity that triggers a
systematic increase in the thermodynamic kappa; (ii) estimates the
polytropic index of SEPs, which is anticorrelated with kappa, serving as
an independent measure to validate the increase in kappa; (iii) derives
the entropy transfer by using its theoretical relationship with kappa;
and (iv) compares SRB wave intensity with the entropy transferring to
SEPs to demonstrate their wave-particle coupling. We lastly expose the
thermodynamic association between type III SRB wave intensity and SEP
entropy transfer as well as their respective coupling, thus developing a
paradigm for further systematic investigations among other types of wave
activity and particle populations.</description>
</item>
<item>
<title> Radio Stars in the Era of New Observatories</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PASP..137k6001M</link>
<description>An international conference Radio Stars in the Era of New Observatories
was held at the Massachusetts Institute of Technology Haystack
Observatory on 2024 April 1719. The conference brought together more
than 60 researchers from around the world, united by an interest in
using radio wavelength observations to explore the physical processes
that operate in stars (including the Sun), how stars evolve and interact
with their environments, and the role of radio stars as probes of our
Galaxy. Topics discussed at the meeting included radio emission from
cool and ultracool dwarfs, extrasolar space weather, stellar masers,
thermal radio emission from evolved stars, circumstellar chemistry, low
frequency observations of the Sun, radio emission from hot stars,
applications of very long baseline interferometry techniques to stellar
astrophysics, stellar explosive events, the detection of radio stars in
the latest generation of widefield sky surveys, the importance of radio
stars for understanding the structure and evolution of the Milky Way,
and the anticipated applications for stellar astrophysics of future
radio observatories on the ground and in space. This article summarizes
research topics and results featured at the conference, along with some
background and contextual information. It also highlights key
outstanding questions in stellar astrophysics where new insights are
anticipated from the next generation of observational facilities
operating at meter through submillimeter wavelengths.</description>
</item>
<item>
<title> Improvement Method for Solar Radio Burst Long-tailed Detection Using Probabilistic Diffusion Generative Models</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PASP..137k4504W</link>
<description>Solar radio burst (SRB) detection plays a crucial role in solar physics
research and space weather warning. However, multi-class SRB detection
suffers from a long-tailed distribution, where the number of samples in
most classes (long-tailed classes) is extremely small, while a few
classes (head classes) dominate the dataset. To address this issue, we
propose a diffusion model for SRBs detection (DiffuSRBsD) model, a
generative augmentation method employing diffusion model for long-tailed
class enhancement. DiffuSRBsD introduces a mask-conditioned generation
strategy to control SRB morphology in spectrograms and employs textual
inversion to embed multiple SRB features into a unified semantic
representation. Furthermore, we develop a memory structural similarity
index measure, a generative image filter specifically for SRBs.
Extensive experiments on a benchmark Dataset of SRBs demonstrate that
DiffuSRBsD significantly improves the performance of representative
detection models, achieving gains of 9.9%, 41.4%, 31.7%, and 11.8% in
mAP@50 for the most long-tailed Type IV SRBs. These results validate the
effectiveness of our approach and offer a novel perspective for
enhancing SRB detection, providing robust data processing support for
space weather prediction. The dataset and code are publicly available at
https://github.com/onewangqianqian/DiffuSRBsD.git.</description>
</item>
<item>
<title> Space Weather Impact of Three Solar Flares Observed by the POEMAS Telescope at 45 and 90 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13034611V</link>
<description>Solar flares are often associated with coronal mass ejections (CMEs)
that, when directed toward Earth, can disrupt the magnetosphere and
impact space weather. In this study, we investigate three long-duration
solar flares observed in 2012 by the POlarization Emission of Millimeter
Activity at the Sun (POEMAS) telescopes at 45 and 90 GHz. We analyze the
correlation between their radio spectral properties, associated CMEs,
and geomagnetic and ionospheric responses, to assess the possibility of
space weather prediction. Spectral fitting of the radio data using a
gyrosynchrotron model reveals accelerated electron populations with a
hard energy distribution (spectral index $(\delta =2.8\pm 0.5)$) that
hardens with time, and magnetic fields of $B=160\pm 50$ G. The most
energetic flare involved a source region 36 times larger than the
others and produced 10 times more energetic electrons. In all three
events, CMEs were launched simultaneously with the flares. The July 12
X1.4 flare was associated with a fast (884 km/s) halo CME that led to a
moderate geomagnetic storm (Dst = 139 nT, Kp = 6). VLF radio data show
that all three flares increased ionospheric electron density, lowering
its boundary from 70 km to 5867 km. These results suggest that long-
duration flares with high flux at 45 GHz and hard radio spectra are
associated with more energetic events characterized by higher GOES
class, greater SXR energy, faster and more energetic CMEs, and stronger
geomagnetic disturbances, highlighting the potential of high-frequency
radio observations as a tool for space weather prediction.</description>
</item>
<item>
<title> Quantification of Perturbation to the Daytime Lower Ionosphere From a Gamma Ray Burst Using ELF Remote Sensing</title>
<link>https://ui.adsabs.harvard.edu/abs/2025GeoRL..5217989G</link>
<description>On 9 October 2022, a powerful gamma ray burst (GRB), GRB221009A, caused
significant changes in the electron density of the lower ionosphere, as
evidenced by VLF (330 kHz) radio wave observations. However, GRB221009A
did not yield any observable signatures at the Schumann resonances (8,
14 Hz), which are also sensitive to the lower ionosphere. We show that
the effects of GRB221009A are observable in a decrease in propagation
velocity of ELF (31,000 Hz) lightning impulses. Analytical and
numerical analysis points to an ionospheric perturbation in which the
GRB increased the daytime electron density uniformly over a wide
altitude range from 50 to 90 km. The GRB perturbation is markedly
different from perturbations from solar flares, which significantly
increase the vertical gradient of the electron density. ELF propagation
velocity is shown to be a technique that can identify the altitude range
of ionospheric perturbations.</description>
</item>
<item>
<title> Signatures of Confined and Eruptive Solar Flares in Microwave Spectra</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...994..103C</link>
<description>We describe how microwave spectra of confined flares differ from those
of eruptive flares. All 29 confined M1.4 soft X-ray flares from NOAA
Active Region 12192 in 2014 October that were observed by the Radio
Solar Telescope Network in the &gt;300 MHz microwave range (encompassing
RSTN frequencies from 410 to 15,400 MHz) had low-frequency (410 MHz)
cutoffs in their peak-flux-density spectra, with peak emission &lt;10 solar
flux units (sfu) at 410 MHz. Wind/Waves observations at 1 MHz for 20 of
these cutoff microwave bursts suggest that few, if any, of the 29 flares
were accompanied by escaping electrons. We find a marked difference
between microwave spectra for samples of intense (M5) confined and
eruptive flares from 2011 to 2016: 20 of 21 confined M5 flares had
cutoff spectra, while 27 of 30 M5 eruptive flares had peak 410 MHz
emission &gt;10 sfu (with a median value of 431 sfu). For the subsets of
these events with Wind/Waves observations, only one of 20 confined
events was unambiguously accompanied by 1 MHz emission, while 25 of the
29 eruptive flares had peak 1 MHz fluxes &gt;10&lt;SUP&gt;3&lt;/SUP&gt; sfu (above a
background of 200400 sfu), with an overall median peak value of
10&lt;SUP&gt;5&lt;/SUP&gt; sfu. These results indicate that strong confined flares
characteristically do not involve or affect open field lines, ruling out
interchange reconnection as a confined-flare generation mechanism,
leaving reconnection between closed loops as the likely alternative. The
microwave spectral signatures of confined and eruptive flares have
potential application for the determination of confinement/eruption for
flares on solar-type stars.</description>
</item>
<item>
<title> Extreme-ultraviolet Wave and Quasiperiodic Pulsations during an Eruptive M-class Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...993...99L</link>
<description>In this paper, we report multiwavelength and multipoint observations of
the prominence eruption originating from active region 11163, which
generated an M3.5 class flare and a coronal mass ejection (CME) on 2011
February 24. The prominence lifts off and propagates nonradially in the
southeast direction. Using the revised cone model, we carry out three-
dimensional reconstructions of the ice-cream-like prominence. It is
found that the latitudinal inclination angle decreases from 60 to
37, indicating that the prominence tends to propagate more radially.
The longitudinal inclination angle almost keeps constant (6). The
highly inclined prominence eruption and the related CME drive an
extreme-ultraviolet (EUV) wave, which propagates southward at speeds of
381.60 and 398.59 km s&lt;SUP&gt;1&lt;/SUP&gt; observed in 193 and 304 ,
respectively. The M3.5 class flare presents quasiperiodic pulsations
(QPPs) in soft X-ray, hard X-ray, EUV, and radio wavelengths with
periods of 80120 s. Contemporary with the flare QPPs, a thin current
sheet and multiple plasmoids are observed following the eruptive
prominence. Combining with the appearance of drifting pulsation
structure, the QPPs are most probably generated by quasiperiodic
magnetic reconnection and particle accelerations as a result of
plasmoids in the current sheet.</description>
</item>
<item>
<title> SIMPL</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...704A..75D</link>
<description>Context. The LOw Frequency ARray (LOFAR) is capable of imaging
spectroscopy of the Sun in the 10240 MHz frequency range, with high
spectral, temporal, and spatial resolution. However, the complex and
rapidly varying nature of solar radio emission  spanning several orders
of magnitude in brightness and further exacerbated by the strong
ionospheric phase distortions during daytime observations, poses major
challenges for calibration, imaging, and automation. Aims. We aim to
develop a fully automated, high-fidelity imaging pipeline optimised for
LOFAR solar observations, capable of handling the intrinsic variability
of solar emission and producing science-ready images with minimal human
intervention. Methods. We have built the Solar Imaging Pipeline for
LOFAR (SIMPL), which integrates excision of radio-frequency interference
(RFI) for the solar-specific scenarios, calibration strategies, and
self-calibration. At present, SIMPL processes data from the LOFAR core
stations and produces total-intensity solar images, with ongoing
developments aimed at enabling full polarimetric imaging and
incorporating increasingly distant antennas. The pipeline is designed to
enable scalable and uniform processing of large archival datasets.
Results. In terms of performance, SIMPL achieves more than an order of
magnitude improvement in imaging dynamic range compared with previous
efforts and reliably produces high-quality spectroscopic snapshot
images. It has been tested across a wide range of solar conditions. It
is currently being employed to process a decade of LOFAR solar
observations, providing science-ready Flexible Image Transport System
(FITS) images for the community and enabling both comprehensive and
novel studies of solar radio phenomena, ranging from quiet Sun emission
and faint non-thermal features to active regions and their associated
dynamic events, such as transient bursts.</description>
</item>
<item>
<title> Source location and evolution of a multilane type II radio burst</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...703A.271Z</link>
<description>Context. Shocks in the solar corona are capable of accelerating
electrons that in turn generate radio emission known as type II radio
bursts. The characteristics and morphology of these radio bursts in the
dynamic spectrum reflect the evolution of the shock itself, together
with the properties of the local corona where the shock propagates.
Aims. In this work we study the evolution of a complex type II radio
burst with a multilane structure to find the locations where the radio
emission is produced and relate them to the properties of the local
environment where the shock propagates. Methods. Using radio imaging, we
were able to separately track each lane composing the type II burst and
relate the position of the emission to the properties of the ambient
medium, such as density, Alfvn speed, and magnetic field. Results. We
show that the radio burst morphology in the dynamic spectrum changes
with time and is related to the complexity of the local environment. The
initial stage of the radio emission is characterized by a single broad
lane in the spectrum, while the later stages of the radio signature
evolve in a multilane scenario. The radio imaging reveals how the
initial stage of the radio emission separates with time into different
locations along the shock front as the density and orientation of the
magnetic field change along the shock propagation. At the time when the
spectrum shows a multilane shape, we find a clear separation of the
imaged radio sources propagating in regions with different densities.
Conclusions. By combining radio imaging with the properties of the local
corona, we describe the evolution of a type II radio burst and, for the
first time, identify three distinct radio emission regions above the
coronal mass ejection front. Two regions were located at the flanks,
producing earlier radio emission than the central position, in
accordance with the complexity of density and Alfvn speed values in the
regions where radio emission is generated. This unprecedented
observation of a triple-source structure provides new insights into the
nature of multilane type II bursts.</description>
</item>
<item>
<title> Effects of anisotropy of beam temperature on Langmuir and transverse wave spectra generated by beamplasma instability</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PhPl...32j2108T</link>
<description>Understanding the dynamics of beamplasma interaction is key to
understanding solar radio bursts of types II and III. Most of the
numerical work done on the topic assumes a beam that is isotropic in
temperature. As we are not aware of any fundamental reason for that
assumption, in this work, we analyze the effect that beam temperature
anisotropy has on the dynamics of the beam-plasma system, assuming a
two-dimensional geometry. The numerical results obtained show that the
increase in the beam parallel temperature leads to a decrease in the
Langmuir wave emission, and are corroborated by an analytical
description of the relationship between beam parallel temperature and
Langmuir wave intensity. We also investigate the effect of temperature
anisotropy on electromagnetic waves generated by the nonlinear dynamics,
and obtain that the change of the beam parallel temperature affects the
intensity for both the fundamental and harmonic emissions, with a more
pronounced effect for harmonic emission.</description>
</item>
<item>
<title> Multi-scale modelling of energetic particle dynamics and radio signatures in coronal and heliospheric plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PhDT........13H</link>
<description>Solar Energetic Particles (SEPs) accelerated during space weather events
such as solar flares, Coronal Mass Ejections (CMEs), and corotating
interaction regions, can reach energies up to several GeV per nucleon
for ions and several tens MeV for electrons, thereby posing significant
risks to satellites, astronauts, and ground-based systems. Understanding
SEP acceleration and transport, along with their associated radio
signatures, is crucial for enhancing space weather forecasts and
mitigation strategies. This thesis presents, in three stages, a novel,
physics-based framework to simulate the acceleration, transport, and
radio emission of SEPs in realistic solar wind and coronal environments.
Building on an earlier implementation in which the MagnetoHydroDynamic
(MHD) model EUHFORIA has been coupled with the focused transport code
PARADISE, we first replace EUHFORIA with the more advanced inner
heliospheric solar wind MHD code Icarus, which supports localised grid
refinements and higher shock resolutions via adaptive mesh refinement.
Next, to study SEP and CME dynamics below 0.1 au, the framework is
extended into the corona using the COCONUT MHD model. Finally, we
integrate the Ultimate Fast Gyrosynchrotron Codes to compute radio
emission from energetic electrons trapped in a CME flux rope.
Applications for each stage demonstrate significant advances in
modelling particle dynamics in both the corona and heliosphere. The
framework enables realistic simulations of particle acceleration at
finely resolved shocks, investigation of particle confinement and escape
in low-coronal magnetic flux ropes, and direct linkage of these
processes to observable type IV radio emission, offering valuable
diagnostic capabilities for CME magnetic fields and SEP properties near
the Sun. Moreover, the integration of coronal and heliospheric domains
represents a key step towards global-scale simulations of CME and SEP
events from the solar surface to Earth's orbit and beyond, supporting
future efforts to untangle the complex, interconnected processes
governing space plasmas.</description>
</item>
<item>
<title> Observations of successive CMEs and their successive Type II solar radio bursts in the corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatSR..1534279V</link>
<description>This paper reports the observations of two coronal shocks from two
Coronal Mass Ejections (CMEs) for the Successive type II Solar radio
bursts observed on 02 May 2021 in the frequency range of 80  1 MHz with
the time interval of  20 minutes between them. Both the bursts show
clear band splitting features in the harmonic band. The estimated
heights for the source of the first type II burst lies in the range of
2.06  2.93  with the average speeds of 601  76, 700  91 and 783  105
km  for 2 X, 3.5 X and 5 X Saito electron density models, and the
heights for the source of the second type II burst lies in the range of
2.24  3.83  with the average speeds of 1063  113, 1287  145 and 1478
 172 km . The successive CMEs are observed by the twin Solar
Terrestrial Relations Observatory STEREO-A between 11:20  12:21 UT in
the Extreme Ultra Violet Imager (EUVI) and in the Internally Occulting
Refractive Coronagraphs (COR1) FOV, the two coronal shocks are generated
by the two successive CMEs observed at (11:30) 11:26 UT and (11:55:00)
11:56 UT according to ST-A (EUVI) COR1 observations and most likely
released from the same active region. The average speeds of CMEs at COR1
FOV are about 574  64 km  and 595  82 km . The simultaneous
observations of the EUV structures and the radio bursts, their
coinciding height-time further confirms that the successive CMEs are
responsible for the successive shocks and their related radio bursts in
the corona. The observed band-splitting in the successive type-II radio
bursts provides the compression ratios of 1.26 and 1.45 respectively.
Therefore, these observations confirms the presence of shock waves in
the corona.</description>
</item>
<item>
<title> Reconnection and Viscous Control of Dayside Field Aligned Currents for Northward Interplanetary Magnetic Field</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13034547M</link>
<description>We study the morphology and magnitude of dayside field aligned currents
(FACs) for northward interplanetary magnetic field (IMF) using
observations from the Active Magnetosphere and Planetary Electrodynamics
Response Experiment (AMPERE). For near zero IMF clock angles the FACs
form a quadrupolar pattern centered at local noon, which is associated
with the reverse convection cells driven by lobe reconnection. The
poleward pair of FACs, known as the northward ${B}_{Z}$ or NBZ FAC
system, comprises upward and downward FAC pre and post noon; and the
equatorward pair have the opposite polarity. The magnitude of the NBZ
FACs is modulated by dipole tilt and phase of the solar cycle, the
former controlling the solar zenith angle in the vicinity of the FACs,
and the latter controlling the solar radio flux at 10.7 cm (F10.7), both
of which contribute to the conductance of the ionosphere. The NBZ FACs
are also modulated by the magnitude of the IMF (or the Z component of
the IMF for near zero clock angle), which we presume controls the lobe
reconnection rate. The NBZ FACs do not respond to the X component of the
IMF, solar wind speed, nor solar wind density, so we presume that these
do not affect the lobe reconnection rate. High solar wind speed leads to
the appearance of region 1 and 2 FACs at auroral latitudes, which we
suggest are associated with a viscous interaction between the solar wind
and the magnetosphere.</description>
</item>
<item>
<title> Solar Flare Induced Gradient Drift Instability Observed by SuperDARN HF Radars</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033824C</link>
<description>Solar flares are a rapid increase in solar irradiance, specifically in X
ray and Extreme Ultraviolet spectra, which enhances the ionization in
the dayside ionosphere and creates Sudden Ionospheric Disturbances
(SIDs). SIDs are known to create space weather impacts on traveling high
frequency (HF: 330 MHz) radio waves, by disrupting the communication
channels. In this study, we examine ionospheric scatters at dawn
terminator, which stems from a severe X9.3 flare on 6 September 2017
peaked at 12:02 UT, utilizing SuperDARN HF coherent scatter radars and
Global Navigation Satellite System (GNSS) Total Electron Content (TEC)
observations. Specifically, we are interested in the transients in the
ionospheric electrodynamics at the sub auroral latitude near the
terminator stemming from the flare effect. Observations suggest that
flare induced density gradient likely favors the formation of gradient
drift instability near the dawn terminator, leading to the
irregularities observed by the SuperDARN radars with line of sight (LoS)
Doppler velocity reaching nearly 300 m/s. The flare amplifies the
eastward TEC gradient near the dawn terminator by approximately 23
times compared to a geomagnetically quiet and non flare day. The
observed irregularities, attributed to flare driven instabilities,
exhibit a velocity consistent with the equatorial return flow of
ionospheric Hall convection. In contrast to prior studies indicating
decreased cross polar cap potential and associated ionospheric
convection flow, our findings show the flare is followed by an increase
in localized electric field near the dawn terminator, as depicted in
radar LoS velocity.</description>
</item>
<item>
<title> Research on the Impact of Differences in Solar Flare Backgrounds of the Same Class on Low Frequency Time Code Time Service Signal</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033801Q</link>
<description>This study systematically investigates the impact of solar flares on the
strength and timing deviation of China's low frequency time code (BPC)
time service signals under different occurrence background conditions
based on same class M1.1 class solar flare event. Seven representative
observation cases were selected for the study, with calm day data 24
days before and after the cases used for comparison. The duration of
solar flares and whether they were accompanied by geomagnetic storms
were studied as variables. The study also conducted an in depth analysis
of the changes in BPC during solar flare occurrences using the SYM H
index, Kp index, SuperMAG geomagnetic data, and X ray flux records from
the GOES 16 satellite. The results show that when the X ray flux reaches
its peak, the BPC signals exhibit a sharp decay in strength and
fluctuations in timing deviation. The longer the duration of the flare,
the greater the disturbance to the signal. In the daytime mid period,
the response of BPC signals in the mid to low latitudes to geomagnetic
storm background is not significant, as the dominant effect of solar
radiation on exciting the D layer of the ionosphere masks the influence
of geomagnetic disturbances. This study not only reveals the impact of
background differences of same class solar flares on BPC time service
signals and provides strong support for the current understanding of
signal atmosphere interactions but also offers a theoretical basis for
the anti interference design of BPC systems.</description>
</item>
<item>
<title> Research Progress on Human Body Energy Harvesting and Storage Systems for Wearable Electronic Devices</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JEMat..54.8103L</link>
<description>With the advancement of artificial intelligence, wearable technology is
evolving toward multifunctionality, integration, flexibility, and
intelligence. Wearable electronic products such as smartwatches, fitness
bands, and medical assistive devices are increasingly prevalent in
people's lives. This trend enables rich applications such as health
monitoring, humanmachine interaction, and the Internet of Things.
Energy availability remains a significant challenge for wearable
devices, with energy harvesting emerging as an ideal alternative to
batteries in wearable technology. The rapid development of energy
harvesting creates new opportunities for wearable energy solutions.
Various energy sources can power wearable devices, including mechanical,
thermal, chemical, solar, radio frequency, wind, acoustic, vibration,
and thermal energy. However, providing stable performance over extended
periods remains highly challenging. Moreover, most wearable energy
harvesters rely on specific materials or structures, which may create
inconvenience when applied on the human body. To illustrate the power
supply and storage issues of wearable electronic devices based on the
human body, we review the latest advancements in self-charging power
systems integrated with energy harvesting and storage devices. Key
achievements in this field include the integration of various renewable
energy sources such as mechanical, solar, and thermal energies, as well
as multiple energy sources. Different integration schemes (integrated
within device modules vs. separate units or electrode modules with
shared electrodes) and various mechanisms for storing harvested energy
using electrochemical batteries or supercapacitors demonstrate promising
sustainable power systems for wearable/portable electronics or sensor
environments. These self-charging power systems, utilizing diverse
energy resources, exhibit respective advantages in the field of wearable
energy harvesting.</description>
</item>
<item>
<title> Observations of a Faint Nonthermal Onset before a GOES C-class Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...992L...1B</link>
<description>We present an analysis of a GOES C1-class flare from 2022 September 6,
which was jointly observed as occulted by Nuclear Spectroscopic
Telescope ARray (NuSTAR) and on-disk by Spectrometer/Telescope for
Imaging X-rays (STIX). NuSTAR observed faint coronal nonthermal emission
as well as plasma heating &gt;10 MK, starting 7 minutes prior to the flare.
This onset emission implies that during this time, there is a continuous
electron acceleration in the corona, which could also be responsible for
the observed heating. The nonthermal model parameters remained
consistent throughout the entire onset, indicating that the electron
acceleration process persisted during this time. Furthermore, the onset
coincided with a series of type III radio bursts observed by Long
Wavelength Array-1, further supporting the presence of electron
acceleration before the flare began. We also performed spectral analysis
of the impulsive flare emission with STIX (thermal and footpoint
emission). STIX footpoints and the onset coronal source were found to
have similar electron distribution power-law indices, but with increased
low-energy cut-off during the flare time. This could suggest that the
nonthermal onset is an early signature of the acceleration mechanism
that occurs during the main phase of the flare.</description>
</item>
<item>
<title> Possible First Detection of Gyroresonance Emission from a Coronal Mass Ejection in the Middle Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...992..143M</link>
<description>Routine measurements of the magnetic field of coronal mass ejections
(CMEs) have been a key challenge in solar physics. Making such
measurements is important both from a space weather perspective and for
understanding the detailed evolution of the CME. In spite of significant
efforts and multiple proposed methods, achieving this goal has not been
possible to date. Here we report the first possible detection of
gyroresonance emission from a CME. Assuming that the emission is
happening at the third harmonic, we estimate that the magnetic field
strength ranges from 7.9 to 5.6 G between 4.9 and 7.5 R&lt;SUB&gt;&lt;/SUB&gt;. We
also demonstrate that this high magnetic field is not the average
magnetic field inside the CME, but most probably is related to small
magnetic islands, which are also being observed more frequently with the
availability of high-resolution and high-quality white-light images.</description>
</item>
<item>
<title> Predicting Solar Magnetic Activity from S&lt;SUB&gt;ph&lt;/SUB&gt; and Seismic Parameters Using Random Forest Regression</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...992...99K</link>
<description>We investigate the potential of using the photometric magnetic proxy
S&lt;SUB&gt;ph&lt;/SUB&gt; and seismic parameters, such as the frequency of maximum
power (max) and the large frequency separation (), derived from Solar
and Heliospheric Observatory/Variability of Solar Irradiance and Gravity
Oscillations observations to predict the 10.7 cm solar radio flux, a
widely used index of solar magnetic activity. A random forest regression
model is trained and tested on time series divided into multiple
temporal subsets and input parameter combinations. The model achieves
strong predictive performance (R&lt;SUP&gt;2&lt;/SUP&gt; &gt; 0.92) across
configurations and significantly outperforms a classical linear
regression model. Our results show that S&lt;SUB&gt;ph&lt;/SUB&gt; effectively
captures long-term variations, while the seismic amplitude parameter
Hmax is more responsive to short-term fluctuations. Combining
S&lt;SUB&gt;ph&lt;/SUB&gt; with the full set of seismic parameters yields the
highest accuracy and offers a promising approach for diagnosing activity
in other solar-like stars where direct magnetic field measurements are
infeasible.</description>
</item>
<item>
<title> Relevance to PSP and Other Space Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...992...80S</link>
<description>The aim of this paper is to demonstrate that electron current
oscillations may generate electromagnetic waves as type III radiation
and whistler waves without the involvement of the classical plasma
emission via the coalescence of waves. Particle-in-cell (PIC) simulation
results of a corestrahl plasma without initial current compensation are
presented, which describe the conversion of current-driven Langmuir
oscillations/waves into type III radiation, whereby simultaneously
whistler waves are excited. In contrast to the classical approach of V.
L. Ginzburg &amp; V. V. Zhelezniakov, after which beam-excited Langmuir
waves in a two-step process are converted into electromagnetic
radiation, any instability is suppressed by selecting a low strahl
velocity. Rather, electric field oscillations at the electron plasma
frequency are triggered by the initially noncompensated current of the
strahl. The arising electromagnetic fields exhibit amplitude
oscillations, which are caused by the superposition of the two wave
modes of mixed polarization at the point of mode coupling. This basic
mechanism of wave generation and transformation has already been
described in earlier papers using simple fluid models. It is also the
topic of the companion paper. Besides the fundamental electromagnetic
radiation, the second harmonic of nearly the same intensity has been
obtained, which is an indication of its generation by nonlinear
currents. Measurements of Langmuir waves, type III radiation, and
whistler waves on board various satellites in the solar wind, in
particular Parker Solar Probe observations, are analyzed in the light of
our results. Interpretations of earlier PIC simulations are critically
reviewed.</description>
</item>
<item>
<title> AIA and RHESSI Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...992...43K</link>
<description>We present a comprehensive multiwavelength analysis of a coronal mass
ejection (CME) on 2014 January 8 from the active region (AR) NOAA 11947
by analyzing the data from Atmospheric Imaging Assembly (AIA) on board
Solar Dynamics Observatory, RHESSI, and Hiraiso Radio Spectrograph. The
CME is associated with an M3.6 flare and filament eruption. Observations
from the AIA 171  images reveal the origin of pre-CME arcade 1 hr
prior to the eruptive event. Before the onset of event, the hot AIA 131
and 94  images exhibit an existence of a hot flux rope, which on
eruption results in the activation and eruptive expansion of the pre-CME
coronal arcade. The eruptive process of pre-CME arcade consists of a
slow rise evolution with a speed 3 km s&lt;SUP&gt;1&lt;/SUP&gt;, "arcade-to-
bubble" transformation, and blowout expansion of the CME-bubble with a
fast speed of 400 km s&lt;SUP&gt;1&lt;/SUP&gt;. A differential emission measure
analysis suggests the presence of multithermal plasma in the bubble-
structure and strong plasma heating at the core of the AR. A blowout
expansion of CME is accompanied with multiple type III and a split-band
type II radio bursts in association with X-ray emission up to 50 keV
energies from its source region. Our observations reveal that the
formation and expansion of the CME-bubble serve as the earliest
signatures of the CME, capturing its development in the low corona.
Concurrent X-ray and radio emissions further highlight the critical role
of large-scale magnetic reconnection in powering both the flare
emissions and the early evolution and dynamics of the CME.</description>
</item>
<item>
<title> Ion-scale Turbulence and Energy Cascade Rate in the Solar Corona and Inner Heliosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...991L..57K</link>
<description>Plasma turbulence cascading from MHD to kinetic scales in the
heliospheric plasma is believed to play a key role in coronal heating
and fast solar wind acceleration, but the properties of the turbulence
remain poorly constrained by observations. Here we compare the ion-scale
density fluctuation levels inferred from the properties of solar radio
bursts with the magnetic field fluctuation levels obtained through in
situ measurements in the inner heliosphere. We find that the observed
magnetic and density fluctuation amplitudes are consistent with
excitation by kinetic Alfvn waves (KAWs) and/or KAW structures over a
broad range of distances from the Sun. We then use the radio diagnostics
and the KAW scenario to deduce the radial variation of magnetic
fluctuation amplitudes in regions close to the Sun where in situ
measurements cannot be obtained. Further, we calculate the energy
cascade rate (plasma heating rate) profile over a region that extends
from the low corona (0.1 R&lt;SUB&gt;&lt;/SUB&gt;) into the heliosphere (out to 1
au), and compare it to the energy deposition rate required to drive the
solar wind. The cascade rate agrees with the available in situ
measurements and also provides predictions closer than 10 R&lt;SUB&gt;&lt;/SUB&gt;
where in situ approaches are not available. The results provide unique
diagnostics of the ion-scale plasma turbulence amplitude and energy
cascade rate spanning over 3 orders of magnitude in solar distance.</description>
</item>
<item>
<title> A Monte Carlo Simulation on the Scattering Coefficients of Solar Radio Wave Propagation</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...991..153G</link>
<description>Radio waves undergo scattering by small-scale density fluctuations
during propagation through the solar-terrestrial environment,
substantially affecting the observed characteristics of solar radio
bursts. This scattering process can be effectively modeled as photon
diffusion in phase space. In this study, we present a comprehensive
comparison between the quasilinear diffusion coefficients and those
calculated by ray-tracing the photon trajectories in numerically
generated, broadband, isotropic density fluctuation fields in both 2D
and 3D configurations. The comparative analysis demonstrates that for
weak scattering, the simulated diffusion coefficients agree well with
the quasilinear theoretical predictions. However, when the radio
frequency approaches the electron plasma frequency and/or the density
fluctuation amplitude becomes significant, photons experience strong
scattering. Under such conditions, the quasilinear theory tends to
underestimate the scattering strength of photons induced by 2D density
fluctuations while overestimating the scattering strength in 3D cases.
Furthermore, we implement a group velocity correction to the theoretical
diffusion coefficients, based on the effective propagation speed
averaged over all test photons. The corrected coefficients provide an
accurate quantification of the scattering strength for radio waves
propagating through 3D density fluctuations. The physical mechanisms
underlying these phenomena are elucidated in the discussion.</description>
</item>
<item>
<title> Possible contribution of ground motion to modify ionosphere before the 2011 Tohoku-Oki Mw9.1 earthquake</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.4573C</link>
<description>This study examines the complex interrelationships among ionospheric
NmF2 variations, solar activity F10.7 index, and crustal movements
preceding the 2011 Tohoku-Oki earthquake. NmF2 from 5 ionospheric
stations (Yakutsk, Khabarovsk, Wakkanai, Kokubunji, and Jeju) is studied
together with vertical movement observed by Hi-net tilt meters in Japan.
Results showed that while daytime NmF2 typically correlates with solar
activity (F10.7 solar radio flux), significant deviations were observed
during specific periods. During these intervals, NmF2 variations did not
correlate with space weather parameters as expected but correlate with
the vertical ground motion. We explain these phenomena as due to the
enhanced dynamo electric field, which is produced originally by the
vertical ground motion. Our findings suggest that the ionosphere before
the large earthquake is influenced by the complex Lithosphere-
Atmosphere-Ionosphere interaction such as crustal movements, acoustic-
gravity waves, and dynamo electric field variations.</description>
</item>
<item>
<title> Effects of X2.8-class solar flare on the ionosphere occurred during the recovery phase of a geomagnetic storm over South American and Antarctic sectors</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.4539D</link>
<description>In this investigation, we present and discuss the effects of an
X2.8-class solar flare occurred on 14 December 2023 on the ionospheric F
region and on the geomagnetic field over South American and Antarctic
sectors. This flare coincides with the recovery phase of a geomagnetic
storm. To this end, we rely on vertical total electron content (VTEC)
observations from nearly 250 Global Positioning System (GPS) receiver
stations over South American and Antarctic sectors, complemented by in-
situ electron density observations from Swarm satellites, magnetometer
measurements, and ionospheric sounding observations from ionosondes. The
magnetic observations show a large increase in the variations of the
horizontal component (H) of the geomagnetic field and equatorial
electrojet (EEJ) currents at all stations, synchronized with the
increase in X-rays flux, indicating solar flare effects or magnetic
crochet on the Earth's geomagnetic field. VTEC shows how the impact of
the solar flare on the ionosphere is enhanced from east to west of South
America in the equatorial and low-latitudes. VTEC from a specific GPS
satellite-receiver also shows great effects at mid-latitudes. Results
are confirmed and further elaborated through Swarm in-situ observations.
In addition, an asymmetry is observed in the equatorial ionization
anomaly (EIA), in which the eastern South American sector shows an
intensified EIA compared to the western sector. Ionospheric sounding
observations by ionosondes show total fade out in the echo traces of the
ionograms, characterizing blackouts in the radio signals from equatorial
to low-latitudes. Overall, our results show that an X-class solar flare
occurring near the limb of the solar disk is capable of producing
effects on the Earth's ionosphere with similar or even stronger
intensities than flares occurring at the center of the solar disk.</description>
</item>
<item>
<title> A wide-band high-frequency type-II solar radio burst</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...702A..15V</link>
<description>Aims. Type-II radio bursts are typically observed below 400 MHz and are
characterized by the narrowband, slowly drifting fundamental and
harmonic structures. Here we report an unusual high-frequency wide-band
type-II burst with a starting frequency as high as 670 MHz and an
instantaneous bandwidth as wide as 300 MHz. Methods. We used radio
imaging from the Nanay Radio Heliograph, spectroscopic data from
ORFEES, extreme-ultraviolet (EUV) observations from Solar Dynamics
Observatory, and white-light observations from LASCO to determine the
nature and origin of the observed radio burst as well as its propagation
in the corona. Results. The estimated average spectral drift is 2.18
MHz s&lt;SUP&gt;1&lt;/SUP&gt;, its mean duration at each frequency is 3 min, and
the maximum brightness temperature can exceed 10&lt;SUP&gt;11&lt;/SUP&gt; to
10&lt;SUP&gt;12&lt;/SUP&gt; K. According to the simultaneous EUV and radio imaging
data, the radio sources are distributed over a relatively broad region
centered on a dip in the nose front of the shock-like EUV wave
structure. The dip is likely caused by the strong interaction of the
eruption with the overlying closed dense loops that are enclosed by the
large-scale streamer structure, indicating that the type-II burst
originates from coronal mass ejection shocks interacting with dense,
closed-loop structures. Conclusions. The observations suggest that the
unusual wide-band high-frequency type-II radio burst originates from a
dense streamer region in the corona; this is further evidenced by an EUV
shock-like structure that steepens very close to the solar surface, at
1.23 R&lt;SUB&gt;&lt;/SUB&gt;, and the fact that the type-II radio source
coincides with the shock dip. The wide-band feature is due to the source
stemming from a region with significant density variations and not due
to the intensity variations across the shock structure.</description>
</item>
<item>
<title> Study on the Variation of Low-Frequency Time Code Signals During Medium to Large Solar Flare Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RaSc...6008186Q</link>
<description>This study is based on the 68.5 kHz signal transmitted by China's low-
frequency time code time service system (BPC) and systematically
researches the effects of medium to large solar flares (M/X-class) on
low-frequency time code signals. By analyzing the field strength and
timing deviation data of the BPC signal during 20 typical flare events,
the study reveals the variation patterns of low-frequency time code
signals under disturbances from medium to large solar flares. Case
analyses indicate that, during such flares, the BPC signal intensity
exhibits two response patterns: a single-valley structure and a double-
valley structure. The BPC signal response is divided into two stagesa
rapid change phase and a gradual change phasewhich show a strong linear
relationship with the development of the solar flare. Meanwhile, the BPC
timing deviation displays a bipolar pulse characteristic, and after the
flare, the instability in signal performance is closely associated with
the double-valley response in field strength. These phenomena suggest
that the changes in the BPC time code signal are closely related to the
effects of ionospheric disturbances during solar flares on the
superposition characteristics of the BPC ground-wave and sky-wave
signals. This first systematic investigation analyzes low-frequency
time-code signal variation during medium-to-large solar flares,
revealing their response characteristics. It provides significant
insights into the low-frequency time-code signal propagation-solar
activity association and lays a solid theoretical foundation for
improving time-service stability and reliability.</description>
</item>
<item>
<title> Statistical Study of DH Type II Bursts and Associated CMEs During Solar Cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RAA....25i5002T</link>
<description>Decameter-hectometric (DH) Type II bursts, arising from coronal mass
ejection (CME)-driven shock waves, are crucial for understanding solar-
terrestrial interactions and space weather forecasting. This study
provides a comprehensive statistical analysis of CMEs associated with DH
type II solar radio bursts during Solar Cycle 24 (20092019), utilizing
data from the Wind/WAVES, Solar TErrestrial RElations
Observatory/SWAVES, and Solar and Heliospheric Observatory/LASCO
catalogs. Analyzing 180 events, we report key spectral and kinematic
properties, including a mean CME speed of (1058  531) km s&lt;SUP&gt;1&lt;/SUP&gt;
and a mean width of (288.39  99.3), with 62% classified as halo CMEs.
About 12% of the total CMEs are accelerated, 58% of them are
decelerated, and 30% of them are constant. Similarly, CMEs having a
speed  800 km s&lt;SUP&gt;1&lt;/SUP&gt; are constant, and those with speed  800
km s&lt;SUP&gt;1&lt;/SUP&gt; are decelerated. DH type II bursts displayed a mean
starting frequency of (12,169.72  4939) kHz, ending frequency of
(2152.69  3022.07) kHz, bandwidth of (10,017  5353) kHz, and an
average duration of (345.62  453) minutes. A power-law relationship was
established between the drift rate (df/dt) and burst duration (D),
characterized by df/dt = 2749.07  D&lt;SUP&gt;0.88&lt;/SUP&gt;, highlighting the
inverse dependence of drift rate on burst longevity. This suggests a
dynamic interplay between shock parameters and the ambient solar corona.
The findings underscore the persistent and robust spectral coverage of
CME-driven shocks, offering new insights into their evolution and impact
on the heliospheric environment.</description>
</item>
<item>
<title> Radiation efficiency of electromagnetic wave modes from beam-generated solar radio sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatAs...9.1292K</link>
<description>During type III solar radio bursts, electromagnetic waves are radiated
at the plasma frequency &lt;SUB&gt;p&lt;/SUB&gt; and its harmonics by electrostatic
wave turbulence generated by electron beams ejected from the Sun in
randomly inhomogeneous solar wind and coronal plasmas. These emissions,
detected for decades by spacecraft and radiotelescopes, are split by the
plasma magnetic field into three modes, X, O and Z, with different
dispersion, polarization and radiation properties. Here, using three
independent and converging approachesparticle-in-cell simulations, a
theoretical model of waves in a random medium and analytical
calculations in the framework of turbulence theorywe demonstrate that
only a small fraction of electromagnetic energy radiated at
&lt;SUB&gt;p&lt;/SUB&gt; (10%) escapes from beam-generated radio sources, mainly
as O-mode waves and, depending on plasma conditions, as X-mode waves.
Most energy is radiated in the Z -mode and can therefore be observed
only close to sources. The results provide strong support for
interpretation of observations performed up to close distances from the
Sun by spacecraft such as Parker Solar Probe and Solar Orbiter. This
work, based on general approaches requiring few assumptions, makes it
possible to study the properties of radio emission under realistic solar
conditions, and thereby provides a solid basis for the development of
theoretical tools for probing space and time variations of beam-plasma
systems in the solar wind.</description>
</item>
<item>
<title> Detecting fast-variation pulsations in solar hard X-ray and radio emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2025MNRAS.542L..48L</link>
<description>Quasi-periodic pulsations (QPPs) at sub-second periods are frequently
detected in the time series of X-rays during stellar flares. However,
such rapid pulsations are rarely reported in the hard X-ray (HXR)
emission of the small solar flare. We explored the QPP patterns with
fast-time variations in HXR and radio emissions produced in a small
solar flare on 2025 January 19. By applying the fast Fourier transform,
the fast-variation pulsations at a quasi-period of about 1 s are
identified in the HXR channel of 2080 keV, which were simultaneously
measured by the Hard X-ray Imager and the Konus-Wind. The rapid
pulsations with a same quasi-period were also detected in the radio
emission at a lower frequency range of about 40100 MHz. The
restructured HXR images show that the QPP patterns mainly locate in
footpoint areas that connect by hot plasma loops, and they appear in the
flare impulsive phase. Our observations suggest that the fast-variation
pulsations could be associated with non-thermal electrons that are
periodically accelerated by the intermittent magnetic reconnection, and
the 1-s period may be modulated by the coalescence instability between
current-carrying loops and magnetic islands.</description>
</item>
<item>
<title> An assessment of potentially space weather causing CMEs through analysis of associated interplanetary type II solar radio bursts and solar energetic particle events</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JASTP.27406579U</link>
<description>This study investigates the space weather implications of coronal mass
ejections (CMEs) by analyzing 39 metric type II solar radio bursts with
decametrichectometric (DH) counterparts during a segment of Solar Cycle
24. To minimize projection effects, only limb CMEs originating far from
the solar disk center (central meridian distances between&lt;mml:math&gt;&lt;mml:
mrow&gt;&lt;mml:mi&gt;60&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; and &lt;mm
l:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;90&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:m
ath&gt;) were considered. The events were categorized into three groups:
(i) all metric type II bursts with DH counterparts (m-DH), (ii) those
accompanied by solar energetic particle (SEP) events (m-DH-SEP), and
(iii) those without SEP events (m-DH-NonSEP). Analysis of CME parameters
revealed that m-DH-SEP events are associated with faster (average speed
of 1203 km/s) and wider CMEs compared to m-DH-NonSEP events (average
speed of 333 km/s). Additionally, the fraction of halo CMEs increased
across the groups: m-DH-NonSEP (62.5%), m-DH (74.3%), and m-DH-SEP
(93%). A strong positive correlation (Pearson's CC = 0.76;&lt;mml:math&gt;&lt;mml
:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;SE&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:m
i&gt;cc&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;mml:mo&gt;=&lt;/mml:mo&gt;&lt;mml:mi&gt;0.18&lt;/mml:m
i&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;) was found between CME speeds and the
logarithmic peak intensity of SEP events. Notably, 87% of m-DH-SEP
events originated from the western hemisphere in StonyHurst coordinates,
consistent with favorable magnetic connectivity to Earth. Further
analysis indicated that 62.5% of western hemisphere metric type II
bursts with DH counterparts were followed by SEPs at Earth, compared to
only 13% without DH counterparts. These findings confirm that fast and
wide CMEs associated with DH type II bursts are effective in
accelerating energetic particles, underscoring the significance of DH
type II bursts as indicators of SEP events and their relevance in space
weather forecasting.</description>
</item>
<item>
<title> demonstration of technical readiness and initial science highlights</title>
<link>https://ui.adsabs.harvard.edu/abs/2025FrASS..1266743K</link>
<description>Solar radio emissions offer unique diagnostic insights into the solar
corona. However, their dynamic and multiscale nature, along with several
orders of magnitude variations in intensity, pose significant
observational challenges. To date, at gigahertz frequencies, MeerKAT
stands out globally with high potential of producing high-fidelity,
spectroscopic snapshot images of the Sun, enabled by its dense core,
high sensitivity, and broad frequency coverage. Yet, as a telescope
originally designed for observing faint galactic and extragalactic
sources, observing the Sun at the boresight of the telescope requires
customized observing strategies and calibration methods. This work
demonstrates the technical readiness of MeerKAT for solar observations
at the boresight of the telescope in the UHF (5801015 MHz) and L-band
(9001670 MHz) frequency ranges, including optimized modes, a dedicated
calibration scheme, and a tailored, entirely automated calibration and
imaging pipeline. The quality of solar images is validated through
morphological comparisons with the solar images at other wavelengths.
Several unique early science results showcase the potential of this new
capability of MeerKAT. Once fully commissioned and operational, this
will unlock novel solar studies, significantly expand the scientific
portfolio of MeerKAT, and lay the groundwork for solar observations with
the mid-frequency telescope of the upcoming Square Kilometre Array
Observatory, for which MeerKAT serves as a precursor.</description>
</item>
<item>
<title> The Time Delays in Reaction of the Ionosphere and the Earth's Magnetic Field to the Solar Flares on 8 May and Geomagnetic Superstorm on 10 May 2024</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Atmos..16.1106S</link>
<description>In the paper we consider the pulsed disturbances caused in the
ionosphere by an extreme G5-level geomagnetic superstorm on 10 May 2024,
and by the X1.0 and M-class solar flares on 8 May 2024, which preceded
the storm. Particular attention is paid to the short-term delays and the
sequence of disturbance appearance in the ionosphere and geomagnetic
field during these extreme events. The results of a continuous Doppler
sounding of the ionosphere on an inclined radio path with a sampling
frequency of 25 Hz were used, as well as the data of a ground-based mid-
latitude fluxgate magnetometer LEMI-008, and an induction magnetometer
IMS-008, which operated with a sampling frequency of 66.6 Hz. Ionization
of the ionosphere by the intense X-ray and extreme ultraviolet radiation
of solar flares was accompanied by the equally sudden and similarly
timed disturbances in the Doppler frequency shift (DFS) of the
ionospheric signal, which had an amplitude of 2.05.8 Hz. The largest
pulsed burst in DFS was registered 68 s after an X1.0 flare on 8 May
2024 at the time when the change of the X-ray flux was at its maximum.
Following onto the effect in the ionosphere, a disturbance in the
geomagnetic field appeared with a time delay of 35 s. This disturbance
is a secondary one that arose as a consequence of the ionosphere
response to the solar flare. It was likely driven by the contribution of
ionospheric currents and electric fields, which modified the Earth's
magnetic field. On 10 May 2024, a G5-level geomagnetic superstorm with a
sudden commencement triggered an impulsive reaction in the ionosphere. A
response in DFS at the calculated reflection altitude of the sounding
radio wave of 267.5 km was detected 58 s after the commencement of the
storm. The sudden impulsive changes in Doppler frequencies showed a
bipolar character, reflecting complex dynamic transformations in the
ionosphere at the geomagnetic storm. Consequently, the DFS amplitude
initially rose to 5.5 Hz over 86 s, and then its sharp drop to 3.2 Hz
followed. Using the instruments that operated in a mode with a high
temporal resolution allowed us to identify for the first time the
impulsive nature of the ionospheric reaction, the time delays, and the
sequence of disturbance appearances in the ionosphere and geomagnetic
field in response to the X1.0 solar flare on 8 May 2024 as well as to
the sudden commencement of the extreme G5-level geomagnetic storm on 10
May 2024.</description>
</item>
<item>
<title> hyperparameter selection</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AstTI...2..280D</link>
<description>Radio interferometric imaging samples visibility data in the spatial
frequency domain and then reconstructs the image. Because of the limited
number of antennas, the sampling is usually sparse and noisy. Compressed
sensing-based on convex optimization is an effective reconstruction
method for sparse sampling conditions. The hyperparameter for the
l&lt;SUB&gt;1&lt;/SUB&gt; regularization term is an important parameter that
directly affects the quality of the reconstructed image. If its value is
too high, the image structure will be missed. If its value is too low,
the image will have a low signal-to-noise ratio. The selection of
hyperparameters under different levels of image noise is studied in this
paper, and solar radio images are used as examples to analyze the
optimization results of compressed sensing algorithms under different
noise conditions. The simulation results show that when the salt-and-
pepper noise density is between 10% and 30%, the compressed sensing
algorithm obtains good reconstruction results. Moreover, the optimal
hyperparameter value has a linear relationship with the noise density,
and the mean squared error of regression is approximately .</description>
</item>
<item>
<title> Imaging and Radio Signatures of ShockPlasmoid Interaction</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...991L...3K</link>
<description>Understanding how shocks interact with coronal structures is crucial for
understanding the mechanisms of particle acceleration in the solar
corona and inner heliosphere. Using simultaneous radio and white-light
observations, we investigate the interaction between a coronal mass
ejection (CME)-driven shock and a plasmoid. LASCO and STEREO-A COR-2
white-light images are analyzed to track the evolution of the plasmoid,
CME, and its associated shock, while the Wind/WAVES and STEREO/WAVES
dynamic spectra provide complementary radio signatures of the
shockplasmoid interaction at 7 R&lt;SUB&gt;&lt;/SUB&gt;. An interplanetary type
II radio burst was detected as the shock propagated through the
plasmoid. The merging of the plasmoid into the CME was accompanied by
interplanetary type III radio bursts, suggesting escaping electron beams
during the reconnection process. These observations clearly demonstrate
that shockplasmoid interactions can enhance the efficiency of particle
acceleration associated with CMEs, with implications for electron
acceleration in flare and heliospheric current sheets as well.</description>
</item>
<item>
<title> Measuring the Magnetic Field of a Coronal Mass Ejection from the Low to Middle Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...990L..50C</link>
<description>A major challenge in understanding the initiation and evolution of
coronal mass ejections (CMEs) is measuring the magnetic field of the
magnetic flux ropes (MFRs) that drive CMEs. Recent developments in radio
imaging spectroscopy have paved the way for diagnosing the CMEs'
magnetic field using gyrosynchrotron radiation. We present magnetic
field measurements of a CME associated with an X5-class flare by
combining radio imaging spectroscopy data in microwaves (118 GHz) and
meter waves (2088 MHz), obtained by the Owens Valley Radio
Observatory's Expanded Owens Valley Solar Array (EOVSA) and Long
Wavelength Array (OVRO-LWA), respectively. EOVSA observations reveal
that the microwave source, observed in the low corona during the
initiation phase of the eruption, outlines the bottom of the rising MFR-
hosting CME bubble seen in extreme ultraviolet and expands as the bubble
evolves. As the MFR erupts into the middle corona and appears as a
white-light CME, its meter-wave counterpart, observed by OVRO-LWA,
displays a similar morphology. For the first time, using gyrosynchrotron
spectral diagnostics, we obtain magnetic field measurements of the
erupting MFR in both the low and middle corona, corresponding to coronal
heights of 0.02 and 1.83 R&lt;SUB&gt;&lt;/SUB&gt;. The magnetic field strength is
found to be around 300 G at 0.02 R&lt;SUB&gt;&lt;/SUB&gt; during the CME initiation
and about 0.6 G near the leading edge of the CME when it propagates to
1.83 R&lt;SUB&gt;&lt;/SUB&gt;. These results provide critical new insights into the
magnetic structure of the CME and its evolution during the early stages
of its eruption.</description>
</item>
<item>
<title> Plasma Instability in Front of Ejected Energetic Electrons and Type III Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...990..100K</link>
<description>Type III radio bursts are signatures of the fluxes of near-relativistic
electrons ejected during solar flares. These bursts are frequently
observed by spacecraft such as the Parker Solar Probe. It has been
traditionally believed that these electron beams generate Langmuir waves
through the two-stream instability, which are then converted into
electromagnetic waves. In this study, we revise that model, by examining
how the electron distribution becomes truncated due to the "time-of-
flight" effect, as the beam travels through a randomly inhomogeneous and
gently varying solar wind plasma. Rather than the two-stream
instability, this truncation destabilizes the distribution and leads to
the generation of Langmuir waves via a linear instability; we confine
our analysis to this linear regime and do not take into account the
backreaction of the generated Langmuir waves on the electron
distribution, which is nonlinear. The instability grows until slower
electrons arrive and dampen the waves. Our qualitative analysis shows
that the resulting wave intensity growth and decay closely match the
intensitytime profile of observed type III radio bursts at the
fundamental frequency, supporting this modified theory.</description>
</item>
<item>
<title> Low-Frequency Type II Radio Bursts and Associated Solar Flares, Coronal Holes, and CMEs During 2001 to 2015</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Ap.....68..387M</link>
<description>We have analyzed 20 low-frequencies (LF) type-II radio bursts associated
with solar coronal mass ejections (CMEs), coronal holes (CHs), and solar
flares observed during the solar cycle 23 and solar cycle 24, which
consist of the period of year 1997 to year 2015. A total number of 505
types-II radio bursts were observed during the above period out of which
only 20 types II radio bursts have frequencies  1 MHz. The time
duration of 20 LF type II bursts ranges from 5 min to 2020 min. On
investigation of 17 type-II bursts associated CMEs, solar flares, and
coronal holes we also found that 12 types-II burst related CMEs observed
when there were CHs and solar flares within 10 and 5 type-II burst-
associated CMEs found when there were CHs and solar flares within 30,
respectively. In this paper we have done statistical analysis of low
frequency type II radio bursts and related solar phenomena. The LF type-
II radio bursts start after the peak time of associated solar flares. In
this paper each LF type-II radio burst and other related solar phenomena
are seen and analyzed to understand the origin of LF type-II radio
bursts from the Sun in the latest scenario of solar heliophysics.</description>
</item>
<item>
<title> A short-term prediction of ionospheric TEC using the RF-Prophet model for GNSS stations in China</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..76.3654T</link>
<description>The ionospheric total electron content (TEC) is a crucial parameter for
studying ionospheric variability and space weather. Short-term
forecasting of the ionosphere is also vital for detecting near-Earth
space environment changes. This study proposes a random forest (RF)
feature selection method combined with the Prophet model. The best
features are selected by random forest training, and the Prophet model
is used to forecast ionospheric TEC data for the short term. This paper
presents the construction of the RF-Prophet model using TEC data from 16
GNSS stations at CMONOC and five parameters selected through training,
namely Lyman alpha, Auroral Electrojet Index (AU index), Polar Cap Index
(PC-index), Auroral Lower Index (AL index), and Solar Radio Flux at 10.7
cm (F10.7). The model's performance is evaluated by comparing it with a
single Prophet model, using 30 days of historical TEC data as the
training set and selecting a one-day sliding forecast experiment for the
2015 high solar activity and 2018 low solar activity years. The
experimental results indicate that the RF-Prophet model has a lower one-
year average root mean square error (RMSE) of all stations in the 2015
and 2018 test sets compared to the Prophet model. Specifically, in the
2015 test set, the RMSE of the RF-Prophet model improved by 9.40 %
compared with the Prophet model; in the 2018 test set, the RMSE of the
RF-Prophet model improved by 7.19 % compared with the Prophet model.</description>
</item>
<item>
<title> Pre-Flare Current Sheet, Build-Up of Eruptive Filament, Flare and Eruption Onset in the Frame of the Tether-Cutting Magnetic Reconnection Scenario</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ARep...69..864S</link>
<description>We present multiwavelength analysis of the pre-flare phase, as well as
the onset of the powerful X4.9 near-limb eruptive solar flare on
February 25, 2014 (SOL2014-02-25T00:39), revealing the tether-cutting
geometry. This event provides an excellent opportunity to investigate
pre-flare and flare energy release in details utilizing available large
volume of observational data in different spectral ranges, suitable limb
position of the flare, high power of its energy release, favorable
spatial distribution of pre-flare and flare emission sources and well-
observed eruption. We aim at determining relationship between the region
of pre-flare energy release with the regions where the flare started to
develop, and to investigate a detailed chronology of energy release
during the pre-flare time interval and the beginning of the impulse
phase. Using X-ray, ultraviolet (UV) and radio microwave data we found
that the pre-flare energy release site was compact and localized in the
vicinity of interaction (tether-cutting type) of larger-scale magnetic
structures near the polarity inversion line of the magnetic field. The
analysis indicates that a pre-flare current sheet could be in this
region. Good correspondence between the location of the pre-flare and
flare emission sources visible at the very beginning of the impulsive
phase is shown. We found relationship between dynamics of the energy
release in the pre-flare current sheet and formation of the future flare
eruptive structure. The growth of the magnetic flux rope was associated
with activation of plasma emissions, flows and an increase of UV
radiation fluxes from the region where the pre-flare current sheet was
located. The eruptive flux rope gradually grew due to "feeding" by
magnetized plasma ejected from the reconnecting pre-flare current sheet.
Finally, it is shown that the most probable trigger of the eruption was
a local fast microflare-like magnetic reconnection in the pre-flare
current sheet. Some local instability in the pre-flare sheet could lead
to a transition from the slow to fast reconnection regime. As a result,
an ejection from the sheet was initiated and the eruptive flux rope lost
its stability. Then, the eruptive flux rope itself initiated formation
of the main reconnecting flare current sheet as in the Standard Flare
Model (under the flux rope) during its movement, and intense emissions
associated with the impulsive phase were observed.</description>
</item>
<item>
<title> Bidirectional anisotropic solar energetic particle events observed by Solar Orbiter</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...701A.123D</link>
<description>Context. Solar energetic particle (SEP) events are critical for
understanding particle acceleration and transport in the heliosphere.
While most SEP events involve outward streaming particles along open
magnetic field lines, bidirectional events characterized by simultaneous
sunward and anti-sunward particle flows offer unique insights into
magnetic field topology and the interplay of multiple acceleration
sources. Aims. We investigate the origin and transport of energetic
particles in two rare bidirectional anisotropic SEP events observed by
Solar Orbiter, with a particular emphasis on their association with
magnetic flux ropes. Methods. Energetic particles, solar wind plasma,
magnetic field, and solar radio measurements were analysed. Via the
velocity dispersion analysis, we determined release times and path
lengths for distinct particle populations. Automated flux rope
identification and magnetic helicity diagnostics were used to
characterize magnetic flux ropes. Results. Both events showed two clear
velocity dispersion signatures with opposite particle anisotropies
during their onset phase. The sunward streaming protons, characterized
by a delayed release time, a harder spectral index, and higher
intensities, may be due to coronal mass ejection-driven shock
acceleration, while the promptly released anti-sunward streaming protons
are likely linked to flare acceleration. Notably, in both cases, small-
scale flux ropes were identified in situ during the time intervals
corresponding to the bidirectional particle streaming. Path lengths
derived for sunward and anti-sunward injections were substantially
greater than nominal values of the Parker field lines, further evidence
of the role of the flux rope in shaping particle trajectories.
Conclusions. These observations demonstrate that magnetic flux ropes can
significantly affect magnetic connectivity to the source region and SEP
propagation in the inner heliosphere, and that simultaneous velocity
dispersion from two distinct particle sources can be used to place
direct constraints on the topology of the flux rope. Our results
highlight the value of combining particle anisotropy, release time,
source spectra, and magnetic structure diagnostics to unravel SEP
transport in complex transient magnetic structures, and also present new
challenges for the current SEP transport model.</description>
</item>
<item>
<title> Modelling gyrosynchrotron emission from coronal energetic electrons in a CME flux rope</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...701A..53H</link>
<description>Context. Solar flares and coronal mass ejections (CMEs) can accelerate
electrons, causing bursts such as type IV emissions in the solar radio
continuum. Although radio spectroscopy is a powerful diagnostic tool for
the corona, the origin and mechanisms of type IV bursts remain
uncertain. In situ measurements can occasionally shed some light on
these mechanisms, but they are limited in space and time. Sophisticated
numerical modelling offers the best approach to improve our
understanding of the physical processes underlying particle dynamics and
radio emission. Aims. This research examines type IV radio bursts,
exploring the effects of various electron distribution properties and
CMEs on their generation and characteristics. To transcend idealised
assumptions, we employed realistic anisotropic electron distributions 
obtained from particle transport simulations within complex
magnetohydrodynamic (MHD) environments  as input for radio emission
models. Methods. We used the three-dimensional coronal MHD model COCONUT
to generate coronal background configurations, including a CME modelled
as an unstable modified TitovDmoulin magnetic flux rope (MFR). These
MHD simulations were used by the PARADISE particle transport code, which
injects energetic electrons into the MFR and tracks their evolution.
Finally, we fed the electron distributions and solar wind parameters
into the Ultimate Fast Gyrosynchrotron Codes to compute radio emission
along lines of sight. Results. Electrons injected close to the flux
rope's central axis remained largely confined, producing a
gyrosynchrotron emission spectrum resembling observed type IV
characteristics. Varying observer positions, CME properties, and
spectral indices of the electron energy distributions modified the
intensities and durations of the observed bursts. The strongest
gyrosynchrotron emission was observed as originating from the CME
flanks. Conclusions. Our results indicate that gyrosynchrotron emission
is the major component in type IV spectra, although additional
contributors cannot be ruled out.</description>
</item>
<item>
<title> Catalogue description and first statistical results</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...701A..20W</link>
<description>Context. The acceleration of particles at the Sun and their propagation
through interplanetary space are key topics in heliophysics.
Specifically, solar energetic electrons (SEEs) measured in situ can be
linked to solar events such as flares and coronal mass ejections (CMEs)
since they are also observed remotely in a broad range of
electromagnetic emissions such as in radio and X-rays. Solar Orbiter,
equipped with a wide range of remote-sensing and in situ detectors,
provides an excellent opportunity to investigate SEEs and their solar
origin from the inner heliosphere. Aims. We aim to record all SEE events
measured in situ by Solar Orbiter, and to identify and characterise
their potential solar counterparts. The results have been compiled in
the Comprehensive Solar Energetic Electron event Catalogue (CoSEE-Cat),
which will be updated regularly as the mission progresses. The catalogue
contains key parameters of the SEEs, as well as the associated flares,
CMEs, and radio bursts. In this paper, we describe the catalogue and
provide a first statistical analysis. Methods. The Energetic Particle
Detector (EPD) was used to identify and characterise SEE events, infer
the electron release time at the Sun, and determine the composition of
related energetic ions. Basic parameters of associated X-ray flares
(timing, intensity, source location) were provided by the
Spectrometer/Telescope for Imaging X-rays (STIX). This was complemented
by the Extreme Ultraviolet Imager (EUI), which added information on
eruptive phenomena. CME observations were contributed by the coronagraph
Metis and the Solar Orbiter Heliospheric Imager (SoloHI). Type III radio
bursts observed by the Radio and Plasma Waves (RPW) instrument provided
a link between the SEEs detected at Solar Orbiter and their potential
solar sources. The conditions in interplanetary space were characterised
using Solar Wind Analyzer (SWA) and Solar Orbiter Magnetometer (MAG)
measurements. Finally, data-driven modelling with the Magnetic
Connectivity Tool provided an independent estimate of the solar source
position of the SEEs. Results. The first data release of the catalogue
contains 303 SEE events observed in the period from November 2020 until
the end of December 2022. Based on the timing and magnetic connectivity
of their solar counterparts, we find a very clear distinction between
events with an impulsive ion composition and ones with a gradual one.
These results support the flare-related origin of impulsive events and
the association of gradual events with extended structures such as CME-
driven shocks or erupting flux ropes. We also show that the commonly
observed delays of the solar release times of the SEEs relative to the
associated X-ray flares and type III radio burst are at least partially
due to propagation effects and not exclusively due to an actual delayed
injection. This effect is cumulative with heliocentric distance and is
probably related to turbulence and cross-field transport.</description>
</item>
<item>
<title> The Role of Coronal Shock Waves</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..114W</link>
<description>We investigate the relationship between the gamma-ray emission measured
with the Large Area Telescope on board Fermi (Fermi-LAT9 and radio
signatures of coronal shock waves in four behind-the-limb (BTL) solar
flares. All events were associated with metric type II radio bursts.
Both start and end times of the radio bursts were synchronized with the
gamma-ray emission. The type II bursts associated with the BTL gamma-ray
flares had higher speeds and lower formation heights than those of an
average sample. These findings support the notion that the highly
relativistic ions that produce the gamma-rays in BTL flares are
accelerated at CME-driven propagating coronal shock waves rather than in
large-scale coronal loops.</description>
</item>
<item>
<title> A new type of fine spectral structure in the solar radio emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SCPMA..6809631K</link>
<description>Not Available</description>
</item>
<item>
<title> Solar Activity and Polar Ozone</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RuMH...50..683I</link>
<description>The paper presents the results of studying the influence of solar
activity on polar ozone in the Arctic and Antarctic. The polar ozone
satellite measurements in 19792024 presented on the NASA website (USA,
http://ozonewatch.gsfc.nasa.gov) and the corresponding characteristics
of solar activity, namely, the sunspot number and the magnitude of a
solar radio emission flux with a wavelength of 10.7 cm were used. An
analysis of the data showed that positive deviations of polar ozone
prevail under high solar activity. On average, under high solar
activity, polar ozone deviations from long-term means normalized to
standard deviations increase with the growth of solar activity. In
19792024, only positive polar ozone anomalies were observed in the
Arctic and Antarctic under high solar activity.</description>
</item>
<item>
<title> Heating Mechanisms and Radio Response from the Solar Chromosphere to Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RAA....25h5020T</link>
<description>Heating mechanism in the solar atmosphere (from chromosphere to corona)
is one of the top-challenges in modern astronomy. The classic mechanisms
can be divided into two categories: wave heating (W) and magnetic
reconnection heating (X). Both of them still face some problems
currently difficult to overcome. Recently, we proposed a new mechanism,
called magnetic-gradient pumping heating (MGP, or P) which seems to
overcome those difficulties, but still lacks sufficient observational
evidence. Which one really explained the physics of hot corona exactly?
How can observations be used to identify and verify the heating
mechanism? Since different heating mechanisms will generate non-thermal
particles from different accelerations and experience different
propagations, they will have different responses in the broadband
spectral radio observations. Among them, the non-thermal electrons from
W mechanisms are closely related to shock-wave acceleration, and their
radio response should be a group of spike bursts with random
distribution of drifting rates; the non-thermal electrons from X
mechanisms are accelerated by reconnecting electric field with
bidirectional flow, and their radio response should be type III pairs or
spike pairs; P mechanism will produce energetic particle upflows, and
their radio response should be unidirectional fiber bursts with moderate
negative drifting rates. Therefore, the heating mechanism can be
identified and verified from the broadband dynamic spectral radio
observations. Additionally, using high-resolution radioheliographs and
spectral-imaging observations, the heating mechanisms in different
regions can be identified and verified separately, thereby demonstrating
the physical essence of the hot corona.</description>
</item>
<item>
<title> Polarization Ratios of Turbulent Langmuir/Z-mode Waves Generated by Electron Beams in Magnetized Solar Wind Plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...989L..38P</link>
<description>The polarization ratios F = E&lt;SUB&gt;&lt;/SUB&gt;&lt;SUP&gt;2&lt;/SUP&gt;/E&lt;SUP&gt;2&lt;/SUP&gt;
of beam-generated turbulent Langmuir/Z-mode (LZ) waves and
electromagnetic emissions radiated at plasma frequency &lt;SUB&gt;p&lt;/SUB&gt;
from such sources are studied in weakly magnetized and randomly
inhomogeneous plasmas. Large-scale and long-term 2D/3V particle-in-cell
simulations with parameters relevant to type III solar radio bursts are
performed. Statistical studies using waveforms recorded by virtual
satellites are carried out to determine the distributions of
polarization ratios as a function of beam and plasma parameters. This
efficient method, which mimics waveform recording by spacecraft in the
solar wind, leads to results consistent with observations. Moreover,
plasma random density fluctuations n turn out to be the key factor
responsible for the increase in polarization ratios up to F  1. Indeed,
it is demonstrated that linear mode conversion at constant frequency
near &lt;SUB&gt;p&lt;/SUB&gt; of LZ waves scattering on n is the most efficient
and fastest process to produce large polarization ratios in randomly
inhomogeneous plasmas. This is due to electromagnetic slow extraordinary
Z-mode wave emission by LZ wave turbulence. The results provide guidance
to theoretical studies and useful support to estimate the average level
of density fluctuations in solar wind plasmas.</description>
</item>
<item>
<title> A Flare-related Decimetric Type-IV Radio Burst Induced by the X2 Radiation of Electron Cyclotron Maser Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...989L..24L</link>
<description>The radiation mechanism of decimetric wideband and pulsating radio
bursts from the Sun (in terms of decimetric type-IV (t-IVdm) burst) and
other flaring stars is a long-standing problem. Early investigations
were based on the leading-spot hypothesis for the Sun and yielded
contradictory results. Here, we analyzed the flare-associated t-IVdm
burst on 20110924 with medium-strong levels of polarization and from
sources near a sunspot. We found that the emission is intermittent and
the maximum T&lt;SUB&gt;B&lt;/SUB&gt; exceeds 10&lt;SUP&gt;11&lt;/SUP&gt; K, with well-defined
upper and lower frequency cutoffs. The radio sources are left-handed
polarized, located above the sunspot with a negative polarity. The
sources align well with the sites of the second harmonic of the local
electron gyrofrequency. These findings provide essential evidence that
the burst is induced by the electron cyclotron maser emission (ECME) in
the harmonic X mode. We further modeled the transport of downward-
streaming energetic electrons along a coronal loop and found that most
electrons get mirrored within the specific altitude range of 20100 Mm.
This explains why such bursts tend to have well-defined spectral ranges.
We also found the ECME-radiating energetic electrons exhibit a shell-
like velocity distribution function instead of the generally presumed
loss-cone distribution. The study greatly expands the application of
ECME in solar radio astronomy and provides solar samples for similar
bursts from other flaring stars.</description>
</item>
<item>
<title> Observations of Microwave Emission from Solar Jets and Comparison with Magnetohydrodynamic Simulations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...989..200A</link>
<description>We computed the thermal microwave emission from a 3D magnetohydrodynamic
(MHD) simulation and compared it with observations of solar jets. The
simulation treats the emergence of magnetic flux into the solar
atmosphere and its interaction with a low, preexisting ambient magnetic
field. This interaction leads to the formation and development of a jet,
driven by an eruption. The computed 17 GHz radio emission is compared
with a number of observed jets, with respect to their morphology, their
flux, and the rise time of the radio flux. We find that the MHD model
reproduces the characteristics of lower-intensity jets reasonably well,
whereas there are differences with stronger jets. We suggest possible
ways to obtain more realistic jets from MHD simulations, so that they
better match the real jets.</description>
</item>
<item>
<title> A Multispacecraft Analysis and Modeling of Type III Radio Burst Exciter Deceleration in Inhomogeneous Heliospheric Plasma</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...989..118A</link>
<description>Electron beams accelerated in solar flares and escaping from the Sun
along open magnetic field lines can trigger intense radio emissions
known as type III solar radio bursts. Utilizing observations by Parker
Solar Probe (PSP), STEREO-A, Solar Orbiter, and Wind spacecraft, the
speeds and accelerations of type III exciters are derived for simple and
isolated type III solar bursts. For the first time, simultaneous four
spacecraft observations allow us to determine positions and correct the
resulting velocities and accelerations for the location between the
spacecraft and the apparent source. We observe velocities and
acceleration to change as u(r)  r&lt;SUP&gt;0.37  0.14&lt;/SUP&gt; and a(r) 
r&lt;SUP&gt;1.71  0.20&lt;/SUP&gt; with radial distance from the Sun r. To explain
the electron beam deceleration, we develop a simple gas-dynamic
description of the electron beam moving through plasma with
monotonically decreasing density. The model predicts that the beam
velocity decreases as u(f)  f&lt;SUP&gt;1/4&lt;/SUP&gt;(r), so the acceleration
changes r&lt;SUP&gt;1.58&lt;/SUP&gt; (and speed as r&lt;SUP&gt;0.29&lt;/SUP&gt;) for the
plasma density profile n(r)  r&lt;SUP&gt;2.3&lt;/SUP&gt;. The deceleration is
consistent with the average observation values corrected for the type
III source locations. Intriguingly, the observations also show
differences in velocity and acceleration of the same type III observed
by different spacecraft. We suggest the difference could be related to
the additional time delay caused by radio-wave scattering between the
spacecraft and the source.</description>
</item>
<item>
<title> Challenging Established Paradigms</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...988L..73D</link>
<description>Polarimetric radio observations of the Sun can provide rich information
about emission mechanisms and the propagation medium. For the past five
decades, solar polarimetric studies at low radio frequencies have almost
always assumed the absence of linear polarization. This has been based
on the expectations from coronal propagation effects. Here we present
the first robust evidence of linear polarization from solar emissions at
meter wavelengths using simultaneous measurements with two telescopes of
very different designs separated by thousands of kilometersthe
Murchison Widefield Array and the upgraded Giant Metrewave Radio
Telescope. Both data sets show consistent linear polarization fractions,
confirming this detection. Rapid changes in morphology, as well as the
fractional linear polarization at small time and frequency spans,
further rule out any possibilities of an instrumental origin. Assuming
the absence of linear polarization in solar radio emissions can result
in incorrect interpretation of solar observations as well as those of
other flare stars, which are often guided by learnings from solar
studies. This discovery highlights the need for relaxing this assumption
and is essential for precise estimation of polarization signatures,
ultimately leading to a better understanding of the plasma conditions in
the Sun and other stars.</description>
</item>
<item>
<title> Energy Budget in the 2017 September 7 "Cold" Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...988..260F</link>
<description>A subclass of early impulsive solar flares, cold flares, was proposed to
represent a clean case, where the release of the free magnetic energy
(almost) entirely goes to the acceleration of the nonthermal electrons,
while the observed thermal response is entirely driven by the nonthermal
energy deposition to the ambient plasma. This paper studies one more
example of a cold flare, which was observed by a unique combination of
instruments. In particular, this is the first cold flare observed with
the Expanded Owens Valley Solar Array and, thus, for which the dynamical
measurement of the coronal magnetic field and other parameters at the
flare site is possible. With these new data, we quantified the coronal
magnetic field at the flare site but did not find statistically
significant variations of the magnetic field within the measurement
uncertainties. We estimated that the uncertainty in the corresponding
magnetic energy exceeds the thermal and nonthermal energies by an order
of magnitude; thus, there should be sufficient free energy to drive the
flare. We discovered a very prominent soft-hard-soft spectral evolution
of the microwave-producing nonthermal electrons. We computed energy
partitions and concluded that the nonthermal energy deposition is likely
sufficient to drive the flare thermal response similarly to other cold
flares.</description>
</item>
<item>
<title> I. The differential rotation profile</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...700L...3R</link>
<description>Context. Although the differential rotation rate on the solar surface
has long been studied using optical and extreme ultraviolet (EUV)
observations, associating these measurements with specific atmospheric
heights remains challenging due to the temperature-dependent emission of
tracers observed in EUV wavelengths. Radio observations, being primarily
influenced by coherent plasma processes and/or thermal bremsstrahlung,
offer a more height-stable diagnostic and thus provide an independent
means to test and validate rotational trends observed at other EUV
wavelengths. Aims. We aim to characterise the differential rotation
profile of the upper chromosphere using cleaned solar full-disc 17 GHz
radio imaging from the Nobeyama Radioheliograph spanning a little over
two solar cycles (19922020). Methods. A tracer-independent method based
on automated image correlation was employed on daily full-disc 17 GHz
radio maps. This method determines the angular velocities in 16
latitudinal bins of 15 each by maximising the 2D cross-correlation of
overlapping image segments. Results. The best-fit parameters for the
differential rotation profile are A = 14.520  0.006/day, B = 1.443 
0.099/day, and C =0.433  0.267/day. These results suggest that the
upper chromosphere rotates significantly faster than the photosphere at
all latitudes, with a relatively flatter latitudinal profile. We also
observed a very weak anti-correlation, &lt;SUB&gt;s&lt;/SUB&gt; = 0.383 (94.73%),
between the equatorial rotation rate and solar activity. Conclusions.
Our findings reaffirm the potential of radio observations to probe the
dynamics of the solar chromosphere with reduced height ambiguity. The
overlap of the equatorial rotation rate (A) found in this study with
that for 304  in the EUV regime lends additional support to the view
that the equatorial rotation rates increase with height above the
photosphere. Future coordinated studies at wavelengths with better-
constrained height formation will be crucial for further understanding
the complex dynamics of the solar atmosphere.</description>
</item>
<item>
<title> The source sizes of type II radio bursts with LOFAR</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...700A.274K</link>
<description>Context. Solar radio bursts can provide important insights into the
underlying physical mechanisms that drive the small and large-scale
eruptions on the Sun. Since metric radio observations can give us direct
observational access to the inner and middle corona, they are often used
as an important tool to monitor and understand the coronal dynamics.
Aims. While the sizes of the radio sources that can be observed in the
solar corona are essential for understanding the nature of density
turbulence within the solar corona and its subsequent influence on the
angular broadening observed in radio source measurements, the smallest
radio sources associated with solar radio bursts have so far been
limited by observational techniques and the radio instrument's
baselines. Methods. We selected three type II bursts that were observed
with the LOFAR core and remote stations in the Solar Cycle 24. We
estimated the sizes and shapes (ellipticity) of the radio sources from
20200 MHz using a two-dimensional (2D) Gaussian approximation. Results.
Our analysis shows that the smallest radio source size for type II
bursts in the solar corona that can be observed in the solar atmosphere
at low frequencies is 1.5'0.5' at 150 MHz. However, even though the
observations were taken with remote baselines (with a maximum distance
of 85 km), the effective baselines were much shorter (15 km), likely
due to snapshot imaging of the Sun. Conclusions. Our results show that
the radio source sizes are less affected by scattering than suggested in
previous studies. Our measurements indicate smaller source sizes at
frequencies below 95 MHz compared to previous reports, though some
overlap exists with measurements at higher frequencies when using
smaller baselines.</description>
</item>
<item>
<title> Observation and Modeling of Small Spatial Structures of Solar Radio Noise Storms Using the uGMRT</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..109M</link>
<description>One of the most commonly observed solar radio sources in the metric and
decametric wavelengths is the solar noise storm. These are generally
associated with active regions and are believed to be powered by the
plasma emission mechanism. Since plasma emission is emitted primarily at
the fundamental and harmonic of the local plasma frequency, it is
significantly affected by density inhomogeneities in the solar corona.
The source can become significantly scatter-broadened due to the multi-
path propagation caused by refraction from the density inhomogeneities.
Past observational and theoretical estimates suggest some minimum
observable source size in the solar corona. The details of this limit,
however, depend on the modeling approach and details of the coronal
turbulence model chosen. Hence pushing the minimum observable source
size to smaller values can help constrain the plasma environment of the
observed sources. In this work, we for the first time, use data from the
upgraded Giant Metrewave Radio Telescope in the 250  500 MHz band, to
determine multiple instances of very small-scale structures in the noise
storms. We also find that these structures are stable over timescales of
15  30 minutes. By comparing the past observations of type III radio
bursts and noise storms, we hypothesize that the primary reason behind
the detection of these small sources in noise storm is due to the local
environment of the noise storm. We also build an illustrative model and
propose some conditions under which the minimum observable source size
predicted by theoretical models, can be lowered significantly.</description>
</item>
<item>
<title> Multiple Sources of a Type II Radio Burst Within a Coronal Mass Ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300..108F</link>
<description>Solar type II radio bursts are generated through plasma emission caused
by energetic electrons that are accelerated by shock waves during solar
eruptions. These bursts serve as tracers of shock waves in the corona.
However, the complexity of solar eruptions and the lack of radio imaging
observations have hampered our understanding of type II bursts. The
newly built Daocheng Solar Radio Telescope (DSRT) detected a rare type
II burst. Its harmonic shows an initial herringbone (HB), followed by
three nearly parallel lanes. These lanes form a framed pattern: a
central main lane (termed MAIN) with a higher brightness temperature and
wider bandwidth, flanked by two well-defined fringes, F1 and F2. Radio
and extreme ultraviolet imaging observations indicate that the sources
of the HB are precisely located on the flank of the leading shock wave
driven by a coronal mass ejection (CME). In contrast, the MAIN and F2
sources correlate in terms of time, location, electron number density,
and propagation velocity with an ascending coronal loop. In contrast,
the F1 sources are associated with a nearby but distinct coronal loop.
These observations suggest that at least three sources of the type II
burst accompany the CME. A scenario involving multiple shock waves
within the CME is proposed to explain the presence of the different
radio sources.</description>
</item>
<item>
<title> Theoretical Considerations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...91B</link>
<description>The Sun is a powerful source of radio emissions, so much so that, unlike
most celestial sources, this emission can dominate the system noise of
radio telescopes. We outline the theory of noise in maps formed by
Fourier synthesis techniques at radio wavelengths, with a focus on self-
noise: that is, noise due to the source itself. As a means of developing
intuition we consider noise for the case of a single dish, a two-element
interferometer, and an n-element array for simple limiting cases. We
then turn to the question of the distribution of noise on a map of an
arbitrary source observed at radio wavelengths by an n-element
interferometric array. We consider the implications of self-noise for
observations of the Sun in a companion paper.</description>
</item>
<item>
<title> Solar Use Cases</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...90B</link>
<description>Noise in images of strong celestial sources at radio wavelengths using
Fourier synthesis arrays can be dominated by the source itself, so-
called self-noise. We outlined the theory of self-noise for strong
sources in a companion paper. Here we consider the case of noise in maps
of radio emission from the Sun which, as we show, is always dominated by
self noise. We consider several classes of science use cases for current
and planned arrays designed to observe the Sun in order to understand
limitations imposed by self-noise. We focus on instruments operating at
decimeter and centimeter wavelengths but the results are applicable to
other wavelength regimes.</description>
</item>
<item>
<title> A novel fine spectral structure of solar radio bursts with periodic beaded stripes observed by CBSm of CMP-II</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SCPMA..6809611L</link>
<description>A novel fine spectral structure in solar radio bursts has been
discovered using the Chashan broadband solar radio spectrometer at meter
wavelengths (CBSm), an instrument of the Chinese Meridian Project-Phase
II (CMP-II). The structure features periodic narrow-band stripes with a
typical recurrence time &lt; 1 s (occasionally reaching 8 s), often
drifting from high to low frequencies and accompanied by absorptions,
with trailing stripes appearing at the end of preceding ones. Some
stripes exhibit periodic beaded (or pearl-like) enhancements with a
periodicity of 0.1 s. The beaded stripes are reported for the first
time ever. Data from the DAocheng Radio Telescope (DART) indicate a
radio emission brightness temperature exceeding 10&lt;SUP&gt;9&lt;/SUP&gt; K,
originating above brightening loops in active region AR 13664. We
proposed a novel generation mechanism of the periodic stripes on the
basis of the double plasma resonance (DPR) instability, and explained
the beaded substructure in terms of modulation by low-frequency
magnetohydrodynamic (MHD) waves. The study highlights the CBSm's
capability to detect high-resolution fine spectral structures and offers
novel insights into the emission mechanism and source characteristics of
solar radio bursts.</description>
</item>
<item>
<title> Detecting Ionospheric Disturbances Using High Frequency Coastal Radar Transmissions From the West Coast of the United States</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RaSc...6008235T</link>
<description>Coastal radar system are located around the world and many happen to
transmit at frequencies capable of skywave propagation via the
ionosphere. Therefore, they can be detected hundreds to thousands of
kilometers away. This paper demonstrates the opportunity to detect 39
Coastal Ocean Dynamics Application Radar transmitters located on the
western coast of the United States using three HF radio receivers in
Utah and New Mexico. It also illustrates the possibility to use the
phase and Doppler measurements of these signals to derive displacements
of the refracting ionospheric layer up to meter resolution for the 2023
annular solar eclipse, an M-class solar flare, and a Falcon 9 second
stage reentry. This study demonstrates the feasibility and usefulness of
coastal radar systems to make ionospheric measurements and conduct
research.</description>
</item>
<item>
<title> Noise Reduction Method for Radio Astronomy Single Station Observation Based on Wavelet Transform and Mathematical Morphology</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RAA....25g5014Q</link>
<description>The 21 cm radiation of neutral hydrogen provides crucial information for
studying the early universe and its evolution. To advance this research,
countries have made significant investments in constructing large low-
frequency radio telescope arrays, such as the Low Frequency Array and
the Square Kilometre Array Phase 1 Low Frequency. These instruments are
pivotal for radio astronomy research. However, challenges such as
ionospheric plasma interference, ambient radio noise, and instrument-
related effects have become increasingly prominent, posing major
obstacles in cosmology research. To address these issues, this paper
proposes an efficient signal processing method that combines wavelet
transform and mathematical morphology. The method involves the following
steps: Background Subtraction: Background interference in radio
observation signals is eliminated. Wavelet Transform: The signal, after
removing background noise, undergoes a two-dimensional discrete wavelet
transform. Threshold processing is then applied to the wavelet
coefficients to effectively remove interference components. Wavelet
Inversion: The processed signal is reconstructed using wavelet
inversion. Mathematical Morphology: The reconstructed signal is further
optimized using mathematical morphology to refine the results.
Experimental verification was conducted using solar observation data
from the Xinjiang Observatory and the Yunnan Observatory. The results
demonstrate that this method successfully removes interference signals
while preserving useful signals, thus improving the accuracy of radio
astronomy observations and reducing the impact of radio frequency
interference.</description>
</item>
<item>
<title> Confined vs. eruptive M-class flares in solar cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2025BlgAJ..43...34M</link>
<description>This report presents a quantitative comparison between confined,
eruptive and all (2177) M-class solar flares (SFs) over the last two
solar cycles (SC) and separately in SC 23 and 24. The properties of the
SFs, related radio bursts and the parent sunspots (Hale type and total
area) are examined. The differences are presented and discussed in the
framework of space weather.</description>
</item>
<item>
<title> A 5055 GHz Millimeter-wave Radiometer Spectrometer for Solar Flare Detection</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..279...29X</link>
<description>During solar flare eruptions, millimeter-wave radiation is emitted,
which is highly efficient and sensitive to high-energy electrons,
allowing for the extraction of unique magnetic field information.
Therefore, we have developed a 5055 GHz solar millimeter-wave
radiometer system. The system employs a 50 cm diameter Cassegrain
antenna to receive circularly polarized solar radiation signals. These
signals enter the analog front-end system, where they undergo power
division, filtering, and detection operations, resulting in voltage
signals. Subsequently, the signals are processed by the digital receiver
for analog-to-digital conversion and smoothing and are finally
transmitted to the host computer via the RS422 protocol to display the
intensity of solar radiation. The system's performance metrics are as
follows: a noise figure of &lt;2.5 dB, system linearity 0.9999, a time
resolution range of 0.0011 s, and a dynamic range exceeding 30 dB. The
system began routine observations in 2024 October and successfully
captured the world's first 50 GHz band solar flare data in December.
Currently, the system is effectively observing during the 25th solar
activity maximum period, which is expected to provide valuable data for
solar physics research.</description>
</item>
<item>
<title> Deep Active LearningBased Classification of Solar Radio Spectrogram Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..279...25L</link>
<description>The study of solar burst activity can provide early warnings for the
environmental protection of the solarterrestrial space environment.
With the improvement of solar radio observation techniques, observation
devices have generated enormous amounts of observation data. To solve
the shortcomings of time-consuming and error-prone manual recognition,
researchers have begun to use deep learning to recognize and
automatically classify solar radio outbursts. Deep learning will depend
on a large number of labeled samples; however, the labeling of samples
requires a lot of time and manual labor. This leads to low efficiency.
In addition, the labeled samples are not all valuable samples, so it is
necessary to improve the effectiveness of the labeled samples and select
the high-value samples. The occurrence of active-learning techniques
provides an opportunity to solve this problem. In this study, we
developed a progressive deep convolutional generative adversarial
network model. Then, we combined it with deep active learning to
complete the automatic classification of solar radio spectrum data. We
used solar radio spectrum data from the Chashan Observatory (CSO) of
Shandong University and Learmonth Observatory in Australia. The results
show that the method proposed in this paper can achieve high accuracy in
the automatic recognition of solar radio spectrum data and solve the
time-consuming problem of labeling a huge number of data samples.
Finally, we applied the results to the CSO and realized the automatic
recognition of solar radio spectral data.</description>
</item>
<item>
<title> Research on High-precision Fiber Transmission and Compensation for a Solar Radio Heliograph</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..279....4Z</link>
<description>Solar radio bursts are a major source of space weather hazards. Thus,
developing solar observation systems is essential. The heliograph, based
on synthetic aperture imaging and a dual interferometer, enables high-
resolution solar imaging, offering rich spatial information beyond
conventional radio spectrometers. The performance of a synthetic
aperture heliograph depends critically on time-frequency synchronization
among multiple antennas. On this basis, we have conducted research on
fiber time-frequency synchronization. The research allows the long-
distance transmission and synchronization of signals generated by the
rubidium atomic clock via optical fiber. Analysis and testing
demonstrated that the research achieved frequency stability of 7 
10&lt;SUP&gt;13&lt;/SUP&gt;/1 s and an accuracy of 0.466 ppm. After compensation,
the average time difference achieved 4.6 and 5.4 ps for frequency and
time standard signal, respectively. These results not only indicate that
our scheme meets the requirements of the synthetic aperture heliograph
but also demonstrate good applicability and scalability, providing a
solid foundation for the future development of solar observation
systems.</description>
</item>
<item>
<title> Highly Polarized Type III Storm Observed with Parker Solar Probe</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...987L..34P</link>
<description>The Parker Solar Probe (PSP) spacecraft observed a large coronal mass
ejection (CME) on 2022 September 5, shortly before closest approach
during the 13th PSP solar encounter. For several days following the CME,
PSP detected a storm of Type III radio bursts. Stokes parameter analysis
of the radio emission indicates that the Type III storm was highly
circularly polarized (with fractional polarization up to 0.4). Left-
hand circularly polarized (LHC) emission dominated at the start of the
storm, transitioning to right-hand circularly polarized (RHC) emission
at the crossing of the heliospheric current sheet on September 6. We
analyze the properties of this Type III storm. The drift rate of the
Type IIIs indicates a constant beam speed of 0.1c, typical for Type
III-producing electron beams. The sense of polarization is consistent
with fundamental emission generated primarily in the O-mode. The stable
and well organized post-CME magnetic field neatly separates the LHC- and
RHC-dominated intervals of the storm, with minimal overlap between the
senses of polarization. The proximity of PSP to the source region, both
in radial distance and in heliographic longitude, makes this event an
ideal case study to connect in situ plasma measurements with remote
observations of radio emission.</description>
</item>
<item>
<title> Small-scale Inhomogeneity Effects on Coherent Solar Radio Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...987...84Z</link>
<description>The coherent radio emission mechanism of solar radio bursts (SRBs) is
one of the most complicated and controversial topics in solar physics.
To clarify the mechanism(s) of different types of SRBs, (radio-) wave
excitation by energetic electrons in homogeneous plasmas has been widely
studied via particle-in-cell (PIC) code numerical simulations. The solar
corona is, however, inhomogeneous over almost all spatial scales. Due to
the kinetic nature of SRBs, small-scale inhomogeneities in the plasma
could influence the excitation and emission properties of SRBs. In this
paper, we thus investigate the effects of small-scale inhomogeneity (in
the magnetic field as well as plasma density or temperature) of plasmas
in the solar corona on radio-wave emission by ring-beam distributed
energetic electrons utilizing 2.5-dimensional PIC simulations. The
typical length scale of the small-scale inhomogeneity we consider in
this study is on the order of the proton gyroradius. Both beam and
electron-cyclotron maser instabilities can be triggered with the
presence of energetic ring-beam electrons. The resultant spectrum of the
excited electromagnetic waves presents a zebra-stripe pattern in the
frequency space. The inhomogeneous density or temperature in plasmas
influences the frequency bandwidth and location of these excited waves.
Our results can hence help to diagnose the plasma properties at the
emission sites of SRBs. Applications of our results to SRBs with a
zebra-stripe pattern are discussed.</description>
</item>
<item>
<title> Solar energetic electron events with a spectral bump break</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...699A...2L</link>
<description>Aims. We present ten solar energetic electron (SEE) events measured by
Wind/3DP at 1 to 200 keV with a bump break in the electron peak flux
versus energy spectrum. We examined their acceleration sources and/or
processes at the Sun. Methods. We assumed that these bump SEE events
consist of two electron populations: a primary population (described by
the pan-spectrum (PS) function), and a bump population (described by the
Gaussian function), which dominate at low and high energies,
respectively. We constructed two formulae to fit the SEE energy spectrum
by multiplying a PS function with a natural exponential form of the
Gaussian function (i.e., the MUL formula) and by adding a PS function
with a Gaussian function (i.e., the ADD formula). Results. The fitting
results suggest that the MUL fitting can reflect the physical nature in
the formation of these bump events. For the primary electron population,
the MUL fitting obtains an upward-bending double power-law spectrum for
event 10 with a spectral index of 3.58 (1.74) at energies below (above)
4.6 keV, and a single power-law spectrum for the other nine events with
a median spectral index of 2.52&lt;SUP&gt;+0.29&lt;/SUP&gt;&lt;SUB&gt;0.25&lt;/SUB&gt;. For the
bump electron population, the fitted center energy has a median value of
59.1&lt;SUB&gt;3.2&lt;/SUB&gt;&lt;SUP&gt;+18.1&lt;/SUP&gt; keV. For the events associated with
soft X-ray flares (west limb coronal mass ejections), the flare class
(angular width of the coronal mass ejection) is positively correlated
with the estimated electron number of the power-law population
N&lt;SUB&gt;pl&lt;/SUB&gt; and of the bump population N&lt;SUB&gt;bp&lt;/SUB&gt; (the number
ratio N&lt;SUB&gt;bp&lt;/SUB&gt;/N&lt;SUB&gt;pl&lt;/SUB&gt; at 10400 keV). Conclusions. These
results indicate that for these bump SEE events, the power-law electron
population can be produced by some flare-related processes that occur
high in the corona, while the bump population can be accelerated by some
processes related to coronal mass ejections that act on the power-law
population. The bump-like spectrum might also be the intermediate
spectrum during the evolution from single power-law to downward-bending
double power-law.</description>
</item>
<item>
<title> Comparison of Observed and Predicted Electron Density Profiles From 15 to 26 April 2001</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033197W</link>
<description>Solar flares significantly affect Mars's ionosphere, yet there are few
comparisons between observed and simulated densities in the M1 and M2
ionospheric layers during solar flares. Here we compare observed and
simulated electron density profiles for the X14.4 solar flare of 15
April 2001 and the M7.8 solar flare of 26 April 2001. We use
observations from Mars Global Surveyor radio occultations and
simulations from the Mars Global Ionosphere-Thermosphere Model (M-GITM).
Due to poor constraints on the solar spectrum incident upon Mars at this
time, simulated M2 electron density values were 50% larger than
observed. Yet the relative changes in M2 electron density during these
two flares were reproduced to 10% accuracy. When accurate solar
irradiance data are available, absolute M2 electron density values are
simulated accurately. Due to the omission of electron impact ionization
from the M-GITM model, the simulated M1/M2 density ratio was under-
predicted by a factor of approximately 3. Yet the relative changes in M1
electron density during these two flares were reproduced to 20%
accuracy. The model can accurately predict relative changes in M1 and M2
electron densities during a solar flare. If accurate solar irradiance
data are available, it can accurately predict absolute changes in M2
electron densities. If a simple parameterization of electron impact
ionization were incorporated into the model, then it would likely
predict absolute changes in M1 electron densities accurately as well.
The M-GITM model is well-suited to studies of time-varying phenomena in
the ionosphere of Mars.</description>
</item>
<item>
<title> Monitoring Solar Radio Bursts With an Expansive Array of Antennae at High Schools Nationwide</title>
<link>https://ui.adsabs.harvard.edu/abs/2025E&amp;SS...1204114A</link>
<description>The Sun Radio Interferometer Space Experiment (SunRISE) Ground Radio Lab
(GRL) is a Science, Technology, Engineering, Arts, and Mathematics
(STEAM) project, sponsored by NASA's SunRISE mission and organized by
the University of Michigan College of Engineering. The project aims to
engage and train the next generations of scholars. To achieve this, the
project deployed antennas to 18 high schools nationwide to observe solar
radio bursts (SRB). SRBs are defined as low-frequency radio emissions
emanated by accelerated electrons associated with extreme solar
activity, including solar flares and coronal mass ejections (CMEs). Type
II SRBs were found to predominantly correspond to coronal shocks caused
by CMEs, highlighting particle acceleration events in the solar
atmosphere and interplanetary space. These bursts can act as early
warning signs of upcoming solar disturbances which can lead to
geomagnetic storms. The type II bursts were then investigated to
estimate the corresponding shock and Alfvn speeds: 277 &lt;
v&lt;SUB&gt;shock&lt;/SUB&gt; &lt; 1,480 km/s and 194 &lt; v&lt;SUB&gt;A&lt;/SUB&gt; &lt; 947 km/s at
heliocentric distances of around 12 solar radii, respectively. The
Alfvn Mach number was further found to be 1.2 &lt; M&lt;SUB&gt;A&lt;/SUB&gt; &lt; 2,
while the measured magnetic field strength followed a single power law
of B(r) = 0.3 r&lt;SUP&gt;2&lt;/SUP&gt;, where r represents the heliocentric
distance. Our results were found to agree with previous studies. Through
SunRISE GRL, an ever-expanding catalog of SRBs is being collected by
high school students nationwide, curated by a team of solar physics
experts, and made publicly available to the scientific community to make
progress toward the SunRISE mission's objectives.</description>
</item>
<item>
<title> Statistics of Coronal Mass Ejections in Solar Flares with Helioseismic Response</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AstBu..80..294S</link>
<description>This paper presents the results of a statistical analysis of the
properties of coronal mass ejections (CMEs) associated with solar flares
that exhibit a helioseismic response (''sunquakes'') in comparison with
flares that do not show photospheric disturbances. The analysis is based
on observations of the solar corona in the ultraviolet range (from the
Atmospheric Imaging Assembly on board the Solar Dynamics Observatory,
SDO/AIA) and the visible range (from the Large Angle Spectroscopic
Coronagraph on board the Solar and Heliospheric Observatory,
SOHO/LASCO). We considered samples of flares with different lower
thresholds based on the Geostationary Operational Environmental
Satellites (GOES) classification: above M1.0, M5.0, and M7.0. A
correlation analysis was also carried out between CME parameters and the
total energy of the sunquakes. Additionally, for flares above
M7.0-class, information on the presence of radio bursts across a wide
range of wavelengths, as well as hard X-ray emission, was analyzed. It
was found that CMEs accompanying flares with a helioseismic response
tend to have higher velocities in the lower corona (according to AIA
data) compared to flares without photospheric disturbances. The
distribution of CME masses is approximately the same regardless of the
presence or absence of sunquakes during the flares. An analysis of
dimming properties showed that they are more impulsive in terms of
temporal dynamics in flares with sunquakes. CMEs in flares above
M7.0-class that exhibit helioseismic responses are less massive and
slower in the outer corona according to LASCO data. The correlation
analysis did not reveal strong relationships between acoustic energy and
CME parameters based on AIA observations, but for several parameters
(kinetic energy, CME mass, and dimming depth), statistically significant
correlations were identified according to the -criterion. In contrast to
flares with sunquakes, there was an almost complete absence of type III
radio bursts and a rare occurrence of type II bursts in the M7.0-class
flares without photospheric disturbances. The spectral peak of microwave
bursts tends to occur at higher frequencies in flares with sunquakes
than in those without. According to our analysis, flares with sunquakes
likely possess the ability to efficiently generate fast coronal dimmings
and shock waves, even in the presence of poorly developed CMEs in the
upper corona (in comparison to flares without photospheric
disturbances). These events are also characterized by pronounced
signatures of electron acceleration, with particles escaping the
acceleration region both toward the solar surface and outward from it.
In our view, this indicates that the possibility of an eruptive origin
for sunquakes cannot be ruled out. Accelerated electrons may act as both
the primary and secondary agents responsible for initiating the
photospheric perturbation.</description>
</item>
<item>
<title> Polarization Analysis of Type III Langmuir/Z-mode Waves with Coherent Magnetic Component Observations by Solar Orbiter</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...985L..29F</link>
<description>Observations from the Solar Orbiter spacecraft provide unique insights
into the interaction between electron beams and the plasma background in
the source regions of type III radio emissions. We analyze this
interaction by examining the high-frequency electric and magnetic
components of in situ wave measurements, focusing on their polarization
properties. Using electron data from onboard instruments, we model the
electron velocity distribution function and numerically solve the
dispersion relation. We compare the predicted polarization of the
electric and magnetic components with the observations. Our findings are
consistent with propagation in the Langmuir/Z-mode at an oblique
wavevector. We explain the magnetic component and transverse
polarization by the presence of small density fluctuations, without the
need for mode conversion.</description>
</item>
<item>
<title> First Detection of Low-frequency Striae in Interplanetary Type III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...985L..27K</link>
<description>We report the first detection of type III solar radio burst striae in
the 3080 kHz range, observed by the Cluster-4 spacecraft during an
exceptionally quiet solar period. These low-frequency fine structures,
which drift slowly in frequency and exhibit narrow bandwidths, provide a
novel diagnostic of plasma processes in the inner heliosphere. The
detected striae, interpreted as fundamental plasma emission, exhibit a
frequency drift rate of 0.328 Hz s&lt;SUP&gt;1&lt;/SUP&gt; and a bandwidth of 1.3
kHz. By combining high-resolution radio observations with well-
calibrated in situ electron velocity distribution function data from the
Wind spacecraft, we characterized the plasma properties of the burst
source region near 0.32 au. Our analysis estimates relative density
fluctuations, at the effective turbulence scale length, as approximately
3.4% (inferred from striae bandwidths), 0.62% (from intensity
fluctuations), and 3.5% (from a heliocentric distance-based empirical
model). These findings offer critical insights into small-scale density
inhomogeneities and turbulence that affect electron beam propagation.
This study underscores the potential of combining well-calibrated in
situ electron data with radio burst measurements to probe the physical
conditions of the solar wind and to refine our understanding of solar
radio bursts across a broad frequency range.</description>
</item>
<item>
<title> High-resolution Observational Features of Type I Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...985..257Y</link>
<description>In this paper, we statistically studied the characteristic features of
solar radio Type I bursts observed by Chashan broadband solar radio
spectrometer at meter wavelengths from 00:06 to 07:28 UT on 2023
December 13. Based on the image morphology, we develop a method to
identify individual Type I bursts on the dynamic spectra from a
connected region with a ratio of the duration to bandwidth less than or
equal to 3.8 and the area sum (total pixels) greater than 4. In total,
102,073 and 78,773 bursts are detected on right-hand circular
polarization and left-hand circular polarization components,
respectively. We find Type I bursts with a mean lifetime of 0.7 s, a
mean bandwidth of 5.6 MHz, and a relative bandwidth f/f&lt;SUB&gt;0&lt;/SUB&gt; of
about 2%3%. Consistent with the previous findings of hard X-ray pulses,
microwave pulses, Type III bursts, and decimetric spikes, Type I bursts
exhibit their duration, bandwidth, peak intensity, and area sum with a
power-law distribution. From the linear fitting in loglog space, we
obtain the slope index between 1 and 3.5 for various parameters.
Meanwhile, Type I bursts display the mean polarization degree in the
range from 22% to 33%, and different bursts have various degrees. We
find that Type I bursts tend to appear as a chain, and the short periods
of 0.92 and 1.22 s are detected in two burst chains. Our finding would
be an observational constraint for the emission mechanism and physical
model of solar Type I radio bursts.</description>
</item>
<item>
<title> Imaging and spectropolarimetric observations of a band-split type II solar radio burst with LOFAR</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...698A.175N</link>
<description>Context. Type II solar radio bursts are generated by electrons
accelerated by coronal shock waves. They appear in dynamic spectra as
lanes drifting from higher to lower frequencies at the plasma frequency
and its harmonic. These lanes can often be split into two or more sub-
bands that have similar drift rates. This phenomenon is called band-
splitting, and its physical origins are still under debate. Aims. Our
aim is to investigate the origin of band-splitting using novel imaging
and spectropolarimetric observations of a type II solar radio burst from
the Low Frequency Array (LOFAR). Methods. We used LOFAR imaging at
multiple frequencies and time steps to track the locations of the radio
sources corresponding to the two components of the band-split emission
lane. In addition, we estimated the degree of circular polarisation
(dcp) for both components using LOFAR's full Stokes dynamic spectra.
Results. From the imaging of the type II burst, we found two close but
clearly separated emission regions clustered over several frequencies
spanning each split band. One emission region corresponds to the lower
frequency band and the other to the higher frequency band of the split
lane. Using the full Stokes dynamic spectra, we also found the dcp to be
very similar for both bands. Conclusions. The two distinct emission
regions suggest that the split bands originate from two separate regions
at the shock. The similar values of dcp for both sub-bands correspond to
similar values of magnetic field strength in the two regions and
indicate little to no change in the emission region plasma. Thus, our
findings are in contradiction with previous theories, which have
suggested that split bands originate in the same region but upstream and
downstream of the shock. Instead, our results suggest that both bands
originate in two separate upstream regions since we find a clear
separation in locations and no magnetic compression.</description>
</item>
<item>
<title> Studying the Inner Heliosphere Using Radio Signals Transmitted From Spacecraft Orbiting Mars</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SpWea..2304225E</link>
<description>In this campaign, we used very long baseline interferometry (VLBI) radio
telescopes to track the carrier radio signal transmitted from spacecraft
orbiting Mars during the Mars solar conjunction. The campaign extended
from September $6\text{th}$ to November $6\text{th}$ 2021 and targeted
the Mars Express (MEX) and Tianwen-1 (TIW) spacecraft. The aim was to
study the structure of the solar corona within 40 solar radii using the
radio sounding technique developed by the Planetary Radio and Doppler
Experiment (PRIDE). Previous work by the group has studied the effect of
the solar wind and interplanetary scintillation on spacecraft signals at
a large range of solar elongations. Here, we apply the same methodology
to characterize the inner regions of the solar wind and attempt to
capture the formation of transient solar phenomena such as solar flares
or coronal mass ejections (CMEs). We found that the phase scintillation
measurements fit the expected model of the electron content for the
line-of-sight very close to the Sun. Experimental outliers, where the
scintillation results deviated significantly from the expected electron
content model, were compared with ancillary data from the LASCO C2 and
C3 coronagraph instruments and found to correspond directly to solar
transient events.</description>
</item>
<item>
<title> Robust Statistical Techniques for Operational Maintenance of the 10.7 cm Solar Radio Flux</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SpWea..2304060B</link>
<description>The F10.7 solar radio flux is a critical quantity for operational space
weather nowcasting and forecasting, where it is routinely used as a
driver for coupled atmospheric models to estimate a variety of important
quantities such as the neutral atmospheric density. Although there have
been several successful developments in the way of parametric modeling
to ensure F10.7 coverage during outages (often using the sunspot number
or radio flux observations at neighboring wavelengths), these
developments have refrained from employing comprehensive cross-
validation schemes to ensure model generalizability, and can benefit
from recently-developed techniques for modeling nonlinear phenomena. We
present an approach that uses Feature Ordering by Conditional
Independence (FOCI) to identify favorable surrogates for the F10.7 index
and combines this with modeling of F10.7 with linear models and
Generalized Additive Models (GAMs). We find that this approach offers
notable improvements in reconstructing F10.7 over gaps of various
lengths, with GAMs yielding mean error of ${\sim} $2.8%, compared to
polynomial methods that yield mean errors of ${\sim} 3.1$%. We
additionally demonstrate the effect of reconstruction error on neutral
densities modeled by the NRLMSISE2.0 thermosphere model.</description>
</item>
<item>
<title> The High-Energy Protons of the Ground Level Enhancement (GLE74) Event on 11 May 2024</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...73P</link>
<description>High energy solar protons were observed by particle detectors aboard
spacecraft in near-Earth orbit on May 11, 2024 and produced the
74&lt;SUP&gt;th&lt;/SUP&gt; ground level enhancement (GLE74) event registered by
ground-based neutron monitors. This study involves a detailed
reconstruction of the neutron monitor response, along with the
identification of the solar eruption responsible for the emission of the
primary particles, utilizing both in situ and remote-sensing.
Observations spanning proton energies from a few MeV to around 1.64 GeV,
collected from the Solar and Heliospheric Observatory (SOHO), the
Geostationary Operational Environmental Satellite (GOES), the Solar
Terrestrial Relations Observatory (STEREO-A), and neutron monitors, were
integrated with records of the associated solar soft X-ray flare,
coronal mass ejection, and radio bursts, to identify the solar origin of
the GLE74. Additionally, a time-shift analysis was conducted to link the
detected particles to their solar sources. Finally, a comparison of
GLE74 to previous ones is carried out. GLE74 reached a maximum particle
rigidity of at least 2.4 GV and was associated with a series of type
III, type II, and type IV radio bursts. The release time of the primary
solar energetic particles (SEPs) with an energy of 500 MeV was estimated
to be around 01:21 UT. A significant SEP flux was observed from the
anti-Sun direction with a relatively broad angular distribution, rather
than a narrow, beam-like pattern, particularly during the main phase at
the particle peak flux. Comparisons with previous GLEs suggest that
GLE74 was a typical event in terms of solar eruption dynamics.</description>
</item>
<item>
<title> Extended Scenarios for Solar Radio Emissions With Downshifted Electron Beam Plasma Excitations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033597L</link>
<description>First-principle studies of radiative processes aimed at explaining the
origin of type II and type III solar radio bursts raise questions on the
implications of downshifted electron beam plasma excitations with
frequency (slightly) below the plasma frequency $\left(\omega \lesssim
{\omega }_{pe}\right)$ in the generation of radio emissions. Unlike the
beam-induced Langmuir waves $\left(\omega rsim {\omega }_{pe}\right)$ in
the standard radio emission plasma model, the primary wave excitations
of cooler and/or denser beams have predominantly downshifted
frequencies. Broadbands of such downshifted excitations are also
confirmed by in situ observations in association with terrestrial
foreshock and electron beams (in contrast to narrowband Langmuir waves),
but their involvement in radiative processes has not been examined so
far. We revisit three radiative scenarios specific to downshifted
primary excitations, and the results demonstrate their direct or
indirect involvement in plasma radio emission. Downshifted excitations
of an electron beam primarily play an indirect role, contributing to the
relaxation to a plateau-on-tail still able to induce Langmuir beam waves
that satisfy conditions for nonlinear wave-wave interactions leading to
free radio waves. At longer time scales, the primary excitations can
become predominantly downshifted, and then directly couple with the
secondary (backscattered) Langmuir waves to generate the second harmonic
of radio emissions. Two counter beams are more efficient and lead to
faster radiative mechanisms, involving counterpropagating downshifted
excitations, which couple to each other and generate intense, broadband
and isotropic radio spectra of downshifted second harmonics. Such a
long-lasting (second) radio harmonic can thus be invoked to distinguish
regimes with downshifted $\left(\omega \lesssim {\omega }_{pe}\right)$
primary excitations.</description>
</item>
<item>
<title> Ionospheric and Thermospheric Response to the 13 June 2022 M-Class Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033526S</link>
<description>On 13 June 2022, an M3-class solar flare erupted at 03:00 UT that lasted
nearly eight hours, causing increased ionization and shortwave radio
blackouts. Here, we combine measurements made by the NASA Ionospheric
Connections Explorer (ICON) mission to assess the evolution of the
ionosphere-thermosphere system in response to this flare. We find that
increased solar extreme ultraviolet (EUV) radiation during the flare did
increase O&lt;SUP&gt;+&lt;/SUP&gt; plasma in the region that was directly exposed to
the flare, but this effect was moderated by thermospheric perturbations
as evidenced by a decrease in column O/N&lt;SUB&gt;2&lt;/SUB&gt; (O/N&lt;SUB&gt;2&lt;/SUB&gt;)
that accompanied the sequence of events. Larger increases in
O&lt;SUP&gt;+&lt;/SUP&gt; were seen in the same region the day after the flare as
the non-impulsive, long-term solar EUV irradiance continued to increase
and the thermospheric O/N&lt;SUB&gt;2&lt;/SUB&gt; recovered. When energetic
particles arrived 3 days after the event, the ionospheric impact was
delayed by about a day compared to the thermospheric changes. Changes in
O/N&lt;SUB&gt;2&lt;/SUB&gt; inferred from far ultraviolet airglow are also strongly
correlated with relative changes in atomic oxygen independently
determined by simultaneous ICON measurements of EUV airglow. These
results demonstrate the magnitude, duration, and complexity of change
that even moderate M-class flares can generate in the ionosphere and
thermosphere.</description>
</item>
<item>
<title> Case study of the African low and mid-latitude regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JASTP.27006477U</link>
<description>We simultaneously evaluate the contributions of the mostly used solar
activity indices to the modelling of geomagnetic storms using principal
component analysis (PCA). The selected indices are the sunspot number
(SSN), solar radio flux at a wavelength of 10.7 cm (&lt;mml:math&gt;&lt;mml:mrow&gt;
&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn
&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;), 12-month running average of SSN (&lt;mml:math&gt;&lt;mm
l:mrow&gt;&lt;mml:mi&gt;R&lt;/mml:mi&gt;&lt;mml:mn&gt;12&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;),
81-day running average of &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;
10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; (&lt;
mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:m
o&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;81&lt;
/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;), and the modified 
&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:
mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; index herein referred to as 
&lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:
mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;mml:mi&gt;p&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;. The
assessment of these indices was accomplished by first developing five
storm-time empirical models of the ionosphere with ionospheric total
electron content (TEC) as dependent variable, and each of the five solar
proxies as the independent variable. As the energy from the Sun differs
from one latitudinal region to another on Earth, two locations at
different latitudes were considered for the analysis. Based on their
long data coverage periods, Hartebeesthoek (HRAO, geographic
coordinates: 25.89 S, 27.69 E; geomagnetic coordinates: 36.32 S,
94.69 E), South Africa; and Mbarara (MBAR, geographic coordinates: &lt;mml
:math&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;0&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;60&lt;/mml:mn&gt;&lt;
mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; S and &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:m
n&gt;30&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;74&lt;/mml:mn&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mm
l:mrow&gt;&lt;/mml:math&gt; E, geomagnetic coordinates: &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:
mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;22&lt;/mml:mn&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/m
ml:mrow&gt;&lt;/mml:math&gt; S and &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;102&lt;/mml:mn&gt;&lt;mml:m
o&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;36&lt;/mml:mn&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;
E), Uganda, were chosen to represent the middle and low latitude
ionospheric regions, respectively. Their data coverage periods are 27
September 1996 to 30 March 2024 (HRAO) and 17 July 2001 to 30 March 2024
(MBAR) and only storm-time TEC data within these periods selected based
on the criterion &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;D&lt;/mml:mi&gt;&lt;mml:mi&gt;s&lt;/mml:mi
&gt;&lt;mml:mi&gt;t&lt;/mml:mi&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:mn&gt;50&lt;/mml:m
n&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; nT or &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;
mml:mi&gt;K&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;p&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml
:msub&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;mml:mn&gt;4&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; were
considered for the statistical analysis. Through PCA decomposition, TEC
data were broken up into a matrix of principal directions of the maximum
variances in the dataset (or matrix of eigenvectors of the covariance
matrix) and a matrix of principal components (PCs) which represent the
projection of data onto the principal directions. For each model, PCs
were thereafter modelled in terms of the corresponding solar activity
index and the modelled quantities were further combined with the
original PC vectors to get the reconstructed TEC for the entire period
of the study. With reference to the ionospheric storm-time model
implemented using SSN as solar activity representation, a statistical
analysis revealed that, overall, the storm-time empirical models
developed using either &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;
/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, &lt;mml
:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;
mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;81&lt;/mm
l:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;
mml:mi&gt;R&lt;/mml:mi&gt;&lt;mml:mn&gt;12&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, or &lt;mml:math
&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:m
n&gt;7&lt;/mml:mn&gt;&lt;mml:mi&gt;p&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, perform about 8%,
15%, 18%, 22%, respectively, better in reconstructing actual TEC than
the SSN based model for HRAO, and 11%, 23%, 19%, 24% for MBAR.
Validating the models over selected four storms, results showed that
running average based indices led to more accurate TEC predictions
compared to the usual daily Wolf's SSN and &lt;mml:math&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F
&lt;/mml:mi&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;mml:mo&gt;.&lt;/mml:mo&gt;&lt;mml:mn&gt;7&lt;/mml:mn&gt;&lt;/mml:mr
ow&gt;&lt;/mml:math&gt;.</description>
</item>
<item>
<title> Solar Radio Burst Detection Based on Deformable DETR</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..278....4W</link>
<description>Solar radio burst (SRB) detection is crucial for solar physics research
and space weather forecasting. The main challenges faced are noise
interference in the spectrum and the diversity of SRBs. However, most
research focuses on classifying whether SRBs exist or detecting a single
type of SRB. Existing detection models exhibit deficiencies in the
accuracy of SRB detection. Moreover, existing detection models cannot
effectively handle background noise interference in solar radio
spectrograms and the significant scale variations among different burst
types. This paper proposes a high-performance detection model for SRBs
based on the Deformable DEtection TRansformer (DETR) called DETR4SBRs.
First, this study designed a scale-sensitive attention module to better
address the scale variations of SRBs. Subsequently, this study
introduced collaborative hybrid auxiliary training to mitigate the
positivenegative sample imbalance issue in Deformable DETR. The
experimental results demonstrate that the proposed model achieves a
mAP@50 of 83.5% and a recall rate of 99.4% on the SRBs data set.
Additionally, the model exhibits excellent noise-robust performance and
can efficiently detect and locate Type II, III, IV, and V SRBs. The
model proposed in this study provides robust support for preliminary SRB
data processing and has significant implications for space weather
forecasting. The source code and data are available on
https://github.com/onewangqianqian/SSA-Co-Deformable-DETR.git, and the
software is archived on Zenodo.</description>
</item>
<item>
<title> Impulsive Solar Flares in the Parker Solar Probe Era. I. Low-energy Electron, Proton, and Alpha Beams</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...985...19A</link>
<description>Multiple instruments on board the Parker Solar Probe spacecraft have
detected signatures of impulsive electron and ion beam events over the
course of the first 20 encounters. The energy spectra of these events
are characterized by a peak originating in the low-frequency bandwidth
of the FIELDS sensor and descending over time in energy until it merges
with the bulk of the solar wind as observed by the Solar Wind Electrons,
Alphas, and Protons suite. All events are well associated with Type III
radio bursts, and some are well correlated with soft and hard X-rays
generated by impulsive solar flares. These dispersive energy beam
phenomena are essential in understanding particle acceleration,
transport, and energy partitioning between electrons and ions as a
result of impulsive solar flares. In this work, we present an analysis
of said events and leverage multiwavelength observations that are
conducted by instruments on multiple platforms. Our results show, for
the first time, that solar flares are observed to be the source of low-
energy ions in interplanetary space. This discovery has never been
previously observed at such low energies by instruments at 1 au.</description>
</item>
<item>
<title> Investigating an Erupting Metric-decimetric Radio Depression and Its Physical Origin</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...984...97W</link>
<description>We present direct metric-decimetric radio imaging observations of a
fascinating quiescent filament eruption on 2024 March 17 using data from
the DAocheng Radio Telescope, with a combination of the Solar Dynamics
Observatory and the Chinese H Solar Explorer. At the radio band, even
though the filament is difficult to identify in its early phase, it
rapidly became distinct and formed a continuous loop-like dark structure
during the eruption, i.e., so-called radio depression. Compared with the
fragmentation of the erupting filament observed at the H and EUV bands,
the radio depression appeared more coherently. Based on synthetic radio
images from a three-dimensional magnetohydrodynamics simulation of a
flux-rope-filament eruption, it is suggested that the radio depression
originates from the absorption of cold and dense materials within the
erupting flux rope to the background emission. The absorption seems to
be stronger than that at the H and EUV bands, thus leading to their
apparent discrepancies. Moreover, the radio depression is also found to
occupy the lower part but not the whole body of the flux rope.</description>
</item>
<item>
<title> The Efficiency of Harmonic Emissions Excited by Energetic Electrons in Coronal Loops</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...984....1Y</link>
<description>Magnetic reconnection is a key process that drives the energy release in
solar flares. This process can occur at multiple locations along the
coronal loop. The reconnection generates energetic electrons capable of
exciting wave modes and emissions as they propagate through the loop. In
this follow-up study, we investigate the influence of the injection site
location of these energetic electrons, either at the looptop (LT) or at
the leg of the loop around a footpoint (FP), on the excitation of wave
modes, especially the second harmonic emissions (X2) in coronal loops.
Our simulations reveal that the injection location significantly impacts
the spatial distribution and intensity of excited wave modes. When
electrons are injected at the LT, electromagnetic X2, and Z-modes
dominate along the loop, with minimal excitation of Langmuir waves.
Conversely, the present study reveals that injection close to FP leads
to a strong Langmuir wave excitation throughout the loop, particularly
as electrons ascend toward the LT. We find that X2 and Z-modes are
consistently excited at the injection site with different intensities,
regardless of the injection location. However, electron injection near
the FP scenario creates favorable conditions for significant Langmuir
wave generation, potentially leading to plasma emission under specific
circumstances. These findings emphasize the importance of electron
injection location in determining the properties of the excited and
emitted waves in solar coronal loops.</description>
</item>
<item>
<title> On the limitations of using metric radio bursts as diagnostic tools for interplanetary coronal mass ejections</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...697L...9K</link>
<description>Aims. Metric radio bursts are often said to be valuable diagnostic tools
for studying the near-sun kinematics and energetics of the
interplanetary coronal mass ejections (ICMEs). Radio observations also
serve as indirect tools to estimate the coronal magnetic fields.
However, how these estimated coronal magnetic fields are related to the
magnetic field strength in the ICME at 1 AU has rarely been explored.
Our aim was to establish a relation between the coronal magnetic fields
obtained from the radio observations very close to the Sun and the
magnetic field measured at 1 AU when the ICME arrives at the Earth.
Methods. We performed statistical analyses of all metric type II radio
bursts in solar cycles 23 and 24 that were found to be associated with
ICMEs. We estimated the coronal magnetic field associated with the
corresponding CME near the Sun (middle corona) using a split-band radio
technique and compared them with the magnetic fields recorded at 1 AU
with in situ observations. Results. We found that the estimated magnetic
fields near the Sun using radio techniques are not well correlated with
the magnetic fields measured at 1 AU using in situ observations. This
could be due to the complex evolution of the magnetic field as it
propagates through the heliosphere. Conclusions. Our results suggest
that while metric radio observations can serve as effective proxies for
estimating magnetic fields near the Sun, they may not be as effective
close to the Earth. At least, no linear relation could be established
using metric radio emissions to estimate the magnetic fields at 1 AU
with acceptable error margins.</description>
</item>
<item>
<title> Non-thermal energy release in the post-impulsive phase of the May 9, 2021 event</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...697A.216Z</link>
<description>Context. In the standard model of solar flares, a magnetic flux rope
erupts and gets ejected from the Sun. The current sheets that form in
its wake are the seat of magnetic reconnection, which is thought to
power energy release throughout the long-lasting decay phase of the
thermal X-ray emission. This model has been broadly tested with plasma
diagnostics at soft X-ray, EUV, and H wavelengths. Aims. The primary
aim of the present investigation is to shed light on the acceleration of
non-thermal electrons in the post-impulsive phase through hard X-ray
(HXR) radiation and radio spectroscopic imaging at decimeter-to-meter
wavelengths. We focus our study on the case of a C4.0 class flare on May
9, 2021. Methods. This event was fully observed by multiple instruments
from three different vantage points in space. We analyzed the spectrum
and the source configuration of X-ray emission with the Spectrometer-
Telescope for Imaging X-rays (STIX) on board the Solar Orbiter
spacecraft, complemented by the Gamma-Ray Burst Monitor (GBM) aboard the
Fermi mission, and the radio emission with Nanay Radioheliograph (NRH)
and the ORFEES spectrograph. The extreme ultraviolet images from both
Solar TErrestrial RElations Observatory (STEREO-A) and Solar Dynamics
Observatory (SDO) were applied to trace the evolution of thermal plasma
and coronal magnetic structures. Results. The radio spectrum at
decimeter-to-meter wavelengths shows broadband continuum emission (type
IV burst), which is a well-known radio signature of time-extended
electron acceleration in eruptive flares. Both moving and stationary
radio sources were identified. Energetic electrons were observed in
X-rays up to 20 keV, displaying a significant correlation with the time
evolution of the stationary type IV radio burst during the long duration
decay phase, which lasted over 50 minutes. The X-ray photon spectral
index is relatively steep with a value of around  7.5 and the
integrated electron flux above 30 keV is on the order of 1.6 
10&lt;SUP&gt;32&lt;/SUP&gt; electron s&lt;SUP&gt;1&lt;/SUP&gt;. Conclusions. This case study
provides for the first time evidence that HXR emission accompanies the
onset of a stationary type IV radio burst. It ties together several
pieces of evidence to support that non-thermal electrons are released
into large-scale magnetic flux ropes during the post-impulsive phase of
eruptive solar flares. The energies of the non-thermal electrons
inferred from the X-ray spectral analysis confirm indirect estimates
from radio observations. Electron acceleration processes appear as a
significant signature of post-impulsive energy release, with energies in
the range from several to tens of kiloelectron volts (keV).</description>
</item>
<item>
<title> Correlation Between the Delay and Rise Time of VLF/LF Amplitudes During 20 Solar X-Ray Flares Observed in February 2014 at Mid-Latitude</title>
<link>https://ui.adsabs.harvard.edu/abs/2025RaSc...6008103L</link>
<description>During daylight hours, the concentration of electrons in the ionosphere
can be amplified by solar flares, which may subsequently influence the
propagation of radio waves. Previous research on Very Low Frequency
(VLF) signals focused on X-class and M-class flares. This study expands
the scope to include a broader frequency range and C-class flares.
During 20-28 February 2014, signals from 15 transmitters (18.3-81.0 kHz)
were recorded by a receiver in Bath, UK. 20 solar flares captured during
this period are investigated. A new methodology was employed to
determine the rise times of the received amplitudes for comparison with
the solar X-ray flux recorded by the Geostationary Operational
Environmental Satellite geostationary satellite. The time delays between
the onset of the X-ray flux and the onset of received amplitude changes
are calculated. The general trend shows that shorter delays are linearly
correlated to longer rise times of the amplitudes. It is found that the
absolute slopes of the linear correlation between the delay and the rise
time of M-class flares are larger than those of C-class flares. Two
flares showed onset times of received amplitudes preceding the X-ray
flux onset. A possible explanation for this is that the received signals
might also be influenced by hard X-rays rather than the analyzed soft
X-rays. In summary, this study demonstrates the effects of small C-class
and M-class flares on the propagation of VLF/LF signals and offers
insights for further research on solar flare impacts on radio waves and
the lower ionosphere.</description>
</item>
<item>
<title> Tracing the heliospheric magnetic field via anisotropic radio-wave scattering</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatSR..1511335C</link>
<description>Astrophysical radio sources are embedded in turbulent magnetised
environments. In the 1 MHz sky, solar radio bursts are the brightest
sources, produced by electrons travelling along magnetic field lines
from the Sun through the heliosphere. We demonstrate that the magnetic
field not only guides the emitting electrons, but also directs radio
waves via anisotropic scattering from density irregularities in the
magnetised plasma. Using multi-vantage-point type III solar radio burst
observations and anisotropic radio wave propagation simulations, we show
that the interplanetary field structure is encoded in the observed radio
emission directivity, and that large-scale turbulent channelling of
radio waves is present over large distances, even for relatively weak
anisotropy in the embedded density fluctuations. Tracing the radio
emission at many frequencies (distances), the effects of anisotropic
scattering can be disentangled from the electron motion along the
interplanetary magnetic field, and the emission source locations are
unveiled. Our analysis suggests that magnetic field structures within
turbulent media could be reconstructed using radio observations and is
found consistent with the Parker field, offering a novel method for
remotely diagnosing the large-scale field structure in the heliosphere
and other astrophysical plasmas.</description>
</item>
<item>
<title> Exploring the Origin of Multi-Periodic Pulsations During a White-Light Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033772L</link>
<description>We explored the quasi-periodic pulsations (QPPs) at multiple periods
during an X4.0 flare on 2024 May 10 (SOL2024-05-10T06:27), which
occurred in the complex active region of NOAA 13664. The flare radiation
reveals five prominent periods in multiple wavelengths. A 8-min QPP is
simultaneously detected in wavelengths of HXR, radio, UV/EUV, Ly$\alpha
$, and white light, which may be associated with nonthermal electrons
periodically accelerated by intermittent magnetic reconnection that is
modulated by the slow wave. A quasi-period at 14 min is observed in the
SXR and high-temperature EUV wavebands, and it may be caused by
repeatedly heated plasmas in hot flare loops. A quasi-period at about 18
min is only observed by STIX, with reconstructed SXR images suggesting
that the 18-min period pulsations should be considered as different
flares. Meanwhile, a 3-min QPP is simultaneously detected in wavelengths
of HXR, radio, and UV/EUV, which is directly modulated by the slow
magnetoacoustic wave leaking from sunspot umbrae. At last, a 2-min QPP
is simultaneously detected in HXR and radio emissions during the pre-
flare phase, which is possibly generated by a quasi-periodic regime of
magnetic reconnection that is triggered by the kink wave.</description>
</item>
<item>
<title> Characteristics Near Dawn and Dusk</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033610T</link>
<description>The characteristics of very low frequency (VLF) radio wave propagation
in the Earth-ionosphere waveguide are determined particularly through
dawn and dusk using phase and amplitude measurements of man-made signals
propagating below the ionospheric D region. For the first time
variations of "Wait" height and sharpness parameters, H' and , have
been determined for dawn and dusk conditions. These measurements provide
observational data to constrain D region modeling efforts, extending the
capabilities of VLF propagation monitoring for geophysical phenomena
such as lightning, solar flares, and energetic particle precipitation.
At mid-latitudes, H' varied from 85 km at night, then, starting from
solar zenith angle (SZA)  97.5, rapidly down to 73 km at dawn (SZA =
90), then back up to 78 km at SZA  75 and then down to the
appropriate noon value for the latitude (and season). In contrast, from
noon through dusk to night, H' varied essentially monotonically from 70
to 75 km through 80 to 85 km. At low latitudes no dawn minimum in H'
was observed, due to the reduced effect of galactic cosmic rays (GCR).
Sharpness, , varied from its nighttime value of 0.6 km&lt;SUP&gt;1&lt;/SUP&gt;
down to a minimum of 0.25 km&lt;SUP&gt;1&lt;/SUP&gt; at SZA 85 near dusk or 75
near dawn, rising again to (SZA-dependent) noon values of 0.350.5
km&lt;SUP&gt;1&lt;/SUP&gt;. The results are interpreted through the geophysical
effects controlling D region electrons, including the daytime dominant
role of solar Lyman- from low to mid-latitudes, and the greater role of
GCR at increasingly higher mid-latitudes.</description>
</item>
<item>
<title> The Effects of Solar Flares and Geomagnetic Storm on the Upper and Lower Ionosphere Across the Malay Archipelago Between 8th and 15th May 2024</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033601A</link>
<description>The Mother's Day Storm is the strongest solar storm event in Solar Cycle
25 to date and has been the strongest solar storm since the Halloween
storm of 2003. This event provides a great opportunity to investigate
the effect of the solar storm on the upper and lower ionospheres. In
this study, we investigated the response of the ionosphere to solar
flares and geomagnetic storms between 8th and 15th May 2024, using very
low frequency radio waves (VLF) collected by our newly built UTM-SID VLF
receiver and analyzing the Total Electron Contents (TEC), detrended TEC
(dTEC), and Rate Of TEC change Index (ROTI) derived from Global
Positioning Satellite System (GNSS) signals across the Malay Archipelago
Region. UTM-SID successfully detected 38 out of 114 solar flares that
occurred during this period, and the detection depended on the intensity
and time of the solar flare. 7 dTEC and 5 ROTI responses were noted,
along with a rapid enhancement of vertical TEC (vTEC) of up to 0.5 TECU
during severe solar flares. Meanwhile, the geomagnetic storm that
occurred on 1112 May had induced high dTEC and ROTI variations, with
dTEC reaching 5 TECU and ROTI of 0.5 TECU/min, suggesting the occurrence
of a Travelling Ionospheric Disturbance (TID). Additionally, Equatorial
Plasma Bubbles (EPB) were found to be suppressed on 11 May and a pre-
sunrise EPB was noted on 12 May. Background VLF signals are also
enhanced during this period.</description>
</item>
<item>
<title> Simultaneous multi-spacecraft observations with VLBI radio telescopes to study the interplanetary phase scintillation</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ExA....59...19M</link>
<description>Ground-based observations of spacecraft signals have been used to study
space weather. However, single spacecraft measurements observed from the
Earth have limitations in studying the structure and evolution of solar
plasma as they are unable to differentiate spatial and temporal
variations. To overcome this limitation and improve our understanding of
interplanetary scintillation, we simultaneously observed radio signals
transmitted by two co-orbiting spacecraft: the ESA Mars Express (MEX)
and the Chinese National Space Administration Tianwen-1 (TIW-1). We
conducted the observations from April to November 2021 using the
University of Tasmania's VLBI radio telescopes at 8.4 GHz. We employed
the Planetary Radio Interferometer and Doppler Experiment (PRIDE)
technique to determine the topocentric Doppler measurements and residual
phase of the carrier signal. These observables were used to quantify the
phase fluctuations of the spacecraft signals caused by solar wind and
hydrodynamic turbulence in the interplanetary medium. The measured phase
fluctuations RMS from both spacecraft show small differences which are
caused by factors such as the spacecraft's motion, onboard electronics,
and variations in the uplink signal path through Earth's ionosphere.
These fluctuations decrease with solar elongation and correlate with
solar radio flux at 10.7 cm (2800 MHz), indicating solar activity. The
estimated total electron contents along MEX and TIW-1's radio lines of
sight are similar, with higher values at lower solar elongations.
Simultaneous multi-spacecraft observations also enable RFI
characterization, frequent spacecraft performance comparisons, and
investigation of solar activity effects on spacecraft performance and
scientific outcomes.</description>
</item>
<item>
<title> X-class Flare on 2023 December 31 Observed by the Solar Ultraviolet Imaging Telescope on Board Aditya-L1</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...983L...6R</link>
<description>We present the multiwavelength study of the ejection of a plasma blob
from the limb flare SOL2023-12-31T21:36:00 from NOAA 13536 observed by
the Solar Ultraviolet Imaging Telescope (SUIT) on board Aditya-L1. We
use SUIT observations along with those from the Atmospheric Imaging
Assembly (AIA) on board the Solar Dynamics Observatory and
Spectrometer/Telescope for Imaging X-rays (STIX) on board Solar Orbiter
to infer the kinematics and thermal nature of the ejected blob and its
connection to the associated flare. The observations show that the flare
was comprised of two eruptions. The blob was ejected during the first
eruption and later accelerated to velocities over 1500 km s&lt;SUP&gt;1&lt;/SUP&gt;
measured at a maximum projected height of 178 Mm from the Sun's
surface. The acceleration of the ejected plasma blob is cotemporal with
the bursty appearance of the hard X-ray light curve recorded by STIX.
Radio spectrogram observations from STEREO-A/WAVES and RSTN reveal type
III bursts at the same time, indicative of magnetic reconnection. DEM
analysis using AIA observations suggests the plasma blob is comprised of
cooler and denser plasma in comparison to the ambient corona. To the
best of our knowledge, this is the first observation of such a plasma
blob in the near-ultraviolet providing crucial measurements for eruption
thermodynamics.</description>
</item>
<item>
<title> Two Phases of Particle Acceleration of a Solar Flare Associated with In Situ Energetic Particles</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...983...33W</link>
<description>How impulsive solar energetic particle (SEP) events are produced by
magnetic-reconnection-driven processes during solar flares remains an
outstanding question. Here we report a short-duration SEP event
associated with an X-class eruptive flare on 2021 July 3, using a
combination of remote sensing observations and in situ measurements. The
in situ SEPs were recorded by multiple spacecraft including the Parker
Solar Probe. The hard X-ray (HXR) light curve exhibits two impulsive
periods. The first period is characterized by a single peak with a rapid
rise and decay, while the second period features a more gradual HXR
light curve with a harder spectrum. Such observation is consistent with
in situ measurements: the energetic electrons were first released during
the early impulsive phase when the eruption was initiated. The more
energetic in situ electrons were released several minutes later during
the second period of the impulsive phase when the eruption was well
underway. This second period of energetic electron acceleration also
coincides with the release of in situ energetic protons and the onset of
an interplanetary type III radio burst. We conclude that these
multimessenger observations favor a two-phase particle acceleration
scenario: the first, less energetic electron population was produced
during the initial reconnection that triggers the flare eruption, and
the second, more energetic electron population was accelerated in the
region above the loop-top below a well-developed, large-scale
reconnection current sheet induced by the eruption.</description>
</item>
<item>
<title> A robust preprocessing pipeline for RATAN-600 solar radio observations data</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;C....5100918K</link>
<description>The advancement of observational technologies and software for
processing and visualizing spectro-polarimetric microwave data obtained
with the RATAN-600 radio telescope opens new opportunities for studying
the physical characteristics of solar plasma at the levels of the
chromosphere and corona. These levels remain some difficult to detect in
the ultraviolet and X-ray ranges. The development of such methods allows
for more precise investigation of the fine structure and dynamics of the
solar atmosphere, thereby deepening our understanding of the processes
occurring in these layers. The obtained data also can be utilized for
diagnosing solar plasma and forecasting solar activity. However, using
RATAN-600 data requires extensive data processing and familiarity with
the RATAN-600. This paper introduces RatanSunPy, an open-source Python
package developed for accessing, visualizing, and analyzing multi-band
radio observations of the Sun from the RATAN-600 solar complex. The
package offers comprehensive data processing functionalities, including
direct access to raw data, essential processing steps such as
calibration and quiet Sun normalization, and tools for analyzing solar
activity. This includes automatic detection of local sources,
identifying them with NOAA (National Oceanic and Atmospheric
Administration) active regions, and further determining parameters for
local sources and active regions. By streamlining data processing
workflows, RatanSunPy enables researchers to investigate the fine
structure and dynamics of the solar atmosphere more efficiently,
contributing to advancements in solar physics and space weather
forecasting.</description>
</item>
<item>
<title> Dynamic spectra of solar radio emissions from weak-turbulence simulation</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...696A.187L</link>
<description>Context. In recent decades, serious efforts have been made in the
analytical and numerical modeling of solar radio bursts generated by the
electron beam interacting with the background plasma, including the
dynamic spectra with decreasing frequency over time/space. These are
type II and type III radio bursts, with the fundamental components at
the local plasma frequency (&lt;SUB&gt;p&lt;/SUB&gt; = 2f&lt;SUB&gt;p&lt;/SUB&gt;) and the
harmonics (n&lt;SUB&gt;p&lt;/SUB&gt; = 2nf&lt;SUB&gt;p&lt;/SUB&gt;). Synthetic spectra built
for a number of radio events were able to reproduce the decreasing
frequency profiles reasonably well, despite the limitations of the
approximate analytical theory. Aims. We propose new modeling of dynamic
radio emission spectra using weak-turbulence (WT) theory. This novel
approach also aims at a self-consistent and quantitative evaluation of
radio emissions, based on first-principles modeling of electron beam
plasma instabilities and nonlinear wave interaction. Methods. We
performed the WT simulation, which has the ability to quantitatively
describe the standard plasma emission involving the nonlinear
interaction of Langmuir (L), ion-sound (S), and transverse
electromagnetic (T) waves. The composite dynamic spectra are constructed
for type II- and type III-like events, against the background electron
density model that behaves as an inverse square of the distance from the
solar source. Results. The new dynamic spectra are obtained distinctly,
with a rapid frequency shift for type III emissions (generated by fast
electron beams from coronal sources), as well as a less steep frequency
drop for type II spectra (whose sources move away from the Sun along
with interplanetary shocks). Upon making a qualitative comparison with
typical solar radio emission events, we find that our first-principle-
based synthetic dynamic spectra are in good agreement. Conclusions. The
findings of the present study demonstrate that the theoretical approach
taken in this paper can be further applied to obtain (i) quantitatively
relevant predictions and replications of the observed dynamic spectra of
radio bursts, and (ii) more realistic large-scale models of the solar
radio source, for example the type II and type III source models
computed from the large-scale magnetohydrodynamics (MHD) simulations or
even from direct spacecraft observations.</description>
</item>
<item>
<title> Electron beam propagation and radio-wave scattering in the inner heliosphere using five spacecraft</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...696A.124C</link>
<description>Context. Solar energetic particles such as electrons can be accelerated
to mildly relativistic velocities in the solar corona. These electrons
travel through the turbulent corona, generating radio waves, which are
then severely affected by scattering. Aims. The physical interpretation
of the discrepancies between the actual and observed radio sources is
still subject to debate. We used radio emission observed by an
unprecedented total of five spacecraft to track the path of radio
sources from the low corona to the inner heliosphere (1575
R&lt;SUB&gt;&lt;/SUB&gt; or 0.070.35 au generated during a solar event on 4
December 2021. Methods. We used the Bayesian multilateration technique
known as BELLA to track the apparent path of radio sources observed by
Parker Solar Probe, STEREO A, Wind, Solar Orbiter, and Mars Express. To
validate the accuracy of the tracked path, we used Nanay
Radioheliograph interferometric imaging at 150 MHz, which was found to
agree with the estimated footpoints predicted by BELLA. We further
validated our results using ACE in situ measurements. Results. We find
that the apparent radio sources followed the path of an Archimedean
Parker spiral, with an associated solar wind velocity of approximately
493 km s&lt;SUP&gt;1&lt;/SUP&gt; (consistent with the corresponding speed observed
at 1 au at the relevant longitude), and connected to the solar surface
at 75 longitude east. Finally, we made quantitative estimates of the
scattering of radio waves, which we found to be in good agreement with
contemporary models of scattering in which the radio waves primarily
propagate along the local Parker spiral. Conclusions. This work shows
conclusive evidence that the cause of the widely observed 'higher-than-
expected' electron densities at interplanetary distances is due to
radio-wave scattering, and provides a more detailed understanding of the
propagation of radio waves emitted near the local plasma frequency in
turbulent astrophysical plasmas.</description>
</item>
<item>
<title> First Global Machine Learning Model to Predict the Rate of TEC Index (ROTI) Response to X-Class Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SpWea..2304247M</link>
<description>Solar flares are bursts of electromagnetic radiation originating in the
Sun's atmosphere. Solar flares cause a rapid increase in ionization in
the ionosphere, resulting in radio signal interference. This paper aims
to predict the ionospheric response to the solar flare of various
characteristics in all latitudes around the dayside ionosphere. X-ray
flux measured by the Geostationary Operational Environmental Satellite
(GOES) satellite associated with 84 solar flare events between 2000 and
2017 are obtained. Global total electron content (TEC) data from more
than 5,000 ground Global Navigation Satellite System receivers are used.
The rate of the TEC Index (Rate of TEC Index (ROTI)) is calculated to
examine the time evolution of ionospheric response. Three selected
events are studied in detail by eliminating the ROTI associated with
stations on the nightside. A nonlinear response of the ionosphere
associated with solar flare characteristics including rise/fall time and
maximum amplitude is discussed. The first global machine learning (ML)
model to predict solar flare impact on Earth's ionosphere through ROTI
parameter is developed. Solar flare parameters measured by the GOES
satellite along with solar radiation angle and ROTI data from 5-degree
latitude ranges are selected as an input to the ML model. Thek-nearest
neighbors and random forest algorithms are used. Quantitative and
qualitative results show that the random forest provides better accuracy
in predicting the time evolution of ionospheric response to X-class
solar flare. The coefficient of determination (${\mathrm{R}}^{2}$) and
the Pearson Correlation Coefficient (r) are used to provide a
quantitative comparison of the model prediction with the actual data.</description>
</item>
<item>
<title> II. Features of the Flare and Its Atypical Microwave Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...29G</link>
<description>As known, large near-Earth proton enhancements usually occur after major
eruptive solar flares accompanied by strong microwave bursts. Typically,
the spectral-maximum frequency of such a burst exceeds 10 GHz, and the
flux exceeds 104 sfu. Ground-level cosmic-ray enhancements (GLEs) are
the most energetic subset of large proton events, and it seems that
microwave bursts in GLE-associated flares should follow this pattern.
This is true in most cases, but in individual events that have produced
GLEs, only moderate microwave bursts have been observed. In particular,
in the SOL2012-05-17 event responsible for GLE71, the spectral-maximum
frequency of the microwave burst did not exceed 10 GHz, and the flux did
not reach 103 sfu. We found that the temporal profile of the microwave
burst followed the smoothed magnetic-reconnection rate, lagging behind
it by about 50 s and that the burst properties were determined by the
following circumstances: i) the magnetic configuration was asymmetric,
and ii) the sources of the gyrosynchrotron emission were the entire
flare arcade and a compact region above the sunspot umbra. Observations
directly demonstrated these features, which were previously inferred for
the SOL2001-12-26 event responsible for GLE63. A long-known discrepancy
was observed between the estimates of the electron spectrum obtained
from hard X-rays and microwaves. However, the hardening of the spectrum
of trapped electrons that has been invoked to explain this discrepancy
was not found in this event. Indications of a relationship between flare
processes and proton acceleration are discussed.</description>
</item>
<item>
<title> Two-Part Interplanetary Type II Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...25P</link>
<description>Two similar-looking, two-part interplanetary type II burst events from
2003 and 2012 are reported and analysed. The 2012 event was observed
from three different viewing angles, enabling comparisons between the
spacecraft data. In these two events, a diffuse wide-band type II radio
burst was followed by a type II burst, which showed emission at the
fundamental and harmonic (F-H) plasma frequencies, and these emission
bands were also slightly curved in their frequency-time evolution. Both
events were associated with high-speed, halo-type coronal mass ejections
(CMEs). In both events, the diffuse type II burst was most probably
created by a bow shock at the leading front of the CME. However, for the
later appearing F-H type II burst, there are at least two possible
explanations. In the 2003 event, there is evidence of CME interaction
with a streamer, with a possible shift from a bow shock to a CME flank
shock. In the 2012 event, a separate white-light shock front was
observed at lower heights, and it could have acted as the driver of the
F-H type II burst. There is also some speculation on the existence of
two separate CMEs, launched from the same active region, close in time.
The reason for the diffuse type II burst being visible only from one
viewing direction (STEREO-A) and the ending of the diffuse emission
before the F-H type II burst appears still need explanations.</description>
</item>
<item>
<title> Features of correlation curves of the Siberian Radioheliograph</title>
<link>https://ui.adsabs.harvard.edu/abs/2025STP....11a..81U</link>
<description>Correlation curves of the multi-frequency Siberian Radioheliograph (SRH)
provide a sensitive indication and demonstrative representation of
monitoring the microwave life of the active Sun. We derive approximate
relationships and briefly discuss the contribution of the quiet Sun,
active regions, radio bursts, satellites, and atmospheric absorption to
the radioheliograph's correlation response. The estimates are obtained
under the assumption that the activity centers and the quiet Sun are
homogeneous disks of different sizes and brightness. The sensitivity of
the correlation curves to weak sources of small angular sizes is due to
their wide spatial spectrum. The wide spectrum means that each pair of
antennas produces a noticeable interferometric response, so the total
response is significant. The correlation curves allow us to estimate
spatial sizes of the radio burst source at different frequencies, but do
not allow us to calculate the shape of its radio spectrum. Variability
in the atmospheric water content over time creates fluctuations of the
received solar radio flux. The correlation response is much less
susceptible to this factor.</description>
</item>
<item>
<title> Fully convolutional neural networks for processing observational data from small remote solar telescopes</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatSR..15.9630J</link>
<description>Heliophysics phenomena on the Sun, such as radio bursts, can strongly
affect satellites and ground-based electronic systems. Therefore, an
insight into the actual image of the Sun with good spatial and temporal
resolution is crucial. In this paper, we explore the possibility of
using fully convolutional networks (FCNs) to improve the images acquired
from remotely operated small solar telescopes whose resolution is
limited by the size of the lens aperture and by atmospheric turbulence.
For this purpose, we use chromosphere data from the 50 mm small H
Telescope of the Silesian University of Technology acquired over many
months under various atmospheric conditions. We compare the obtained
results with the results of raw data processing by a state-of-the-art
deterministic algorithm, multi-frame blind deconvolution (MFBD). In our
research, we investigate the impact of the amount of data and the
complexity of FCNs on the quality of the results and their processing
time. We show that the use of FCNs is a very attractive alternative to
MFBD because they are more energy efficient and allow for the obtaining
of comparable results in orders of magnitude shorter time.</description>
</item>
<item>
<title> Forecasting solar energetic particles using multi-source data from solar flares, CMEs, and radio bursts with machine learning approaches</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatSR..15.9546A</link>
<description>This study presents a consistent method to the inherently imbalanced
problem of predicting solar energetic particle (SEP) events, using a
variety of datasets that include solar flares, coronal mass ejections
(CMEs), and radio bursts. We applied several machine learning (ML)
methods, including Random Forests (RF), Decision Trees (dtree), and
Support Vector Machines (SVM) with both linear (linSVM) and nonlinear
(svm) kernels. To assess model performance, we used standard metrics
such as Probability of Detection (POD), False Alarm Rate (FAR), True
Skill Statistic (TSS), and Heidke Skill Score (HSS). Our results show
that the RF model consistently outperforms the other algorithms across
datasets containing flares, CMEs, and radio bursts. For the sweep
frequency dataset, RF achieved a POD of , a FAR of , a TSS of ,and a HSS
of ). For the fixed-frequency dataset, RF produced a POD of , a FAR of ,
a TSS of  ,and a HSS of ). Key features for SEP prediction include CME
linear speed and angular width across both datasets. For sweep
frequency, flare intensity and integral soft X-ray (SXR) flux are
crucial, while for fixed frequency, the rise time and duration of radio
bursts at 1415 MHz are significant.</description>
</item>
<item>
<title> Effects on the attenuation and phase velocities of the waveguide modes</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JASTP.26806433B</link>
<description>Solar flares are sudden bursts of X-rays and UV rays emitted from
coronal magnetic loops in active regions near sunspots on the sun's
surface. Soft X-rays below 1 nm penetrate the D-region ionosphere,
causing excess ionization and altering its conductivity profile. This
study examines solar flares (C-class and M-class) from the 25th solar
cycle using two Very Low Frequency (VLF, 330 kHz) radio receivers in
the low-latitude Indian region, located in Cooch Behar (CHB) and Kolkata
(CUB). The work focuses on the Indian VLF transmitter VTX at a frequency
of 18.2 kHz to study the effects of solar flares on the D-region
ionosphere and VLF signal propagation characteristics in the earth-
ionosphere waveguide. The solar zenith angle at the CUB station has a
significant impact on the magnitude of VLF amplitude disruption caused
by solar flares, showing a positive correlation (r = +0.82, r = +0.61)
with flare power during low and high solar activity, respectively. In
contrast, CHB exhibits both positive and negative amplitude
perturbations, with a negative correlation (r = 0.83, r = 0.78)
between flare power and VLF amplitude under similar conditions. The Long
Wave Propagation Capability (LWPC) code has been used to explain the
differences in the observed amplitude perturbations due to solar flares
in both receivers. Solar flares weaker than C2.0 at CHB reduce
attenuation and phase velocity of the propagating waveguide modes in the
earth-ionosphere waveguide, causing positive amplitude perturbations,
while stronger flares increase these parameters, resulting in negative
perturbations. In contrast, solar flares of all classes cause an
increase in phase velocities and a decrease in attenuation coefficients
of the propagating waveguide modes along the VTX-CUB propagation path,
resulting in positive VLF amplitude responses. This study highlights
distinct responses of VLF signals to solar flares in different
propagation paths, emphasizing the complex interactions between solar
activity and earth-ionosphere waveguide properties.</description>
</item>
<item>
<title> Trends of Solar, Interplanetary, and Geomagnetic Parameters during the Recent Five Solar Cycles</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JASS...42...29K</link>
<description>This study examined the variations of solar, interplanetary, and
geomagnetic (SIG) parameters from 1974 to 2024 to assess the changes in
the solar cycle. Eleven SIG parameters were analyzed, including the
sunspot number (SSN), solar magnetic field, 10.7 cm solar radio flux,
total solar irradiance, and Ap index. This study also aimed to predict
Solar Cycle 25 using the seasonal autoregressive integrated moving
average (SARIMA) statistical forecasting model. The results showed that
consistent with previous studies, all SIG parameters exhibited a strong
correlation with the SSN. The change in SSN strongly influences the
variations in all SIG parameters, even though some exhibit time-lagged
responses. The cross-correlation analysis revealed a high correlation
coefficient of 0.9678 between the SSN and the 10.7 cm solar radio flux
without delay. Most SIG parameters showed a general weakening trend
toward Solar Cycles 2224. This suggests that solar activity is waning
over time. In particular, the solar polar magnetic field (SPMF) showed a
large decrease in the solar minimum 23/24, and specifically, the SPMF at
the south pole weakened more rapidly than at the north pole. Hence, the
SPMF is changing asymmetrically between the north and south poles. This
weakening of the solar magnetic field suggests an increase in galactic
cosmic rays within the heliosphere, exposing the Earth to higher levels
of cosmic rays. Finally, forecasts for Solar Cycle 25 using the SARIMA
model predict that the SSN will continue to decline after the solar
maximum in 2024, with the predicted minimum SSN of 9.42 in October 2028,
and will likely enter a solar minimum period around 2030.</description>
</item>
<item>
<title> The first analysis of the outward H fluxes measured by IBEX-Lo in 2050 R&lt;SUB&gt;E&lt;/SUB&gt; geocentric distances</title>
<link>https://ui.adsabs.harvard.edu/abs/2025FrASS..1229064P</link>
<description>In this study, we analyze the energetic neutral atom (ENA) observations
measured in the lowest energy channel (1021 eV) of the IBEX-Lo
instrument on Interstellar Boundary Explorer (IBEX) during two spring
seasons, day of year (DOY) 101146, 2009, and DOY 88178, 2013,
confirming the existence of outward hydrogen (H) fluxes at 15 eV. The
outward H flux decreases slightly with distance, showing an intensity of
approximately 10&lt;SUP&gt;6&lt;/SUP&gt; cm&lt;SUP&gt;2&lt;/SUP&gt; s&lt;SUP&gt;1&lt;/SUP&gt;
sr&lt;SUP&gt;1&lt;/SUP&gt; keV&lt;SUP&gt;1&lt;/SUP&gt;. Results also suggest that the outward
H fluxes are not influenced by solar radio flux. We compute the expected
H ENA fluxes at 15 eV using ion flux measurements from the Helium,
Oxygen, Proton, and Electron (HOPE) mass spectrometer aboard the
Radiation Belt Storm Probes (RBSP) during the corresponding period of
the 2013 spring season, combined with a simple exospheric density model
(n H  =  n  H 0        r 0  / r    3, where r 0  = 10 R&lt;SUB&gt;E&lt;/SUB&gt;).
The expected ENA fluxes similarly show a decrease in the intensity with
increasing geocentric distance, which is on the order of
10&lt;SUP&gt;5&lt;/SUP&gt;10&lt;SUP&gt;6&lt;/SUP&gt; cm&lt;SUP&gt;-2&lt;/SUP&gt; s&lt;SUP&gt;1&lt;/SUP&gt;
sr&lt;SUP&gt;1&lt;/SUP&gt; keV&lt;SUP&gt;1&lt;/SUP&gt;. These consistent features suggest that
the outward H fluxes observed by IBEX-Lo are closely related to escaping
H ENAs produced within the inner exosphere (&lt;4 R&lt;SUB&gt;E&lt;/SUB&gt;).</description>
</item>
<item>
<title> Decay of Turbulent Upper-hybrid Waves in Weakly Magnetized Solar Wind Plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...982L..24P</link>
<description>Large-scale and long-term two-dimensional particle-in-cell simulations
of high resolution are performed for the first time to study the
dynamics of electrostatic decay of upper-hybrid wave turbulence
generated by electron beams into Langmuir/-mode () waves in weakly to
moderately magnetized plasmas, in conditions relevant to type III solar
radio bursts. Simulations use parameters characteristic of beamplasma
interactions between 0.1 and 1 au. The impact of plasma magnetic field
on decay is shown, and magnetic properties of  waves are determined.
During their energy transport through k wavevector scales, waves undergo
several decay cascades, acquiring increasing magnetic energy until they
reach electromagnetic -mode dispersion below the plasma frequency.
Whereas the impact of magnetic field on decaying waves of large k = k
is weak, important differences with respect to the unmagnetized plasma
case manifest at small k-scales, where a boundary layer delimiting a
spectral domain free of  energy is revealed. It prevents decayed waves
from reaching the -mode cutoff frequency and a high level of left-handed
polarization, and it modifies the conditions for the appearance of
modulational instabilities and strong turbulence phenomena at k  0.
Ordinary -mode waves are generated jointly with -mode waves at
comparable energy levels, via electromagnetic decay, whereas -mode
emissions are much weaker in most cases. These results provide support
for the interpretation of observations by satellites such as Parker
Solar Probe and Solar Orbiter, and they supply a solid basis for
tackling the more complex problem of dynamics of upper-hybrid wave
turbulence in magnetized plasmas where random density fluctuations
cannot be neglected.</description>
</item>
<item>
<title> Multi-category solar radio burst detection based on task-aligned one-stage object detection model</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Ap&amp;SS.370...23W</link>
<description>Accurate identification of solar radio bursts (SRBs) is essential for
advancing research in solar physics and predicting space weather.
However, the majority of current studies mainly concentrate on detecting
whether SRBs are present or absent, often focusing on only one
particular type of burst. Moreover, the neural network models used for
SRB detection are typically complex, involving a large number of
parameters, which results in slower processing speeds. This study
establishes a dataset encompassing Type II, Type III, Type IIIs, Type
IV, and Type V SRBs collected from e-CALLISTO, including 8,752 SRB
spectrum images and achieving annotations for 10,822 SRBs. We propose a
multi-category SRB detection model based on task-aligned one-stage
object detection (TOOD). TOOD can solve the problem of inconsistent
predictions in classification and localization tasks, and it improves
the detection recall rate. This model aligns classification and
localization tasks and optimizes the neck network by incorporating a
channel attention mechanism. This model achieves higher recall and
accuracy with fewer parameters. This model can accurately detect five
types of SBRs. The experimental results show that the model achieved an
accuracy of 79.9% (AP50) and a recall rate of 95.1% on the SBRs dataset.
A higher recall rate than other models means fewer SRBs are missed in
automatic detection. The model we propose has the potential to make a
substantial impact on solar physics research and space weather studies.
Additionally, the findings in this paper could provide valuable insights
for processing other small-sample astronomical, datasets. The source
code and data is available at
https://github.com/onewangqianqian/MobileNetVitv2-TOOD.git.</description>
</item>
<item>
<title> Particle Acceleration in Solar Flares From Radio and Hard X-Ray Spectra</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AN....34640134V</link>
<description>For a deeper understanding of the physical processes at play in solar
flares, it is necessary to analyze the flare emissions at multiple
wavelengths. This multifrequency approach enables the characterization
of energetic electrons accelerated from hundreds of keV and up to
several tens of MeV. This study reports on the observation of 10 solar
flares, in which the spectral parameters were determined for the cm/mm
and x-ray bands. The radio spectrum was fitted using gyrosynchrotron
emission whereas the hard x-rays fit considered a model of thermal plus
nonthermal emission of accelerated electrons. The results show that the
spectral indices of the energy distribution of nonthermal electrons
emitting in millimeter and hard x-rays do not agree, with the millimeter
spectral index being approximately 2 units harder than that of hard
x-rays. These findings are consistent with previous research and suggest
the existence of a break in the energy spectrum of accelerated
electrons. Moreover, for the only flare where photons exceeding 1 MeV
were detected, the hard x-ray spectra exhibited a broken power-law where
the index of the electron distribution above ~500 keV agreed with the
inferred radio spectral index.</description>
</item>
<item>
<title> Effects of the September 2014 coronal mass ejection chain in the inner Solar System and the response of the Martian ionosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...695A.225I</link>
<description>Context. During September 2014, intense solar activity led to a number
of coronal mass ejections (CMEs) propagating in the heliosphere. The
strong perturbation in the interplanetary magnetic field and the
remarkable enhancements in the energetic particle fluxes accelerated by
the shock waves associated with the CMEs affected the environments of
the inner planets of the Solar System. Aims. Taking advantage of a
relatively favorable position in terms of angular distance among
Mercury, Earth, and Mars, our purpose is to observe the evolution and
impact of strong solar events, providing an overview of the impact of
the same solar phenomena on different planetary environments, with
special interest in the response of Mars' ionosphere as this may have
implications for future exploration of the red planet. Methods. We used
observations from a fleet of spacecraft distributed in the inner Solar
System, such as STEREO B, MESSENGER, Mars Express, and SOHO, to perform
a characterization of the interaction with the planets, investigating
some of the main effects of the CMEs on the different planetary
environments. Besides, we applied a numerical simulation to reconstruct
the magnetic connection from Mercury, Earth, and Mars to the solar
corona on the dates on which the CME events occurred. Results. We find
that the CMEs events analyzed here induced remarkable effects that
affected all the environments of the inner planets of the Solar System.
Enhancements in the solar energetic particle fluxes were observed at
Mercury, Earth, and Mars, with different characteristics. In addition, a
solar radio burst was observed both at Earth and Mars, together with
strong disturbances in the geomagnetic field, and diffuse echoes and
radio black outs in the Martian ionosphere. Conclusions. The proposed
multi-spacecraft and multiparameter analysis, along with the numerical
simulations for reconstructing the magnetic footpoints of the Parker
spiral on the Sun's surface, offer a detailed cause-and-effect framework
for studying space weather events in the Solar System.</description>
</item>
<item>
<title> Bursty acceleration and 3D trajectories of electrons in a solar flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...695A.136B</link>
<description>Context. During a solar flare, electrons are accelerated to non-thermal
energies as a result of magnetic reconnection. These electrons then
propagate upwards and downwards from the energy release site along
magnetic field lines and produce radio and X-ray emission. Aims. On 11
November 2022, an M5.1 solar flare was observed by the
Spectrometer/Telescope for Imaging X-rays (STIX) on board Solar Orbiter
together with various ground- and space-based radio instruments. The
flare was associated with several fine hard X-ray (HXR) structures and a
complex set of metric radio bursts (type III, J, and narrowband). By
studying the evolution of X-ray, extreme ultraviolet, and radio sources,
we aim to study the trajectories of the flare-accelerated electrons in
the lower solar atmosphere and low corona. Methods. We used observations
from the STIX on board Solar Orbiter to study the evolution of X-ray
sources. Using radio imaging from the Nanay Radio heliograph (NRH) and
the Newkirk density model, we constructed 3D trajectories of 14 radio
bursts. Results. Imaging of the HXR fine structures shows several
sources at different times. The STIX and NRH imaging shows correlated
changes in the location of the HXR and radio source at the highest
frequency during the most intense impulsive period. Imaging and 3D
trajectories of all the bursts show that electrons are getting
accelerated at different locations and along several distinct field
lines. Some of the trajectories from the same origin show expansion on
the order of 4 over a height of 110 Mm. The longitude and latitude
extent of the trajectories are 30 and 152. Conclusions. We find that
the electrons producing HXR and radio emission have similar acceleration
origins. Importantly, our study supports the scenario that the flare
acceleration process is temporally and spatially fragmentary, and during
each of these small-scale processes, the electron beams are injected
into a very fibrous environment and produce complex HXR and radio
emission.</description>
</item>
<item>
<title> The reason for the widespread energetic storm particle event of 13 March 2023</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...695A.127D</link>
<description>Context. On 13 March 2023, when the Parker Solar Probe spacecraft (S/C)
was situated on the far side of the Sun as seen from Earth, a large
solar eruption took place, which created a strong solar energetic
particle (SEP) event observed by multiple S/C all around the Sun. The
energetic event was observed at six well-separated locations in the
heliosphere, provided by the Parker Solar Probe, Solar Orbiter,
BepiColombo, STEREO A, near-Earth S/C, and MAVEN at Mars. Clear
signatures of an in situ shock crossing and a related energetic storm
particle (ESP) event were observed at all inner-heliospheric S/C,
suggesting that the interplanetary coronal mass ejection (CME)-driven
shock extended all around the Sun. However, the solar event was
accompanied by a series of pre-event CMEs. Aims. We aim to characterize
this extreme widespread SEP event and to provide an explanation for the
unusual observation of a circumsolar interplanetary shock and a
corresponding circumsolar ESP event. Methods. We analyzed data from
seven space missions, namely Parker Solar Probe, Solar Orbiter,
BepiColombo, STEREO A, SOHO, Wind, and MAVEN, to characterize the solar
eruption at the Sun, the energetic particle event, and the
interplanetary context at each observer location as well as the magnetic
connectivity of each observer to the Sun. We then employed
magnetohydrodynamic simulations of the solar wind in which we injected
various CMEs that were launched before as well as contemporaneously with
the solar eruption under study. In particular, we tested two different
scenarios that could have produced the observed global ESP event: (1) a
single circumsolar blast-wave-like shock launched by the associated
solar eruption, and (2) the combination of multiple CMEs driving shocks
into different directions. Results. By comparing the simulations of the
two scenarios with observations, we find that both settings are able to
explain the observations. However, the blast-wave scenario performs
slightly better in terms of the predicted shock arrival times at the
various observers. Conclusions. Our work demonstrates that a circumsolar
ESP event, driven by a single solar eruption into the inner heliosphere,
is a realistic scenario.</description>
</item>
<item>
<title> Resolving spatial and temporal shock structures using LOFAR observations of type II radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...695A..70M</link>
<description>Context. Collisionless shocks are one of the most powerful particle
accelerators in the Universe. In the heliosphere, type II solar radio
bursts are signatures of electrons accelerated by collisionless shocks
launched at the Sun. Spectral observations of these bursts show a
variety of fine structures often composing multiple type II lanes. The
origin of these lanes and structures is not well understood and has been
attributed to the inhomogeneous environment around the propagating
shock. Aims. Here, we aim to determine the large-scale local structures
near a coronal shock wave using high-resolution radio imaging
observations of a complex type II radio burst observed on 3 October
2023. Methods. By using inteferometric imaging from the Low Frequency
Array (LOFAR), combined with extreme ultraviolet observations, we
investigate the origin of multiple type II lanes at low frequencies
(3080 MHz) relative to the propagating shock wave. Results. We identify
at least three radio sources at metric wavelengths corresponding to a
multi-lane type II burst. The type II burst sources propagate outwards
with a shock driven by a coronal mass ejection. We find a double radio
source that exhibits increasing separation over time, consistent with
the expansion rate of the global coronal shock. This suggests that the
overall shock expansion is nearly self-similar, with acceleration
hotspots forming at various times and splitting at a rate proportional
to the shock's expansion. Conclusions. Our results show the importance
of increased spatial resolution in determining either the small-scale
spatial properties in coronal shocks or the structuring of the ambient
medium. Possible shock corrugations or structuring of the upstream
plasma at the scale of 10&lt;SUP&gt;5&lt;/SUP&gt; km can act as hotspots for the
acceleration of suprathermal electrons. This can be observed as
radiation that exhibits double sources with increasing separation at the
same expansion rate as the global shock wave.</description>
</item>
<item>
<title> Radio dimming associated with filament eruptions in the meter and decimeter wavebands</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...695A..12H</link>
<description>Filament eruptions are considered to be a common phenomenon on the Sun
and other stars, yet they are rarely directly imaged in the meter and
decimeter wavebands. Using imaging data from the DAocheng solar Radio
Telescope (DART) in the 150450 MHz frequency range, we present two
eruptive filaments that manifest as radio dimmings (i.e., emission
depressions). Simultaneously, portions of these eruptive filaments are
discernible as dark features in the chromospheric images. The sun-as-a-
star flux curves of brightness temperature, derived from the DART
images, exhibit obvious radio dimmings. The dimming depths range from
1.5% to 8% of the background level and show a negative correlation with
radio frequencies and a positive correlation with filament areas. Our
investigation suggests that radio dimming is caused by free-free
absorption during filament eruptions obscuring the solar corona. This
may provide a new method for detecting stellar filament eruptions.</description>
</item>
<item>
<title> On a Possible Scenario of Solar Coherent Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2025SoPh..300...23L</link>
<description>The first burst of solar microwave coherent emission observed
simultaneously with two multifrequency two-dimensional radio telescopes
is reported, making it possible to unambiguously interpret the mechanism
of the radiation and to propose a scenario that explains all the
observed features of the burst. Recently, many studies have appeared
that explain coherent bursts of radio emission from the Earth's
magnetosphere and solar corona by an electron cyclotron maser (ECM)
driven by horseshoe distribution. The result of this study is that the
observed coherent burst near the frequency 4.8 GHz is caused by a hollow
beam distribution formed by the oblique injection of electrons into a
magnetic loop. If the pitch-angle is large enough, then the absence of
HXR and the relatively large (about 1 s) pulse duration can be
explained. The measured size of the ECM source, 2.2, corresponds to a
brightness temperature of 5.81010 K. The displacement of the spike
sources with respect to the gyroresonance source is consistent to the
second-harmonic ECM emission, whereas the gyroresonance source is
consistent to the third gyrolayer.</description>
</item>
<item>
<title> Performance of the segment anything model in various RFI/events detection in radio astronomy</title>
<link>https://ui.adsabs.harvard.edu/abs/2025PASA...42...19Y</link>
<description>The emerging era of big data in radio astronomy demands more efficient
and higher-quality processing of observational data. While deep learning
methods have been applied to tasks such as automatic radio frequency
interference (RFI) detection, these methods often face limitations,
including dependence on training data and poor generalisation, which are
also common issues in other deep learning applications within astronomy.
In this study, we investigate the use of the open-source image
recognition and segmentation model, Segment Anything Model (SAM), and
its optimised version, HQ-SAM, due to their impressive generalisation
capabilities. We evaluate these models across various tasks, including
RFI detection and solar radio burst (SRB) identification. For RFI
detection, HQ-SAM (SAM) shows performance that is comparable to or even
superior to the SumThreshold method, especially with large-area
broadband RFI data. In the search for SRBs, HQ-SAM demonstrates strong
recognition abilities for Type II and Type III bursts. Overall, with its
impressive generalisation capability, SAM (HQ-SAM) can be a promising
candidate for further optimisation and application in RFI and event
detection tasks in radio astronomy.</description>
</item>
<item>
<title> Enhancing Deep Learning Ionospheric Modeling With Solar Radiation and Flare Classes</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033319L</link>
<description>The ionosphere is pivotal for satellite navigation, radio communication,
and the modeling of space weather. However, the accurate three-
dimensional modeling of ionospheric features remains a challenge. Since
solar activity introduces changes in space weather, we collected COSMIC
radio occultation observations of 20102020 with a suite of indices
related to solar and geomagnetic activities, especially including solar
EUV and X-ray radiation fluxes, to develop a deep learning model for the
global ionospheric electron density. This model, which is called the
Solar Flare and Radiation Neural Network (SFRNN) and is based on
Embedding, Long Short-Term Memory and fully connected layers, presented
excellent performance in reconstructing ionospheric profiles. In this
study, 28-min was found to be the best input solar radiation interval
for SFRNN with annual RMSEs of 6.24  10&lt;SUP&gt;4&lt;/SUP&gt; to 1.56 
10&lt;SUP&gt;5&lt;/SUP&gt; el/cm&lt;SUP&gt;3&lt;/SUP&gt;. Significantly, during solar flare
events, SFRNN had a lower reconstruction error than the former
artificial neural network (ANN) model that only uses space weather
indices. The most substantial improvement was observed under X-class
flares, where SFRNN exhibited a 18.3% lower Root Mean Squared Error than
ANN. To further validate the modeling accuracy, electron density
profiles derived from Jicamarca incoherent scatter radar (ISR) were
used. SFRNN successfully provided profiles with high consistency with
the ISR observation in the ionospheric layers. Our modeling results
demonstrate that refined solar activity parameters can effectively
improve reconstruction performance.</description>
</item>
<item>
<title> On Thermospheric Molecular Oxygen and Its Relationship to Solar Activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JGRA..13033224G</link>
<description>Observations from the Global-scale Observations of Limb and Disk (GOLD)
mission have provided a new remote-sensing data source of molecular
oxygen profiles in Earth's lower-to-middle thermosphere (120200 km).
GOLD O&lt;SUB&gt;2&lt;/SUB&gt; observations indicate increasing densities of
molecular oxygen at 170 km with rising solar activity between solar
radio flux F10.7 values of 60 and 120 solar flux units (sfu). This is
also seen in comparisons with solar extreme ultraviolet irradiance
Q&lt;SUB&gt;EUV&lt;/SUB&gt; between 1 and 2.25 erg cm&lt;SUP&gt;2&lt;/SUP&gt; s&lt;SUP&gt;1&lt;/SUP&gt;.
However, the empirical Mass Spectrometer Incoherent Scatter radar 2.0
(MSIS 2.0) model overestimates O&lt;SUB&gt;2&lt;/SUB&gt; densities at 170 km at
these low levels of solar activity and predicts a decreasing density
with increasing solar flux below 120 sfu. Additional data sets validate
GOLD observations of O&lt;SUB&gt;2&lt;/SUB&gt; and their relationship with solar
activity. Accurately determining and forecasting O&lt;SUB&gt;2&lt;/SUB&gt; is
critical for accurately modeling plasma densities in the ionosphere and
thermospheric density in the lower-to-middle thermosphere.</description>
</item>
<item>
<title> data and modeling</title>
<link>https://ui.adsabs.harvard.edu/abs/2025CoSka..55b..88S</link>
<description>Solar flares, which are powerful explosions on the Sun's surface, are
well recognized driving forces that have a significant impact on the
near-Earth environment, causing extra ionization within the sunlit
Earth's atmospheric layers. Based on how they affect the lower
ionosphere and its electron density profile, X-ray solar flares can be
categorized. In order to forecast the effects of potential solar
occurrences during the waning phase of Solar Cycle 25, this study
focuses on the disturbances caused by X-ray solar flares. In this paper
we examined Solar Cycle progression i.e. solar activity of highest
intensity (strongest 50 solar flares) during the ascending phase of
Solar Cycle 25 by conducting numerical ionospheric modeling based on the
Geostationary Operational Environmental Satellite (GOES) database on
solar X-ray radiation.</description>
</item>
<item>
<title> Radiosolariz Solar Radio Telescope Short Monopole Antenna</title>
<link>https://ui.adsabs.harvard.edu/abs/2025CRABS..78....9Z</link>
<description>Not Available</description>
</item>
<item>
<title> Universal Constants in Self-organized Criticality Systems</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...980..209A</link>
<description>The occurrence frequency distributions of fluxes (F) and fluences or
energies (E) observed in the majority (in 18 out of 23 cases) of
astrophysical phenomena are found to be consistent with the predictions
of the fractal-diffusive self-organized criticality (FD-SOC) model,
which predicts power-law slopes with universal constants of
&lt;SUB&gt;F&lt;/SUB&gt; = (9/5) = 1.80 for the flux and &lt;SUB&gt;E&lt;/SUB&gt; = (5/3) 
1.67 for the fluence. The theoretical FD-SOC model is based on the
fractal dimension, the flux-volume proportionality, and classical
diffusion. The universal scaling laws predict the size distributions of
numerous astrophysical phenomena, such as solar flares, stellar flares,
coronal mass ejections, auroras, blazars, active galactic nuclei, black
hole systems, galactic fast radio bursts, gamma-ray bursts, and soft
gamma-ray repeaters. In contrast, we identify five outliers of
astrophysical phenomena, i.e., coherent solar radio bursts, random solar
radio bursts, solar energetic particles, cosmic rays, and pulsar
glitches, which are not consistent with the standard FD-SOC model, and
thus require different physical mechanisms.</description>
</item>
<item>
<title> Flares in TESS Data and Optical Spectra</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...980..196R</link>
<description>We studied the flaring activities of M4.5 dwarf AD Leo to understand its
stellar atmospheres and magnetic activities. We present new
observational results on this highly active star, using nonsimultaneous
measurement of Transiting Exoplanet Survey Satellite (TESS) data, time-
series optical spectra, and Giant Meter Radio Telescope 325 MHz radio
data. We revisited the rotation period of 2.23  0.04 days from TESS,
which matches well with previously measured literature values. We
estimated an extremely rare high-energy superflare of 4.9 
10&lt;SUP&gt;35&lt;/SUP&gt; erg and 400 minute duration with a high magnetic field
strength of 1.2 kG. Interestingly, we correlated the duration of a flare
event with its energy,   , and noticed a discrepancy between stellar
and solar flares suggesting a difference in coronal magnetic field
strength. From time-series spectra, we observed H spectral flares in
the range of 10&lt;SUP&gt;30&lt;/SUP&gt;10&lt;SUP&gt;31&lt;/SUP&gt; erg. A 12 minute delay in a
spectral flare event was observed between the emission of the H and Ca
II H and K lines, possibly due to their origination at different spatial
locations in the chromosphere. We noticed the deviation in flare rate
distribution and orbital phases indicates the presence of highly active
regions. Furthermore, an occasional radio detection with a flux density
of 9.46  1.63 mJy at a frequency of 325 MHz might be coherent emission
in the presence of the magnetic field, giving a hint of starplanet
interaction.</description>
</item>
<item>
<title> X-Ray/Radio Quasiperiodic Pulsations Associated with Plasmoids in Solar Flare Current Sheets</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...980..158K</link>
<description>Plasmoids (or magnetic islands) are believed to play an important role
in the onset of fast magnetic reconnection and particle acceleration
during solar flares and eruptions. Direct imaging of flare current
sheets and the formation/ejection of multiple plasmoids in extreme-
ultraviolet images, along with simultaneous X-ray and radio
observations, offers significant insights into the mechanisms driving
particle acceleration in solar flares. Here, we present direct imaging
of the formation and ejection of multiple plasmoids in flare
plasma/current sheets and the associated quasiperiodic pulsations (QPPs)
observed at X-ray and radio wavelengths, using observations from the
Solar Dynamics Observatory/Atmospheric Imaging Assembly, RHESSI, and the
Fermi Gamma-ray Burst Monitor. These plasmoids propagate bidirectionally
upward and downward along the flare current sheet beneath the erupting
flux rope during two successive flares associated with confined/failed
eruptions. The flux rope exhibits evidence of helical kink instability,
with the formation and ejection of multiple plasmoids in the flare
current sheet, as predicted in an MHD simulation of a kink-unstable flux
rope. RHESSI X-ray images show double coronal sources ("looptop" and
higher coronal sources) located at both ends of the flare current/plasma
sheet. Moreover, we detect an additional transient faint X-ray source
(612 keV) located between the double coronal sources, which is
cospatial with multiple plasmoids in the flare current sheet. X-ray
(soft and hard) and radio (decimetric) observations unveil QPPs (periods
 10 s and 100 s) associated with the ejection and coalescence of
plasmoids. These observations suggest that energetic electrons are
accelerated during the ejection and coalescence of multiple plasmoids in
the flare current sheet.</description>
</item>
<item>
<title> Delay of Near-relativistic Electrons with Respect to Type III Radio Bursts throughout the Inner Heliosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...980...96M</link>
<description>Energetic electrons accelerated by solar eruptive events are frequently
observed to have inferred injection times that appear significantly
delayed with respect to electromagnetic emission including type III
radio bursts. This is noteworthy because type III radio emission is
produced by streaming suprathermal electrons, and thus this observed
delay implies either a delayed injection/release of higher-energy
electrons, compared with the suprathermal population, and/or a delay of
the electrons observed in situ in transit through the interplanetary
medium. A number of studies have investigated these delays with
spacecraft located at 1 au. In this study, we examine energetic electron
onsets and type III radio bursts observed by the Integrated Science
Investigation of the Sun (ISIS) and the FIELDS Radio Frequency
Spectrometer instrument on Parker Solar Probe at a variety of
heliocentric distances. With these observations, we can uniquely
decouple the effects of acceleration and transport and shed light on the
source of these delays. We present a survey of electron events observed
by ISIS within the first 6 yr of the mission, including their delays
with respect to type III emission between 0.1 and 0.8 au. These results
suggest that energetic electron delays with respect to type III radio
bursts are not purely produced by a delayed injection/release as has
been suggested, implying that transport processes play a role.</description>
</item>
<item>
<title> ALMA Observations of Solar Spicules in a Polar Coronal Hole</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...980...60B</link>
<description>We report observations of solar spicules at millimeter wavelengths
(mm-) using the Atacama Large Millimeter/submillimeter Array (ALMA).
These are supplemented by observations in optical, ultraviolet (UV), and
extreme ultraviolet (EUV) wavelengths. The observations were made on
2018 December 25 of the northern polar coronal hole. ALMA obtained time-
resolved imaging observations at wavelengths of 3 mm (100 GHz; 2 s
cadence) and 1.25 mm (239 GHz; 2 minutes cadence) with an angular
resolution of 22  13 and 15  07, respectively. Spicules observed at
mm- are easily seen low in the chromosphere whereas spicules in UV
bands are seen to extend higher. The spicules observed at mm- are seen
in absorption against coronal EUV emission, allowing us to estimate the
column depth of neutral hydrogen. Spicular emission at mm-, due to
thermal freefree radiation, allows us to estimate the electron number
density as a function of height. We find that spicule densities,
inferred from the mm- data are uniquely insensitive to assumptions
regarding the temperature of plasma in spicules. We suggest that the
upward mass flux carried by spicules is unlikely to play a significant
role in the mass budget of the solar corona and solar wind, and the
transport of hot material into the corona by spicules may not play a
significant role in coronal heating. However, the possibility that
electric currents, fast kink and torsional waves, or other wave modes
carried by spicules may play a role in transporting energy into the
solar corona cannot be excluded.</description>
</item>
<item>
<title> Constraining Solar Emission Radius at 42 MHz During the 2024 Total Solar Eclipse Using a Student-commissioned Radio Telescope</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...979..203Y</link>
<description>Low-frequency solar radio emission is sourced in the solar corona, with
sub-100 MHz radio emission largely originating from the 10&lt;SUP&gt;5&lt;/SUP&gt;
K plasma around 2 optical radii. However, the region of emission has yet
to be constrained at 3545 MHz due to both instrumentation limitations
and the rarity of astronomical events, such as total solar eclipses,
which allow for direct observational approaches. In this work, we
present the results from a student-led project to commission a low-
frequency radio telescope array situated in the path of totality of the
2024 total solar eclipse in an effort to probe the middle corona. The
Deployable Low-Band Ionosphere and Transient Experiment (DLITE) is a
low-frequency radio array comprised of four dipole antennas, optimized
to observe at 3545 MHz, and capable of resolving the brightest radio
sources in the sky. We constructed a DLITE station in Observatory Park,
a dark-sky park in Montville, Ohio. Results of observations during the
total solar eclipse demonstrate that DLITE stations can be quickly
deployed for observations and provide constraints on the radius of solar
emission at our center observing frequency of 42 MHz. In this work, we
outline the construction of DLITE Ohio and the solar observation results
from the total solar eclipse that transversed North America in 2024
April.</description>
</item>
<item>
<title> Maximum Energy of Particles in Plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...979..161O</link>
<description>Particles are accelerated to very high, nonthermal energies in space,
solar, and astrophysical plasma environments. In cosmic-ray physics, the
Hillas limit is often used as a rough estimate (or the necessary
condition) of the maximum energy of particles. This limit is based on
the concepts of one-shot direct acceleration by a system-wide motional
electric field, as well as stochastic and diffusive acceleration in
strongly turbulent environments. However, it remains unclear how well
this limit explains the actual observed maximum energies of particles.
Here, we show, based on a systematic review, that the observed maximum
energy of particlesthose in space, solar, astrophysical, and laboratory
environmentsoften reach the energy predicted by the Hillas limit. We
also found several exceptions, such as electrons in solar flares and
jet-terminal lobes of radio galaxies, as well as protons in planetary
radiation belts, where deviations from this limit occur. We discuss
possible causes of such deviations, and we argue in particular that
there is a good chance of detecting ultra-high-energy (100 GeV) solar
flare electrons that have not yet been detected. We anticipate that this
study will facilitate further interdisciplinary discussions on the
maximum energy of particles and the underlying mechanisms of particle
acceleration in diverse plasma environments.</description>
</item>
<item>
<title> Evaluating F10.7 And F30 Radio Fluxes As Long-Term Solar Proxies Of Energy Deposition In The Thermosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AnGeo..43..175Q</link>
<description>We use model simulations and observations to examine how well the F10.7
and F30 solar radio fluxes have represented solar forcing in the
thermosphere during the last 60 years of weakening solar activity. We
found that increased saturation of radio fluxes during the last two
extended solar minima leads to an overestimation of solar energy
deposition, which manifests as a change in the linear relation between
thermospheric parameters and F10.7. On the other hand, the linear
relation between thermospheric parameters and F30 remains nearly the
same throughout the whole studied period because of a recently found
relative increase of F30 with respect to F10.7. This explains the
earlier finding that F30 correlates better with several ionospheric and
thermospheric parameters than F10.7 during recent decades. We note that
continued evaluation is needed to see how well F10.7 and F30 will serve
as solar proxies in the future when solar activity may start increasing
toward the next grand maximum.</description>
</item>
<item>
<title> Fine structures of a solar type III radio bursts observed with LOFAR</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AcGeo..73..987D</link>
<description>We present spectral and imaging LOFAR (LOw-Frequency ARray) observations
in the 20 - 40 MHz range of solar radio bursts fine structures, such as
flag-like, sail-like, and dot-like that appeared on 8 April 2019. These
structures were associated with type III solar radio bursts that
occurred in the 40 - 80 MHz band. The mean duration and spectral widths
of the fine structures range from 1.0 to 3.4 s and from 0.3 to 0.9 MHz,
respectively. Additionally, we investigated the radio images of eight
fine structures - two flags, two sails and four dots. This allowed us to
determine their emission source sizes, which ranged from 240 to 392
arcmin2, and their frequencies from 25.58 to 39.25 MHz as well as their
location. They occurred on the east side of the Sun and were most likely
associated with an emerging active region NOAA AR 12738, where a weak
B1.7 flare was observed.</description>
</item>
<item>
<title> Based on X-ray, EUV (DEM analysis), and type-III radio burst observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...694A.188B</link>
<description>Context. In solar flares, non-potential magnetic field energy is
transferred to particle acceleration, heating, and radiation. Multi-
wavelength observations of the solar corona in extreme ultraviolet (EUV)
and X-ray show the consequences of magnetic reconfiguration in lower
heights, while radio observations contain information about the access
of flare-accelerated electrons to greater heights in the solar
atmosphere. Signs of downward and upward particle propagation do not
always appear symmetrically, they depend on the acceleration process,
the sensitivity of the instruments, and the magnetic connectivity. The
magnetic connectivity in various flare phases is therefore a key element
to study in order to gain a better understanding of combined flare
observations. Aims. We aim to draw conclusions about the magnetic
connectivity of specific coronal loops in the active region, the
acceleration region, and the higher corona with respect to different
phases of the flare process. Methods. We investigate the evolution of
particle acceleration, loops heated by the energy release, and the
trajectories of flare-accelerated electrons observed up to one solar
radius (1 R&lt;SUB&gt;S&lt;/SUB&gt;) above the active region in a B-class flare on 6
June 2020. We studied the downward particle acceleration and thermal
evolution with observations by the Spectrometer/Telescope for Imaging
X-rays and with a reconstruction code based on EUV observations. Traces
of flare-accelerated electrons, namely, type-III radio bursts, were
investigated with a spectroscopic solar dynamic radio imager (LOw
Frequency ARray). The radio source positions in heights of 0.4
R&lt;SUB&gt;S&lt;/SUB&gt;1.0 R&lt;SUB&gt;S&lt;/SUB&gt; were compared with the thermal evolution
of coronal loops and with a solar magnetic field model. Results. In this
flare event, similar magnetic reconnection processes and accompanied
heating processes are triggered several times. For loops and periods
with access to the higher corona, type-III bursts from similar
reconnection process are emitted along similar propagation trajectories.
There are no radio bursts associated with the heating process of the
main flaring loop. Conclusions. In this event, the large-scale magnetic
field is rather stable and seems not to be affected by the flare. The
access to loops reaching heights of half a solar radius or more is
suppressed during the main flare phase for flare-accelerated electrons.
This may lead to more effective heating and absent type-III radio bursts
between 20 MHz and 85 MHz.</description>
</item>
<item>
<title> Connecting energetic electrons at the Sun and in the heliosphere through X-ray and radio diagnostics</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...694A.111P</link>
<description>Context. Solar flares release huge amounts of energy, a considerable
part of which is channeled into particle acceleration in the lower
corona. Hard X-ray (HXR) emissions are used to diagnose the accelerated
electrons that bombard the chromosphere, while type III radio bursts
result from energetic electron beams propagating through the corona and
into interplanetary space. The Solar Orbiter mission, launched in 2020,
aims to link solar flare remote observations with heliospheric events,
thus producing useful observations for our understanding of particle
acceleration and propagation from the Sun to the heliosphere. Aims.
While both hard X-Ray and radio emissions result from flare-accelerated
electrons, their relationship is not straightforward. By comparing the
evolution of the X-ray emitting sites and the timing of type III bursts,
our aim is to determine the conditions for associations between X-ray
flares and interplanetary (IP) type III bursts. Methods. We analyzed 15
interplanetary type III bursts that are associated with HXR bursts in
the first available period for simultaneous X-ray/radio observations of
type III bursts from Solar Orbiter (using the RPW and STIX instruments).
X-ray imaging was performed around the onset of the type III bursts,
complemented by EUI 174  images to assess the magnetic configuration of
the corona. Results. All 15 X-ray flares originated from the same active
region on the west limb as observed by Solar Orbiter. In each of the
events, a change in X-ray source morphology occurred shortly (&lt; 6
minutes) before the onset of type III radio bursts, indicating a change
in the electron acceleration region preceding the radio emission.
Considering the delays observed between the two emissions, these
findings describe complex scenarios with multiple reconnection episodes,
some of which may allow accelerated electrons to escape into IP space
when open magnetic field lines are involved (interchange reconnection).
In some cases, X-ray source elongations toward open field lines in the
UV were observed, reinforcing this idea.</description>
</item>
<item>
<title> The widespread solar energetic particle event on 2022 January 20</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...694A..64R</link>
<description>Context. On 2022 January 20, the Energetic Particle Detector (EPD) on
board Solar Orbiter measured a solar energetic particle (SEP) event
showing unusual first arriving particles from the anti-Sun direction.
Near-Earth spacecraft separated by 17 in longitude to the west of Solar
Orbiter measured classic anti-sunward-directed fluxes. STEREO-A and
MAVEN, separated by 18 to the east and by 143 to the west of Solar
Orbiter, respectively, also observed the event, suggesting that
particles spread over at least 160 in the heliosphere. Aims. The aim of
the present study is to investigate how SEPs are accelerated and
transported towards Solar Orbiter and near-Earth spacecraft, as well as
to examine the influence of a magnetic cloud (MC) present in the
heliosphere at the time of the event onset on the propagation of
energetic particles. Methods. We analysed remote-sensing data, including
flare, coronal mass ejection (CME), and radio emission to identify the
parent solar source of the event. We investigated energetic particles,
solar wind plasma, and magnetic field data from multiple spacecraft.
Results. Solar Orbiter was embedded in a MC erupting on 16 January from
the same active region as that related to the SEP event on 20 January.
The SEP event is related to a M5.5 flare and a fast CME-driven shock of
1433 km s&lt;SUP&gt;1&lt;/SUP&gt;, which accelerated and injected particles within
and outside the MC. Taken together, the hard SEP spectra, the presence
of a Type II radio burst, and the co-temporal Type III radio burst being
observed from 80 MHz that appears to emanate from the Type II burst,
suggest that the shock is likely the main accelerator of the particles.
Conclusions. Our detailed analysis of the SEP event strongly suggests
that the energetic particles are mainly accelerated by a CME-driven
shock and are injected into and outside of a previous MC present in the
heliosphere at the time of the particle onset. The sunward-propagating
SEPs measured by Solar Orbiter are produced by the injection of
particles along the longer (western) leg of the MC still connected to
the Sun at the time of the release of the particles. The determined
electron propagation path length inside the MC is around 30% longer than
the estimated length of the loop leg of the MC itself (based on the
graduated cylindrical shell model), which is consistent with the low
number of field line rotations.</description>
</item>
<item>
<title> Correlation between active regions' spectra at high radio frequencies and solar flare occurrences</title>
<link>https://ui.adsabs.harvard.edu/abs/2025NatSR..1544237M</link>
<description>High radio frequencies observations with the Italian network of large
single-dish radio telescopes resulted in &lt;tex-math
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\begin{document}$$$$]]&gt;&lt;/tex-math&gt;450 solar images between 2018 and
2023 in K-band frequency range (18-26 GHz). Solar radio mapping at these
frequencies allows the probing of the Active Regions (ARs) chromospheric
magnetic field close to the Transition Region, where strong flares and
coronal mass ejection events occur. Enhanced magnetic fields up to
1500-2000 G determine anomalous spectra in the ARs brightness compared
to pure free-free emission, due to the addition of a steeper gyro-
resonance component also associated with circular polarisation up to
&lt;tex-math id="IEq2_TeX"&gt;&lt;![CDATA[\documentclass[12pt]{minimal}
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\begin{document}$$$$]]&gt;&lt;/tex-math&gt;40%. When a significant AR spectral
flattening is detected, the probability of a strong flare occurrence
within &lt;tex-math id="IEq3_TeX"&gt;&lt;![CDATA[\documentclass[12pt]{minimal}
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\begin{document}$$$$]]&gt;&lt;/tex-math&gt;30 hours is high (&lt;tex-math
id="IEq4_TeX"&gt;&lt;![CDATA[\documentclass[12pt]{minimal}
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\begin{document}$$$$]]&gt;&lt;/tex-math&gt;89% in terms of statistical
precision). Despite an approximate weekly cadence of our observations,
only &lt;tex-math id="IEq5_TeX"&gt;&lt;![CDATA[\documentclass[12pt]{minimal}
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\begin{document}$$$$]]&gt;&lt;/tex-math&gt;12% of strong flares are
missed/unpredicted within this time interval. Through a correlation
analysis, we assess the trade-off on the sensitivity and the robustness
of this physics-based flare forecast method.</description>
</item>
<item>
<title> Long-term trends of ionospheric electron density related to global warming</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JSWSC..15...56J</link>
<description>Long-term trends of ionospheric electron density have been studied using
vertical sounding measurements at 10 ionosonde stations from European,
Asian, and American longitude sectors. The analysis focuses on studying
the relationship of ionospheric F2 layer noontime peak electron density
(NmF2) data covering a long time period of up to 71 years with the 30 cm
solar radio flux index F30. The long-term behavior of 11-year sliding
averages of noontime NmF2 data shows a substantial decrease from a
stable reference level that is specific for each ionosonde station. The
reference level is defined by a linear model of the noontime F2 layer
11-year sliding peak electron density NmF2* as a function of the
associated 11-year sliding F30 solar activity index F30*. Whereas NmF2*
is proportional to F30* within a small variability range of  1.5% over
nearly two solar cycles until 1982, NmF2* decouples from this linear
relationship with F30* afterwards. The deviation (reduction) may reach
up to 20.6% in 2022 or up to about 5% per decade in the Northern
hemisphere and up to 18.2% in 2022 or about 4% per decade in the
Southern hemisphere. It is expected that such strong changes should have
serious consequences for the accuracy of empirical ionosphere models
utilizing a database that was established before the 1980s. For the
first time, it has been demonstrated that there is a significant
correlation between the observed long-term decrease in ionospheric
electron density and the temperature anomaly (TA) measured at the
Earth's surface. This finding highlights a close connection between
atmospheric changes at lower altitudes, as indicated by surface
temperature records, and variations in the ionospheric electron density
observed over extended periods. Similar to the temperature anomaly (TA),
the concept of "electron density anomaly" (EDA) has been introduced to
characterize deviations in ionospheric electron density from expected
values. Analysis indicates that the EDA exhibits a more pronounced
effect in the Northern Hemisphere compared to the Southern Hemisphere. A
similar pattern occurs with the TA, which supports the idea that a
shared physical mechanism may explain both the EDA and TA phenomena.
This long-term reduction of the electron density reflects ongoing
modifications in the structure and behavior of the Earth's
magnetosphere-ionosphere-thermosphere (MIT) system. The findings suggest
that these changes are closely linked to the increasing concentrations
of greenhouse gases accumulating in the thermosphere. As greenhouse gas
levels rise, their effects extend beyond the lower atmosphere, impacting
the upper atmospheric regions and contributing to observable trends in
ionospheric electron density.</description>
</item>
<item>
<title> Theoretical algorithm and its validation</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JSWSC..15...47C</link>
<description>The Soil Moisture and Ocean Salinity (SMOS) satellite, launched in
November 2009, is equipped with the Microwave Imaging Radiometer with
Aperture Synthesis (MIRAS) payload, which collects high temporal
resolution polarimetric data at 1.413 GHz (L-band), corresponding to a
wavelength of 21.2 cm, with a time resolution of 2.4 s. The Sun is
present in the SMOS images as an alias and is removed from the images to
improve the accuracy of soil moisture and ocean salinity maps. This
paper illustrates the algorithm's theoretical basis for the retrieval of
the solar flux from the SMOS dataset at the time scale of 50 min, and
details the validation process and results. Validation and long-term
stability are evaluated at daily and monthly scales, using the radio-
telescopes and other solar activity proxies as references. Comparison
with the F10.7 index and the flux at 1 GHz from the Nobeyama Radio
Polarimeters (NoRP) shows good agreement with the SMOS solar flux
dataset, with no significant seasonal or temporal drift, unlike data
collected by the Radio Solar Telescope Network (RSTN) at 1.415 GHz. The
SMOS solar flux spectrum reveals both the solar rotation and solar cycle
frequencies, resembling the F10.7 index. The uncertainties in the 50 min
time resolution dataset are assessed, and the precision of the daily
data is further evaluated through auto-regressive modelling, comparing
favourably to results obtained by the radio telescopes, with errors
consistently below 3%. The correlation between SMOS solar flux and both
the Wolf sunspot number and the Mg II proxy shows high agreement, and
suggests that the correlation between the SMOS solar flux and the Mg II
is mostly linear, and stronger than the one between the latter and the
F10.7. Lastly, a prototype for solar radio burst detection is
introduced, and a few solar radio burst events are discussed. This work
demonstrates the added value of the SMOS solar flux in solar physics
studies, thanks to its 15-year-long time series dataset and its proven
stability. The full polarimetric measurements acquired in the L-band at
high temporal resolution represent an innovative point of view for solar
flux observations, alleging SMOS solar flux as a valid resource in the
space weather field, complementing established solar indicators and
contributing to Space Weather applications and studies. The SMOS solar
flux at 50 min time resolution dataset is publicly accessible from
Zenodo as daily files.</description>
</item>
<item>
<title> Estimation of the impact of solar flare spectra on the Earth's ionosphere using the GAIA model</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JSWSC..15...10K</link>
<description>The rapid increase in X-ray and extreme ultraviolet (EUV) emissions
owing to solar flares enhances ionization in the ionosphere, increasing
radio wave attenuation. Among these phenomena, the shortwave
communication disturbance caused by the increased electron density in
the ionospheric D region is known as the shortwave fadeout (SWF). We
investigated the relationship between SWF's magnitude and solar flare
emission, and evaluated the electron density variation in the
ionospheric D region associated with flare. We defined the minimum
frequency (fmin) observed in Japan's ionograms as the SWF's magnitude.
We analyzed ionosonde data for 38 SWF events observed during daytime in
Japan between May 2010 and May 2014. To investigate the relationship
between flares and SWF, we compared the observed X-ray and EUV emissions
during flares with the dfmin (background subtracted fmin). X-ray
(0.10.8 nm) and EUV (1114 nm) emissions correlate with dfmin. Then,
using the GAIA model, a numerical model that treats the entire Earth's
atmosphere, we investigated the effect of the X-ray and EUV solar flare
emissions on the ionosphere, which affects the SWF. The results showed
that the main ionization source in the ionospheric D region was X-ray
emission, and shortwaves were attenuated by 90%. In contrast, in the
ionospheric E and F regions, the primary ionization source was EUV
emission, with only 10% shortwave attenuation. Finally, we estimated
the fmin values and blackout (total fadeout of the ionospheric echo
observed in ionograms) and compared the simulated and observed fmin
values. The hit rate of blackouts was 35% when we only used the GAIA
calculations. Therefore, we estimated fmin using the electron density
variation in the ionospheric D region corresponding to X-ray solar
emission. As a result, the hit rate of the blackout was 68%, and the
linear correlation coefficient between the simulated and observed fmin
values was 0.85. The estimated magnitude of the SWF was improved by
incorporating the effects of X-ray emissions into the ionospheric D
region of GAIA. We are the first to implement a method for evaluating
the electron density in the ionospheric D region using the fmin value.</description>
</item>
<item>
<title> Investigating the drivers of long-term trends in the upper atmosphere over Rome across four decades</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JSWSC..15....8S</link>
<description>The nature of the long-term changes in the upper atmosphere morphology
at mid-latitude remains a subject of debate, particularly regarding
whether these changes are purely driven by geomagnetic and solar
activities or whether forcing from the lower atmosphere, such as
CO&lt;SUB&gt;2&lt;/SUB&gt; variations, may play a role. To contribute to this
debate, we investigate the nature of the long-term trends of the
ionospheric and thermospheric parameters by leveraging on ionosonde data
digitally recorded at the Rome Observatory since 1976. The following
parameters have been investigated under sunlit conditions (12:00 Local
Time): critical frequency of the F1 layer (foF1); critical frequency of
the F2 layer (foF2), atomic oxygen concentration at 300 km ([O]); ratio
between atomic oxygen and molecular nitrogen concentrations at 300 km
altitude ([O]/[N&lt;SUB&gt;2&lt;/SUB&gt;]); exospheric temperature (T&lt;SUB&gt;ex&lt;/SUB&gt;);
thermospheric density at 300 km (). The ionospheric parameters are
manually scaled from digital ionograms, whereas thermospheric parameters
are retrieved using the THERmospheric parameters from IONosonde
observations (THERION) method, which utilises ionosonde observations and
a physical model of the ionospheric F region. To investigate the
influence of the solar and geomagnetic activity on long term variations,
we consider the solar radio flux at 10.7 cm (F10.7) and the geomagnetic
disturbance index Ap. To identify the various frequency/period
components of the time series under consideration and identify the
trends, we leverage the high scale/time resolution offered by the Fast
Iterative Filtering (FIF) algorithm. A regression analysis of
thermosphere/ionosphere parameters against geomagnetic/solar activity
indices has then been conducted to investigate the drivers of long-term
variability. Our findings reveal that the identified trends are
predominantly controlled by external drivers, particularly long-term
solar and geomagnetic activity variations. The adopted methodology,
based on regression modelling, demonstrates that variability in F10.7
and Ap accounts for nearly all of the observed changes, with the
exception of atomic oxygen ([O]), which displays a slightly higher
unexplained variability (~7%). The inclusion of CO&lt;SUB&gt;2&lt;/SUB&gt;
concentration as an additional driver improves the regression model for
[O]. However, the effect remains statistically limited, indicating that
the impact of CO&lt;SUB&gt;2&lt;/SUB&gt; on thermospheric cooling might be of little
significance. Further studies with extended time series are necessary to
better quantify this relationship and evaluate its importance. These
results highlight the predominant influence of solar and geomagnetic
activity in determining upper atmosphere long-term trends at mid-
latitudes.</description>
</item>
<item>
<title> Exploring daily fluctuations of cosmic ray muon components at a low latitude site and their associations with space weather variables</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JApA...46...10A</link>
<description>In this study, cosmic rays (CR) data from the King Abdulaziz University
muon detector in Jeddah (Rc = 14.8 GV), Saudi Arabia, were utilized to
investigate the amplitude and phase components of diurnal variations in
CR muons. The data covered the period from 2007 to 2012 and were fitted
using a single cosine function with a 24-h period and two cosine
functions with periods of 24 h and 12 h, respectively. The distributions
of the phases and amplitudes resulting from these fits were analyzed
across different time spans. The findings of this analysis provided
valuable insights into the diurnal characteristics of CR muons. The mean
amplitude and phase obtained from the single fit were reported as 0.11
 0.51% and 11:00  4.30 UT, respectively. Furthermore, employing the
two-cosine fit revealed that the first phase had a mean occurrence time
of 06:00  6.90 UT, accompanied by an amplitude of 0.10  0.62%. The
second phase occurred at 13:00  3.51 UT, with an amplitude of 0.11 
0.25%. The study observed diverse distributions and trends in amplitude
and phase values across different time scales, including months,
seasons, and years. Additionally, the study investigated the influences
of five solar activity parameters on the diurnal CR components using
Pearson linear, non-parametric Spearman, and Kendall correlations. These
parameters included the interplanetary magnetic field, solar wind speed,
Kp index, Dst index, and solar radio flux at 10.7 cm. The results
revealed that the relationships between solar activity variables and the
diurnal CR parameters were not uniform. There were varying degrees of
correlation, with differences in strength and magnitude depending on the
specific variable and correlation coefficient being examined.</description>
</item>
<item>
<title> A Solar-Powered Mobile Phased Array for Radio Astronomy Observations at Low Frequencies</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JAI....1450009B</link>
<description>In this paper, we present initial results from test observations
conducted with a compact, broadband (meter-decameter range) mobile
antenna array designed for autonomous operation in field conditions.
Powered exclusively by solar energy and independent of stationary
infrastructure, the system is rapidly deployable and well-suited for
remote low-frequency (&lt;100 MHz) radio astronomy. Solar radio bursts were
used as illustrative examples to demonstrate system functionality and
sensitivity under natural conditions. In addition to solar activity, the
antenna array is capable of detecting other astrophysical sources such
as Jupiter and Cas A, confirming its broader applicability. Key
technical characteristics of the antenna and its integrated solar power
station are also described.</description>
</item>
<item>
<title> Correlation between rate of TEC index and positioning error during solar flares and geomagnetic storms using navigation with Indian constellation receiver measurements</title>
<link>https://ui.adsabs.harvard.edu/abs/2025JAGeo..19...49S</link>
<description>The real-time position accuracy of the Global Navigation Satellite
System (GNSS)/Navigation with Indian Constellation (NavIC) receiver is
limited by the dynamic behavior of the ionosphere, particularly in
adverse conditions like solar flares and geomagnetic storms. The NavIC
satellites broadcast dual coherent radio beacon signals on L5 (1,164.5
MHz) and S (2,472.5 MHz) bands for providing position, velocity, and
timing services in all weather conditions. The Total Electron Content
(TEC) and Rate of TEC Index (ROTI) are the potential indicators for
characterizing the ionosphere and its irregularities. In this research
work, the TEC and ROTI are computed from the code and carrier phase
observations of the NavIC receiver located at Kurnool low latitude
station (15.79 N, 78.07 E) with geomagnetic coordinates (7.30 N,
151.65 E). This paper presents a statistical study of TEC, ROTI, and
the correlation between ROTI and NavIC positioning error during highly
intense solar flares (X9.3 and X2.2) and geomagnetic storm conditions.
Compared to quiet days mean TEC, the enhancement is 3 TECU due to X9.3
flares, and the maximum peak of TEC on storm day (September 8, 2017) is
80.92 TECU. Moreover, the correlation coefficient between ROTI and
position error is 0.76 on a quiet day (September 4, 2017), 0.54 on an
intense solar flares day (September 6, 2017), and 0.24 on a storm day
(September 8, 2017), this indicates positional accuracy degradation on a
geomagnetic storm day. The outcome of this research work would be
helpful for investigating characteristics of the northern low latitude
ionospheric irregularities and, in turn, useful for developing suitable
ionospheric nowcasting/prediction models for GNSS applications.</description>
</item>
<item>
<title> Radio absorption in the dayside martian ionosphere enhanced by solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2025Icar..42516342H</link>
<description>Solar flares can cause radio absorption in the D region of the Earth's
ionosphere and consequently interrupt high-frequency radio communication
systems, also known as short-wave fadeout or the Dellinger effect. We
present an analogous radio absorption event observed at Mars during a
solar flare. In this event, the Mars Express Mars Advanced Radar for
Subsurface and Ionospheric Sounding (MARSIS) instrument fortuitously
operated at low altitudes on the dayside around the terminator in a
favorable configuration for surface echo measurements at the flare peak.
The surface echo power during the flare is abnormally weak compared to
nominal echo powers at corresponding solar zenith angles, suggesting
flare-induced radio absorption in the dayside lower ionosphere of Mars.
Additionally, long-term MARSIS data statistically demonstrate the radio
absorption dependence on solar soft X-ray fluxes. Our results point to
the need for Martian space weather prediction including ionospheric
effects on radio waves.</description>
</item>
<item>
<title> Joint Optimization for Cooperative Service-Caching, Computation-Offloading, and Resource-Allocations Over EH/MEC 6G Ultra-Dense Mobile Networks</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ITWC...24.5780C</link>
<description>Service-caching, computation-offloading, and mobile edge-computing (MEC)
have been widely recognized as three key 6G mobile wireless neworking
techniques which can efficiently support implementing the ultra-dense
networks (UDNs) with massive small-cell base stations (SBSs). But, these
impose the new challenges for the UDNs to solely rely on grid power for
energy supplying and to jointly optimize service-caching, computation-
offloading, and resource-allocations. To overcome the above described
difficulties, integrating energy-harvesting (EH) techniques with MEC-
enabled 6G UDNs, we propose to develop the joint optimization schemes
for cooperative service-caching, computation-offloading, and resource-
allocations. In our considered UDNs, there exist a large number of EH-
based stationary users (SUs) or mobile users (MUs), and a mixture of on-
grid SBSs powered by electric grid and off-grid SBSs power-supplied by
solar, radio frequency (RF) energy, etc. Specifically, first we
formulate an energy minimization problem under a non-linear RF-energy EH
model to minimize the sum of weighted energy consumption of users and
off-grid SBSs. Second, for scenarios with SUs, we develop a two-
timescale based joint cooperative service-caching, computation-
offloading, and resource-allocations scheme using the hierarchical
multi-agent deep reinforcement learning. We derive cooperative service-
caching in each time frame, and then derive computation-offloading and
resource-allocations in each time slot. Third, we extend our work to
scenarios with MUs, where MUs can move with certain trajectories at low
speeds. Finally, we validate and evaluate the performances of our
proposed schemes through the extensive simulations.</description>
</item>
<item>
<title> Development of an FX Digital Correlator for Millimeter-Wave Solar Radio Interferometry and Calibration of AmplitudePhase Consistency</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ITIM...74T5333Y</link>
<description>Interferometry technology stands out as a significant trend in radio
observation systems, where correlators act as pivotal components
responsible for real-time data processing. Responding to the operational
needs of Shandong University Chashan Solar Radio Observatory's
39.540-GHz solar radio binary interferometer, a 1.25-Gs/s FX-type
digital correlator was developed. Following a modular framework, the
digital correlator comprises three core modules: data acquisition,
correlation processing, and data transmission. Additionally, it
incorporates adjustable delay compensation and amplitudephase
consistency calibration functionalities to ensure precise signal
alignment and system coherence. The coherent noise injection method is
employed to assess inherent amplitudephase discrepancies in the analog
front end (AFE), while real-time compensation calibration factors are
implemented in FPGA to rectify the amplitudephase consistency of the
AFE. Experimental design and validation were executed, showcasing that
the correlator, featuring dual channels, a 1.25-Gs/s sampling rate, and
14-bit resolution, achieves an adjustable delay compensation accuracy of
0.8 ns. Post-amplitudephase consistency calibration of the AFE links
reveals an amplitude error of approximately 0.2 dB and a phase error of
approximately 7, indicating notable calibration efficacy.
Subsequently, the RTL design of the digital correlator presented in this
article was verified, confirming the logical coherence of the RTL design
and validating the accuracy of the correlation output results through
experimental design. The development of this correlator not only finds
application in other interferometric measurement system scenarios but
also establishes a research groundwork for future digital correlator
advancements in the comprehensive aperture solar imager slated for
development by the research group.</description>
</item>
<item>
<title> Enhancing Receiver Linearity Through Behavioral Modeling of Measured Data and Digital Postcompensation Techniques</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ITIM...7446387Y</link>
<description>The challenge of receiver nonlinearity in radio observation systems
results in diminished system linearity, dynamic range, and sensitivity,
particularly in low-amplitude and linear regions. To address these
issues, this article proposes a digital postcompensation calibration
method based on a nonlinear model of radio receivers. By using nonlinear
digital postcompensation technology, we analyze the nonlinear effects
exhibited by radio receivers. A nonlinear model of radio receivers is
constructed using empirical data. The compensation-linearized output is
generated by compensating for the observed input of the radio
observation system's output response through the inverse model of the
nonlinear model. Subsequently, the receiver response compensates for the
difference between the actual radio receiver response and the response
corresponding to linear gain, thereby eliminating nonlinear distortion
and achieving real-time digital postcompensation linearization of these
effects. We introduce a method for modeling the nonlinear behavior of
radio receivers based on empirical data, along with a nonlinear
postcompensation linearization approach rooted in this model.
Experimental validation via radio observation systems reveals a mean
square error of approximately 0.8226% between the model output and the
system response. Furthermore, the nonlinear postcompensation
linearization method, which is based on the nonlinear model of radio
receivers, significantly enhances system linearity, particularly in the
low-amplitude region and nonlinear region. The amplitude response
difference of the system, concerning the quiet sun and cold space,
shifts from approximately 5 dB to approximately 11 dB, thereby
amplifying the sensitivity of the solar radio observation system.</description>
</item>
<item>
<title> A Modern VLF Radio Receiver Designed for the Array for VLF Imaging of the D-Region (AVID)</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ITGRS..63S7146C</link>
<description>Very-low-frequency (VLF) radio waves are commonly used to remotely sense
the D-region ionosphere. In the past few decades, a few prominent
designs for VLF receivers have come to the forefront of the community,
such as the AWESOME receiver developed at Stanford in the early 2000s.
In the last decade, advancements in off-the-shelf electrical components
and the obsoletion of others motivated a redesign of this receiver
system. The result of this receiver design work is presented in this
article with the measured characteristics of over ten complete systems.
The newly operational array for VLF imaging of the D-region (AVID),
incorporating the updated VLF receiver, is also presented. One early
result from AVID is the characterization of the drift rates of the phase
of two VLF transmitters. The NLK transmitter at 24.8 kHz was found to
drift by 0.07886/s /s, while the NML transmitter at 25.2 kHz was found
to drift by 0.07201/s /s. We also show that the transmitted power of
these transmitters can change over time, by up to ~7% in the case of
NLK. Finally, two early case studies are presented, showing AVID's
ability to observe and track: 1) the effects of an M7.2 solar flare on
the D-region ionosphere and 2) the onset of a 333 nT Dst geomagnetic
storm and the D-region's response to it. These case studies demonstrate
the tools necessary for future work incorporating spatial estimation
algorithms to better characterize disturbances to the D-region
ionosphere.</description>
</item>
<item>
<title> The Outlook of Lunar Observation by 1.3-m Wavelength EISCAT_3D Radar With Large Telescope Antennas of Chinese Meridian Project</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ITGRS..63S3152Y</link>
<description>Earth-based radar (EBR) is an important type of remote sensing
instrument for planetary observation. EBR takes advantages in large-
scale imaging swath, high repeatability, great flexibility, and so on.
The upcoming 233-MHz-frequency European Incoherent Scatter Scientific
Association (EISCAT) 3-D radar system will provide important features to
lunar observation as introduced in this study. EISCAT_3D (E3D) radar is
a powerful multistatic radar system. The 1.3-m wavelength wave of E3D
can penetrate deeper, about 30 m below the lunar average surface, which
can reach the second layer, i.e., layer of ejecta. E3D radar supports
dual/quadrature polarimetry, which gives it good flexibility and lower
ambiguity in the inference of scatter's properties. Also, there is less
ambiguity in scattering regimes between icy and nonicy scatters for
1.3-m wavelength than for shorter wavelengths as given from the
simulation results. Besides, the high topographic resolution (which
requires forming interferometric baselines with distant telescope
antennas) of E3D radar along with its penetration depth makes it
possible for detection of sublunarean cavities by signatures of
depression. As a whole, the 1.3-m wavelength 3-D polarimetric imaging of
the Moon by E3D radar, on a spatial resolution of about 200 m, will be
valuable for obtaining new information about the geology and subsurface
structure of the Moon and can be used in search of buried water ice,
sublunarean cavity, and so on. Furthermore, we envision the
collaboration of E3D radar with large telescope antennas in China,
including Daocheng Solar Radio Telescope (DSRT) and Mingantu spectral
radioheliograph (MUSER) for better imaging ability and detectivity.</description>
</item>
<item>
<title> Frequency-Scanning Waveguide Antenna for Solar Radio Bursts Detection in the UHF Band</title>
<link>https://ui.adsabs.harvard.edu/abs/2025IOJAP...6.1535G</link>
<description>This paper proposes a frequency-scanning antenna designed to operate in
the 400 MHz to 800 MHz band for solar radio astronomy applications. It
is constructed with perforated metallic walls and cylinders, that form a
rectangular leaky waveguide. By adjusting the metallic cylinders in the
appropriate subwavelength holes, the scanning angle of the directive
beams and directivity can be effectively controlled while assuring high
radiation efficiency and gain. Unlike previous leaky waveguides, the
proposed design allows manual tuning of both the leaky-mode phase and
the leakage factors. A 2-meter-long antenna prototype has been
fabricated, and the measurement results show an angular scanning range
from 70 to 30 above the horizon, with a peak gain of 14 dBi and
radiation efficiency exceeding 70% over the entire scanning band. The
application of this antenna to detect solar radio bursts without the
need for Sun tracking is demonstrated.</description>
</item>
<item>
<title> Passive Radar Sounding for Firn Aquifer Monitoring</title>
<link>https://ui.adsabs.harvard.edu/abs/2025IJSTA..1827399P</link>
<description>Firn aquifers may play an important role in the mass balance of the
Greenland ice sheet, but changes in their water storage are challenging
to measure due to their spatiotemporal variability. Here, we explore the
feasibility of passive radar sounding using the Sun as a radio source to
monitor daily to seasonal changes in the firn aquifer water table level.
Our simulations account for time-varying environmental factors (e.g.,
changes in firn temperature, structure, and saturation, as well as snow
accumulation) that impact passive radar measurements of height
fluctuations in the firn aquifer water table. Our results suggest that
passive sounding could be a novel observational tool for quasi-
continuous, seasonal monitoring of firn aquifer properties in polar
regions of interest, such as the Helheim firn aquifer on the Greenland
ice sheet and firn aquifers on Antarctic ice shelves. We conclude by
discussing the opportunities and challenges of near-surface passive
radar sounding, with the goal of enabling low-resource, low-cost
glaciological sensors that complement existing observational tools.</description>
</item>
<item>
<title> Classification of Equatorial Ionospheric Irregularities Using Unsupervised Machine Learning Based on Spatiotemporal ROTI Keograms</title>
<link>https://ui.adsabs.harvard.edu/abs/2025IJSTA..1821769M</link>
<description>Equatorial ionospheric irregularities, particularly those associated
with equatorial plasma bubbles (EPB), can significantly disrupt
satellite navigation and communication systems. As the demand for
reliable Global Navigation Satellite System (GNSS) and communication
services grows, the prediction of ionospheric irregularities becomes
critical. A key step in the prediction process is to identify distinct
spatiotemporal patterns of irregularities, including day-to-day,
longitudinal, and seasonal variations. However, with large datasets,
manually classification or identification of these irregularities is a
complex and challenging task. In this work, we propose unsupervised
machine learning techniques to recognize and group irregularity patterns
in large, unlabeled Rate of Total Electron Content (TEC) Index (ROTI)
keograms. Specifically, two machine learning models: Gaussian Mixture
Model and k-means clustering are employed. The ROTI keograms are
constructed using GNSS data from two low-latitude receiver stations in
Thailand. To reduce redundancy in the keogram images, three feature
extraction techniques are applied before the clustering process. A
comparative analysis is performed to determine the optimal number of
clusters using these models. Based on the results, the optimal
combination of feature extraction and clustering technique is determined
for the proposed clustering model. The resulting k-means model with
contour extractor classifies five distinct patterns of ionospheric
irregularity patterns, providing valuable insights for enhancing EPB
prediction models and deepening our understanding of ionospheric
dynamics. Furthermore, these five irregularity patterns are analyzed in
relation to space weather parameters such as the solar radio flux index
(F10.7), and the geomagnetic index (Kp). The findings contribute to the
development of robust prediction models, improving the reliability of
satellite-based communication and navigation systems.</description>
</item>
<item>
<title> Analysis of the Variability of Diurnal Profiles of Critical foF2 Frequencies in the Light of Solar Radiation</title>
<link>https://ui.adsabs.harvard.edu/abs/2025IJGeo202568818K</link>
<description>This present article was written to analyze the variability of the
diurnal profiles of the critical foF2 frequencies in the light of solar
radiation based on in situ measurements of the ionosonde stations of
Dakar (latitude 14.8 N, longitude 342.6 E) and Ouagadougou (latitude
12.5 N, longitude 358.5 E), respectively, for Sunspot Cycles 21 and
22. The objective being to deduce interpretations in terms of propensity
to occur on the five profiles B, M, R, D, and P referenced to occurrence
between the latitudes of 20 N and 20 S. Thus, on the analyses of
conjunctions in phases or in phase shift observed in the variation of
the sunspot cycle (VSC) and monthly foF2 frequencies (MFVs), we will
note the following: (1) during periods of geomagnetic calm, (a) a
propensity for the formation of the R profile during the growth phases
of the solar cycle and during the periods from the solstices to the
equinoxes and this is due to the conjunction in the growthgrowth phase
between VSC and MFV; (b) a propensity for the formation of the M profile
during the waning phases of the solar cycle and during the periods from
the equinoxes to the solstices and this is due to the conjunction in the
waningdecaying phase between VSC and MFV; (c) a propensity for the
formation of profiles B, D, and P on the one hand during the growth
phases of the solar cycle and during the periods from the equinoxes to
the solstices and on the other hand during the waning phases of the
solar cycle and during the periods from the solstices to the equinoxes
and all these are due to the nonconjunction in the phase between VSC and
MFV. It therefore appears that out of the 16 possible propensities for
profile formations, the R and M profiles are each counted for 12.5%.
Profiles B, P, and D each counted 25%. (2) During periods of geomagnetic
disturbances, notably by SFEs, CMEs, or ionization losses, a profile can
transform into one or other of the other four profiles. Finally, as an
importance or application of this study, we note that (a) foF2
contributes more to the good knowledge of the ionosphere; (b) using the
diurnal profiles of foF2, we could a priori identify periods of lulls in
radio or satellite transmission; (c) by induction, we could count the
solar flares during the day; and (d) the proposed mathematical model is
a basic tool for analyzing foF2 variability.</description>
</item>
<item>
<title> Modeling the transport and anisotropy of energetic electrons in solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2025FrASS..1110579K</link>
<description>Transport of energetic electrons in the flare loop is important to
understanding nonthermal emissions in solar flares. In this work, we
model the propagation of electrons by numerically solving the particle
transport equation which includes the physics of magnetic mirroring and
turbulent pitch-angle diffusion. We find that both the fractions of
electrons trapped in the looptop and precipitating into the solar
surface display a non-monotonic behavior with increasing scattering
rate. In the moderate diffusion regime, the precipitation fraction is
highest and we expect intense nonthermal HXR and microwave emissions at
the footpoints. With no or weak pitch-angle scattering, the velocity
space distribution can be highly anisotropic both in the looptop and
loopleg regions. Different patterns of stripes with positive gradients
in the perpendicular direction can drive the electron cyclotron maser
instability with higher efficiency than the classical loss-cone
distribution, facilitating the excitation of coherent solar radio
bursts. Our simulation results highlight the effects of turbulent pitch-
angle scattering on electron trap/precipitation and anisotropic
distribution in solar flares, which may help us understand the
precipitation of magnetospheric electrons accounting for the aurora as
well.</description>
</item>
<item>
<title> Analysis of 42 Years of Cosmic Ray Measurements by the Neutron Monitor at Lomnick tt Observatory</title>
<link>https://ui.adsabs.harvard.edu/abs/2025E&amp;SS...1203656K</link>
<description>The correlation and physical interconnection between space weather
indices and cosmic ray flux has been well-established with extensive
literature on the topic. Our investigation is centered on the
relationships among the solar radio flux, geomagnetic field activity,
and cosmic ray flux, as observed by the Neutron Monitor at the Lomnick
tt Observatory in Slovakia. We processed the raw neutron monitor data,
generating the first publicly accessible data set spanning 42 years. The
curated continuous data are available in.csv format in hourly resolution
from December 1981 to July 2023 and in minute resolution from January
2001 to July 2023 (Institute of Experimental Physics SAS, 2024,
https://doi.org/10.5281/zenodo.10790915). Validation of this processed
data was accomplished by identifying distinctive events within the data
set. As part of the selection of events for case studies, we report the
discovery of TGE-s visible in the data. Applying the Pearson method for
statistical analysis, we quantified the linear correlation of the data
sets. Additionally, a prediction power score was computed to reveal
potential non-linear relationships. Our findings demonstrate a
significant anti-correlation between cosmic ray and solar radio flux
with a correlation coefficient of 0.74, coupled with a positive
correlation concerning geomagnetic field strength. We also found that
the neutron monitor measurements correlate better with a delay of 721
hr applied to the geomagnetic field strength data. The correlation
between these data sets is further improved when inspecting periods of
extreme solar events only. Lastly, the computed prediction power score
of 0.22 for neutron flux in the context of geomagnetic field strength
presents exciting possibilities for developing real-time geomagnetic
storm prediction models based on cosmic ray measurements.</description>
</item>
<item>
<title> Machine Learning Solar Full Disk Flare Operational Forecasting</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ChJSS..45...82L</link>
<description>Solar flare forecasting is an essential component in space environment
forecasting. Most of the deep learning flare forecasting models
constructed are based on the magnetograms of active regions. Affected by
the projection effect, these models can only forecast the active region
in the center of the Sun. It is difficult to meet the need of
operational flare forecasting of the solar full disk. Based on the
traditional solar activity parameters, in this study, the relationships
between the magnetic type of the active region, area of the active
region, the history of the flare outburst, the 10 cm radio flux and
flares from January 1996 to December 2022 were statistically analyzed.
By using the fully connected neural network, an operational flare
forecasting model for solar full disk active regions was constructed.
This model can forecast the eruption of the M-class or above flares of
the full solar disk active regions in the next 48 h. The F1 score of the
model is 0.4304, the TSS is 0.3689, and the HSS is 0.3906. The model is
compared with the deep learning flare forecasting model constructed in
the previous work, and the results show that the operational forecasting
model constructed in this paper has a better forecasting performance.
Meanwhile, in order to explore the influence of the projection effect,
the solar full disk active regions flare forecasting model constructed
was tested for test data within 30 degrees from the center of the solar
disk, within the interval from 30 degrees to 60 degrees, and over 60
degrees, respectively. The results show that the projection effect has
little influence on the flare forecast model constructed in this study.
The model can be used to forecast flare in the active region of the full
solar disk, and provide an effective tool for operational solar flare
forecasting.</description>
</item>
<item>
<title> Simulation on the Mechanism of Harmonic Maser Emission Through the Wave Coalescence Process</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ChJSS..45...56L</link>
<description>Electron Cyclotron Maser Emission (ECME) driven by electrons with loss-
cone distribution is the main mechanism for explaining solar radio
spikes. However, in strongly magnetized plasmas, the losscone-driven
ECME mainly generates fundamental X mode emissions, which can be
efficiently absorbed when escaping through the second-harmonic layer in
the solar corona. To solve the "escaping difficulty, recent studies
suggested a new mechanism of harmonic maser emission (X2) involving
nonlinear wave coupling process of Z-mode and fundamental X-mode (X1)
waves (Z+ZX2, Z+X1X2). It is necessary to verify the nonlinear wave
coalescence process with theoretical analyses and numerical simulations.
Here, the possibility of a nonlinear wave coupling process is examined
via solving the matching conditions for three-wave resonant interaction
based on the dispersion relation of cold plasma in magneto-ionic
theory.The matching conditions for the Z and/or X1 waves were found to
be satisfied over a wide range of parameters, leading to the production
of X2 emissions that propagate perpendicularly and obliquely relative to
the direction of the background magnetic field. Based on the solutions
obtained in the matching condition analysis, we selected four sets of
solutions of Z+Z and Z+X1 to perform particle-in-cell simulations using
wave pumping method, to verify the nonlinear process of wave coalescence
generating second harmonic X-mode emissions. With X1 and/or Z modes
correctly pumped in the simulation domain, efficient generation of X2
emissions was observed, with saturation achieved within 400
&lt;SUB&gt;ce&lt;/SUB&gt;&lt;SUP&gt;-1&lt;/SUP&gt;. The conversion rate of energies of X2
emissions to Z mode waves varies from 2% to 8%. The study presents
strong evidence to support the new mechanism of harmonic maser emission,
which can be widely applied to explain the solar and space radio
emissions.</description>
</item>
<item>
<title> Research on F10.7 Index Prediction Based on Factor Decomposition and Feature Enhancement</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..276...28Y</link>
<description>The F10.7 index is crucial for assessing solar activity, significantly
impacting communication, navigation, and satellite operations. The
intrinsic complexity and variability of solar activity often result in
sudden perturbations in the F10.7 index, compromising the accuracy and
stability of forecasts. To address this challenge, we propose a novel
prediction strategy that separately forecasts fundamental trends driven
by the medium-to-long-term evolution of the solar cycle and the 27 day
rotational modulation, along with transient disturbances caused by solar
flares and the rapid evolution of active regions. These forecasts are
then integrated to enhance overall prediction accuracy. We incorporate
additional features such as the soft X-ray flare index
(FI&lt;SUB&gt;SXR&lt;/SUB&gt;), magnetic type of the active region (new_Mag), and
X-ray background flux (XBF) to enhance the understanding of the
underlying physical processes of solar activity. Our experiments,
conducted using advanced forecasting models on the SG-F10.7-All data
set, validate the efficacy of our proposed strategy. Notably, the
iTransformer model demonstrates superior performance in both short-term
and medium-term forecasting scenarios. The inclusion of
FI&lt;SUB&gt;SXR&lt;/SUB&gt;, new_Mag, and XBF significantly improves forecasting
accuracy, highlighting their importance in improving the F10.7 index
predictions. Our method outperforms international models from the Space
Weather Prediction Center, British Geological Survey, and Collecte
Localisation Satellites, exhibiting greater accuracy and adaptability
across various solar activity phases. This finding provides a novel
approach for precise forecasting of the F10.7 index.</description>
</item>
<item>
<title> A Study of Real-time Detection Methods for Solar Radio Burst Identification</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJS..276...18Y</link>
<description>Solar flares, coronal mass ejections, and other solar radio burst
phenomena release substantial amounts of solar radiation energy,
resulting in adverse space weather conditions and posing significant
hazards in space. Spectrum analysis conducted manually or with
traditional image processing algorithms is limited by low efficiency and
accuracy. This paper investigates solar radio burst detection methods
and their applications. Five solar radio burst detection
methodsContinuous-3, Sum Flux-3, Continuous Slope, Sum Flux Slope,
and Sum Flux Continuous-3are developed and validated using data from
the Japanese NoRP and the Australian Learmonth Solar Radio Observatory.
The results show that all five methods can detect solar radio bursts to
some degree. Considering the combined metrics of success rate, false
detection rate, and real-time performance, the Sum Flux Continuous-3
method is deemed the optimal method among the five. Additionally, the
Sum Flux Slope method, which is not reliant on historical data,
demonstrates superior universality. Finally, we implement the Sum Flux
Slope method on a 39.540 GHz two-element interferometer, achieving
real-time solar radio burst detection in the upper computer software.
The method also includes functionalities for email alerts, burst
information recording, and control parameter adjustment, confirming its
effectiveness and practicality. Test results demonstrate the method's
effectiveness in real-time solar radio burst detection.</description>
</item>
<item>
<title> Type IV-like Solar Radio Burst Consisting of a Series of Short-time Bursts Observed by PSP</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...979...22M</link>
<description>Solar and interplanetary radio bursts can reflect the existence and
motion of energetic electrons and are therefore a kind of vital
phenomenon in solar activities. The present study reported a solar radio
storm observed by the Parker Solar Probe (PSP) in its eighth orbital
encounter phase, and it lasted about 20 hr in a frequency range of
0.515 MHz, called the type IV-like burst. It consists of a series of
numerous short-time (ST) bursts with the central frequency drifting
slowly from ~5 to ~1 MHz, and each individual ST burst appears at a much
faster frequency drifting rate and has a typical frequency range of a
few MHz and a short duration of about 14 minutes. Based on the
empirical models of the solar atmosphere adopted commonly, combining the
in situ measurement by PSP, we analyzed and compared some possible
mechanisms for the generation of these small-scale ST bursts and
proposed that they were generated probably by a group of solitary
kinetic Alfvn waves (SKAWs) in a magnetic loop accompanying coronal
mass ejection and slowly moving outward, in which the frequency drifting
of individual ST burst is caused by the SKAW's propagation and the
central frequency drifting may be attributed to the motion of the
magnetic loop.</description>
</item>
<item>
<title> Emission Characteristics of Energetic Electrons with Crescent-shaped Velocity Distributions</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...978..134Y</link>
<description>Solar flares release magnetic energy through reconnection, accelerating
electrons into nonthermal velocity distributions, including crescent-
shaped electron populations. These energetic electron distributions are
crucial in driving instabilities that can lead to distinct
electromagnetic emissions. This study investigates the emission
properties of crescent-shaped electron velocity distribution functions
under different frequency ratios (&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;),
critical for understanding plasma conditions in various astrophysical
environments, by comparing the emissions and intensities of waves among
different cases. Here, we study and analyze three distinct frequency
ratio conditions (2.2, 10, and 1, designated as cases A, B, and C,
respectively). We find that the beam-Langmuir and upper-hybrid modes can
be efficiently excited, leading to further plasma emissions in different
cases. Our study reveals that the fundamental (O/F) emission can reach a
maximum value of 10&lt;SUP&gt;4&lt;/SUP&gt;E&lt;SUB&gt;k0&lt;/SUB&gt;, while the harmonics (H)
can extend to 1.5  10&lt;SUP&gt;5&lt;/SUP&gt;E&lt;SUB&gt;k0&lt;/SUB&gt;, depending on the
frequency ratio of the environment. The intensity of the fundamental
mode exceeds previous findings for pure-ring, pure-beam, and ringbeam
distributions, highlighting the impact of crescent-shaped electron
velocity distributions on wave excitation and emission processes. This
effect is notably influenced by different frequency ratios, offering new
insights into the way that nonthermal electron distributions affect the
plasma emission process.</description>
</item>
<item>
<title> Magnetic Field Geometry and Anisotropic Scattering Effects on Solar Radio Burst Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ApJ...978...73C</link>
<description>The fine structures of solar radio bursts reveal complex dynamics in the
corona, yet the observed characteristics of these subsecond bursts are
additionally complicated by radio wave scattering in the turbulent solar
corona. We examine the impact of anisotropic turbulence in radio wave
propagation simulations with nonradial magnetic field structures in
shaping the morphology, time characteristics, and source positions of
fine structures. The apparent sources are found to move along the
direction of the magnetic field lines and not along the density
gradient, whereas the major axis of the scattered source is
perpendicular to the local magnetic field (the scattering anisotropy
axis). Using a dipolar magnetic field structure of an active region, we
reproduce observed radio fine-structure source motion parallel to the
solar limb associated with a coronal loop and provide a natural
explanation for puzzling observations of solar radio burst position
motions with the Low Frequency Array. Furthermore, the anisotropy
aligned with a dipolar magnetic field causes the apparent-source images
to bifurcate into two distinct components, with characteristic sizes
smaller than in unmagnetized media. The temporal broadening induced by
scattering reduces the observed frequency drift rate of fine structures,
depending on the contribution of scattering to the time profile. The
findings underscore the role of magnetic field geometry and anisotropic
scattering for the interpretation of solar radio bursts and highlight
that anisotropic scattering produces more than a single source.</description>
</item>
<item>
<title> Revisiting Sunspot Number As An Extreme Ultraviolet (Euv) Proxy For Ionospheric F2 Critical Frequency</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AnGeo..43...91Z</link>
<description>This study reconsiders sunspot number (Sn) as a solar extreme
ultraviolet (EUV) proxy for modeling the ionospheric F2 layer's critical
frequency (foF2) over the period 1960-2023. We compare the performance
of Sn with F10.7 and F30 solar radio fluxes, focusing on their ability
to model the Ionospheric Global index (IG). Our results reveal that
while F30 has shown a better correlation in recent solar cycles, Sn is
the most stable and reliable over the entire dataset, obtaining the
highest correlation. In addition, if we remove the saturation effects
from considering a maximum value of Sn, the correlation increases,
outperforming all other proxies and correctly predicting the long-term
trend estimated by general circulation models.</description>
</item>
<item>
<title> Investigation Of The October Effect In Very Low-Frequency (Vlf) Signals</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AnGeo..43...55H</link>
<description>Subionospheric very low-frequency (VLF) radio signals are reflected by
free electrons in the ionospheric D-region at about 60-90 km altitude
and can propagate over long distances, which makes them useful for
monitoring the state of the D-region or perturbations due to solar
flares. At the D-region height, the ionosphere is mainly ionized by
solar Lyman- radiation. The reflection characteristics of VLF signals
depend on the state and dynamics of the D-region, which is highly
influenced by Lyman- radiation. Although the amplitude of the received
terrestrial VLF signal changes as a function of solar zenith angle over
the course of the year, the VLF amplitude shows a distinctive sharp
decrease around October, which is hence called the "October effect".
This study investigates the occurrence of the October effect and its
dependencies on latitude and longitude. We developed a method to detect
the occurrence of the October effect in the long-term VLF data and
derive key parameters characterizing (start and end date, intensity) the
sudden decrease in the signal amplitude. This investigation using a
network of VLF stations distributed over low-, middle-, and high-
latitude regions shows that the occurrence of the October effect has a
clear latitudinal dependency, occurring earlier in high-latitude regions
than at midlatitudes. No low-latitude signature is found.</description>
</item>
<item>
<title> Large solar energetic particles and solar radio emissions during Cycle 25. A comparative analysis of trends and characteristics with cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdSpR..75.1415N</link>
<description>Solar energetic particles (SEPs) affect space weather in both the
heliosphere and on Earth. The present study investigates the occurrences
of large SEP events focusing on their influence on the Earth, as well as
their correlation with solar radio bursts (SRBs). The velocity
dispersion analysis (VDA) is used to calculate the release times of
large SEP events from their launch locations, as well as their apparent
path length that connects them to interplanetary magnetic fields lines.
According to the study, 122 large SEP events impacted the planet Earth
from 1997 to 2024. The comparison of occurrence rates with previous
solar cycles (SCs) suggests that SC 25 will peak with greater solar
activity than the cycle 24 in terms of large SEP occurrences since large
SEP events correlate well with the pattern of the sunspot cycle
progression. In general, a few (35 out of 122) large SEP events are
typically released from the Sun at times that coincide with the peak of
associated solar flares and the onsets of corresponding SRBs indicating
no delay while the rest have delayed in the release. The projected
apparent lengths (L) range from 1.0 to 3.0 AU, with L exceeding 1.5 AU
due to particle scattering and launch site pitch angles. The majority
(115/122) of SEP occurrences are accelerated by shock waves from solar
flares, CMEs, and fast plasma flow in the magnetic reconnection regions.
Relevant SRBs for space weather study as they precede large SEP events
diagnose the properties of particle populations propelled by solar
flares and CMEs. This study finds that 90% of the large SEP events are
preceded by solar radio emissions of type II, III and IV; and
WAVES/STEREO revealed &lt;mml:math altimg="si216.svg"&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/
mml:mo&gt;&lt;mml:mn&gt;76&lt;/mml:mn&gt;&lt;mml:mo&gt;%&lt;/mml:mo&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; of
SRBs have continuation in IP medium indicating the dynamics of
associated shocks and electron beams traveling along open and quasi-open
magnetic field lines. Thus, SRB monitoring continues to be a valuable
tool for studying space weather and understanding physical phenomena in
the solar corona and IP medium, such as particle populations that cause
large SEP occurrences.</description>
</item>
<item>
<title> The Impact of Space Weather on Ultraviolet Radiation at Mid Latitudes</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdMet202551692M</link>
<description>Solar ultraviolet (UV) radiation plays a crucial role in various
environmental, atmospheric, and industrial applications, despite
covering only a small portion of the electromagnetic solar radiation.
The distribution of UV radiation reaching the Earth's surface is
influenced by multiple environmental, atmospheric, and astronomical
factors, some of which require further investigation. The aim of this
study is to explore the potential impact of cosmic rays and space
weather parameters on solar UV radiation. To achieve this, the study
utilized solar UV data collected from the King Abdulaziz City for
Science and Technology (KACST) radiometric station, situated in central
Saudi Arabia (latitude 24 43, longitude 46 40, altitude 613 m) for the
period 20152021, along with space weather parameters. These parameters
include solar radio flux at 10.7 cm (F10.7 cm) and sunspot number (SSN),
as well as cosmic ray data from the Oulu neutron monitor for the same
period as the UV data. The study conducted correlation analyses between
the time series UV data and the considered parameters, revealing mutual
relationships between these variables. UV radiation demonstrated a
positive correlation with the SSN and F10.7 cm radio flux while showing
a significant anticorrelation with the CR data. Furthermore, the mean
daily time series of the variables underwent power spectral analyses to
identify potential common periodicities. The spectral analyses showed
several common periodicities in all the variables considered, such as
~410, 172, 165, and 66 days. Based on the correlations and spectral
results, the study suggests that solar signals could have a direct or
indirect impact on the observed solar UV radiation at a specific site.
This finding has significant implications for our understanding of the
factors that affect UV radiation.</description>
</item>
<item>
<title> Analysis of Seismic Ionospheric Effects and Prediction of TEC During Earthquakes Occurred in Indonesia Based on GPS Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2025AdAst202553529M</link>
<description>Total electron content (TEC), which quantifies the quantity of free
electrons in the Earth's ionosphere, is a crucial parameter that
experiences discrepancies during seismic events. This study investigates
the potential of utilizing TEC prediction at the BAKO position in
Indonesia during earthquakes. TEC data and solar parameters were
collected for six preselected earthquakes, encompassing the earthquake
event periods. Three prediction models, namely, ARMA, OKSM 1, and OKSM
2, were employed to predict TEC for a period spanning 8 days. The input
parameters required for TEC prediction were obtained from the IONOLAB
and OMNIWeb database. The OKSM 1 model is constructed with the input
parameters like solar radio flux at 10.7 cm (F10.7), disturbance storm
time index (Dst), solar wind (Sw), sunspot number (SSN), and TEC values,
while the OKSM 2 model is developed with the parameters like geomagnetic
indices (Kp and Ap) and solar indices SSN and F10.7 along with TEC data.
The ARMA model is constructed with TEC data. The primary objective of
this research is to assess the utility of TEC prediction based on the
influence on input parameters for the kriging models and to identify the
most effective model for predicting TEC variations associated with
seismic events. Four evaluation metrics were systematically utilized to
gauge the performance of each model. This rigorous evaluation aims to
deliver perceptions into the predictive accuracy, reliability, and
potential practical implications of TEC predicting during earthquakes.
Upon comparison, the OKSM 2 model demonstrated superior predictive
accuracy, exhibiting a notable agreement with the true TEC. The results
suggest that OKSM 2 holds promise as a reliable model for
earthquakerelated TEC prediction. The average RMSE values range from
4.06 to 8.06, indicating the models' ability to predict seismic events
with a reasonable magnitude of error. Similarly, the average MAE values,
ranging from 3.32 to 6.71, underscore the models' overall accuracy in
predicting the absolute differences between actual and predicted TEC.
The CC values, averaging between 0.97 and 0.99, highlight a strong
relationship between predicted and actual TEC values. Additionally, the
average sMAPE values, ranging from 0.11 to 0.21, demonstrate the models'
effectiveness in minimizing percentagebased errors. While variations
exist across different earthquakes, these average metrics collectively
suggest promising predicting capabilities.</description>
</item>
<item>
<title> Horizontal Short Monopole Antenna for Radiosolariz Solar Radio Telescope</title>
<link>https://ui.adsabs.harvard.edu/abs/2025ARBl...37..118Z</link>
<description>This paper elaborates on the possible implementation of a horizontally
shortened monopole antenna in broadband radio reception of radio
emissions originating from the Sun. The spectrum of interest is in the
low portion of the very high frequency (VHF) radio band. The frequency
range extends down to the top end of the high frequency (HF) spectrum
near 20 MHz and up to 65 MHz. The ionosphere is mostly radio-transparent
to these radio waves, permitting observations of solar activity in the
mentioned radio band. The proposed monopole antenna is an un-tuned
wideband antenna suitable for reception only. This aerial is inadequate
for the transmission of radio waves due to its low efficiency. Another
prerequisite for implementing this antenna is the presence of high
background noise  the background noise level commonly encountered in
the low part of the VHF band, even in rural regions, is of the expected
magnitude. The suggested antenna has superior qualities than most other
antennas suitable for the task. It shows benefits such as small
dimensions, being hard to break, simplicity of construction, and
consisting of a single element both electrically and mechanically. Other
advantages of the proposed antenna include a very low cost of building
and maintenance, straightforward operation, small weight, portability,
an omnidirectional gain pattern in the plane perpendicular to the
antenna element, and a uniformly and monotonically increasing smooth
gain curve as a function of frequency. This aerial has been built for
the aims of the radioSolariz project (www.radiosolariz.space), which is
a Bulgarian radio telescope project initiated in 2019 at the Space
Research and Technology Institute  Bulgarian Academy of Sciences. The
project is backed by a number of designs and innovations protected by
patents and utility models registered at the Patent Office of the
Republic of Bulgaria.</description>
</item>
<item>
<title> Solar flare observations with the Radio Neutrino Observatory Greenland (RNO-G)</title>
<link>https://ui.adsabs.harvard.edu/abs/2025APh...16403024A</link>
<description>The Radio Neutrino Observatory  Greenland (RNO-G) seeks discovery of
ultra-high energy neutrinos from the cosmos through their interactions
in ice. The science program extends beyond particle astrophysics to
include radioglaciology and, as we show herein, solar observations, as
well. Currently seven of 35 planned radio-receiver stations (24
antennas/station) are operational. These stations are sensitive to
impulsive radio signals with frequencies between 80 and 700 MHz and
feature a neutrino trigger threshold for recording data close to the
thermal floor. RNO-G can also trigger on elevated signals from the Sun,
resulting in nanosecond resolution time-domain flare data; such temporal
resolution is significantly shorter than from most dedicated solar
observatories. In addition to possible RNO-G solar flare polarization
measurements, the Sun also represents an extremely useful above-surface
calibration source. Using RNO-G data recorded during the summers of 2022
and 2023, we find signal excesses during solar flares reported by the
solar-observing Callisto network and also in coincidence with &lt;mml:math
altimg="si24.svg" display="inline"
id="d1e1419"&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;/mml:math&gt;2/3 of the brightest excesses
recorded by the SWAVES satellite. These observed flares are
characterized by significant time-domain impulsivity. Using the known
position of the Sun, the flare sample is used to calibrate the RNO-G
absolute pointing on the radio signal arrival direction to sub-degree
resolution. We thus establish the Sun as a regularly observed
astronomical calibration source to provide the accurate absolute
pointing required for neutrino astronomy.</description>
</item>
<item>
<title> Determining the acceleration regions of in situ electrons using remote radio and X-ray observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...693A.296M</link>
<description>Context. Solar energetic particles in the heliosphere are produced by
flaring processes on the Sun or by shocks driven by coronal mass
ejections. These particles are regularly detected remotely as
electromagnetic radiation (X-rays or radio emission), which they
generate through various processes, or in situ by spacecraft monitoring
the Sun and the heliosphere. Aims. Our aim is to combine remote-sensing
and in situ observations of energetic electrons to determine the origin
and acceleration mechanism of these particles. Methods. Here we
investigate the acceleration location, escape, and propagation
directions of electron beams producing radio bursts observed with the
Low Frequency Array (LOFAR), hard X-ray (HXR) emission, and in situ
electrons observed at Solar Orbiter on 3 October 2023. These
observations are combined with a three-dimensional (3D) representation
of the electron acceleration locations and results from a
magnetohydrodynamic (MHD) model of the solar corona in order to
investigate the origin and connectivity of electrons observed remotely
at the Sun to in situ electrons. Results. We observed a type II radio
burst with good connectivity to Solar Orbiter, where a significant
electron event was detected. However, type III radio bursts and hard
X-rays were also observed co-temporally with the electron event, but
likely connected to Solar Orbiter by different far-side field lines. The
injection times of the Solar Orbiter electrons are simultaneous with
both the onset of the type II radio burst, the group of type III bursts,
and the presence of a second HXR peak; however, the most direct
connection to Solar Orbiter is that of the type II burst location. The
in situ electron spectra point to shock acceleration of electrons with a
short-term connection to the source region. Conclusions. We propose that
there are two contributions to the Solar Orbiter electron fluxes based
on the results and magnetic connectivity determined from remote-sensing
data: a smaller flare contribution from the far-side of the Sun and a
main shock contribution from the region close to the eastern limb as
viewed from Earth. We note that these two electron acceleration regions
are distinct and separated by a large distance and are connected via two
separate field lines to Solar Orbiter.</description>
</item>
<item>
<title> Simulation of weak electron beam injection into plasma with open boundary conditions</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...693A.236A</link>
<description>Context. Different high-energy events lead to the generation of electron
beams in the solar atmosphere as well as in planetary magnetospheres.
The propagation of these beams through space plasma becomes a main
source of non-thermal emission, primarily on the harmonics of the
fundamental plasma frequency. Due to the high level of non-linearity and
the complexity of such systems, theoretical studies of them are largely
based on numerical simulations. However, it is still common practice to
use a simplified model in which periodic boundary conditions for fields
and particles are used to simulate an infinite plasma. Aims. In this
work, the first attempt at high-resolution studies of the dynamics of a
weak beam in space plasma using a model with open boundary conditions is
reported. The general results of the simulations are compared with those
obtained previously using the approximation of infinite plasma. Methods.
The continuous injection of an electron beam with an average velocity of
v&lt;SUB&gt;b&lt;/SUB&gt; = 0.25c (c  speed of light) and a relative density of
n&lt;SUB&gt;b&lt;/SUB&gt;/n&lt;SUB&gt;0&lt;/SUB&gt; = 5  10&lt;SUP&gt;4&lt;/SUP&gt; (n&lt;SUB&gt;0&lt;/SUB&gt; 
plasma density) into an unmagnetised plasma was simulated in a quasi-1D
approximation using a collisionless electromagnetic particle-in-cell
code. The background plasma was initially homogeneous and consisted of
electrons and protons with the real mass ratio. The total simulation
time was 10 000 &lt;SUB&gt;p0&lt;/SUB&gt;&lt;SUP&gt;1&lt;/SUP&gt;, where &lt;SUB&gt;p0&lt;/SUB&gt; is the
Langmuir frequency for the given n&lt;SUB&gt;0&lt;/SUB&gt;. Results. The present
simulations demonstrate the formation of a spatially localised Langmuir
turbulence in the close vicinity of the beam injection site. The
continuous injection of fresh beam particles increases the amplitude of
the plasma waves to values larger than those possible when simulating
the same parameters in a simplified model. Plasma waves in this region
turn out to be unstable against the modulation instability, so the
formation of density wells followed by plasma wave trapping is observed.
Some of the beam particles are significantly accelerated by previously
arisen plasma waves. On average, only 10% of the beam energy gets lost
in the system, but the distribution function is transformed into a flat-
top form with a supra-thermal tail. Conclusions. The obtained results
demonstrate several significant differences from the results of
simulations using the approximation of infinite plasma. This fact
emphasises the importance of using of a more realistic model for
simulations of beam-plasma systems. In addition, using the model with
open boundaries, in contrast to the simplified model, will allow us to
correctly investigate the influence of not only random gradients of the
plasma parameters, but also regular ones.</description>
</item>
<item>
<title> V. Magnetohydrodynamic waves in a fibrillar structure</title>
<link>https://ui.adsabs.harvard.edu/abs/2025A&amp;A...693A..19S</link>
<description>Magnetohydrodynamic (MHD) waves, playing a crucial role in transporting
energy through the solar atmosphere, manifest in various chromospheric
structures. Here, we investigated MHD waves in a long-lasting dark
fibril using high-temporal-resolution (2 s cadence) Atacama Large
Millimeter/submillimeter Array (ALMA) observations in Band 6 (centered
at 1.25 mm). We detected oscillations in brightness temperature,
horizontal displacement, and width at multiple locations along the
fibril, with median periods and standard deviations of 240  114 s, 225
 102 s, and 272  118 s, respectively. Wavelet analysis revealed a
combination of standing and propagating waves, suggesting the presence
of both MHD kink and sausage modes. Less dominant than standing waves,
oppositely propagating waves exhibit phase speeds (median and standard
deviation of distributions) of 74  204 km/s, 52  197 km/s, and 28 
254 km/s for the three observables, respectively. This work demonstrates
ALMA's capability to effectively sample dynamic fibrillar structures,
despite previous doubts. This provides valuable insights into wave
dynamics in the upper chromosphere.</description>
</item>
<item>
<title> Possible Mechanisms and Impacts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2204126T</link>
<description>One of the most intense geomagnetic storms of recent times occurred on
10-11 May 2024. With a peak negative excursion of Sym-H below -500 nT,
this storm is the second largest of the space era. Solar wind energy
transferred through radiation and mass coupling affected the entire
Geospace. Our study revealed that the dayside magnetopause was
compressed below the geostationary orbit (6.6 RE) for continuously 6 hr
due to strong Solar Wind Dynamic Pressure (SWDP). Tremendous compression
pushed the bow-shock also to below the geostationary orbit for a few
minutes. Magnetohydrodynamic models suggest that the magnetopause
location could be as low as 3.3RE. We show that a unique combination of
high SWDP (15 nPa) with an intense eastward interplanetary electric
field (IEF&lt;SUB&gt;Y&lt;/SUB&gt;  2.5 mV/m) within a super-dense Interplanetary
Coronal Mass Ejection lasted for 409 min-is the key factor that led to
the strong ring current at much closer to the Earth causing such an
intense storm. Severe electrodynamic disturbances led to a strong
positive ionospheric storm with more than 100% increase in dayside
ionospheric Total Electron Content (TEC), affecting GPS
positioning/navigation. Further, an HF radio blackout was found to occur
in the 2-12 MHz frequency band due to strong D- and E-region ionization
resulting from a solar flare prior to this storm.</description>
</item>
<item>
<title> Improving Solar Proton Event Forecasting by Means of Automated Recognition of Type-III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2204013P</link>
<description>This work reports on an attempt toward improving the Relativistic
Electron Alert System for Exploration (REleASE): the occurrence of a
type-III radio burst as a precondition for a REleASE forecast. REleASE
forecasts are based on the detection of early arrival of near-
relativistic electrons ahead of more hazardous protons from Solar
Energetic Particle (SEP) events. The goal is to allow astronauts on a
Lunar or Mars mission sufficient advance warning to reach a radiation
shelter to minimize radiation dose exposure. We test a new system that
sets a condition of the occurrence of a type-III radio burst, thus
adding independent evidence of particle escape from the Sun, with the
aim of reducing known sources of false-alarms of the existing REleASE
system. The High Energy Solar Particle Events foRecastIng and Analysis
(HESPERIA) REleASE+ system, which takes advantage of availability of
real-time solar radio observations during the passage of STEREO-A by
Earth in 2023, has now been incorporated in the HESPERIA framework. We
discuss the techniques used for automatic detection of type-III radio
bursts preparing for its real-time implementation, the determination of
selection criteria for type-III bursts that are candidates for solar
proton events in the Earth-moon system, and first results of the
combined system.</description>
</item>
<item>
<title> Spectral Analysis of Two-Year Ionospheric Data Series</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Senso..24.7795J</link>
<description>This study demonstrates a rich complexity of the time-frequency
ionospheric signal spectrum, dependent on the measurement type and
platform. Different phenomena contributing to satellite-derived and
ground-derived geophysical data that only selected signal bands can be
potentially sensitive to seismicity over time, and they are applicable
in lithosphere-atmosphere-ionosphere coupling (LAIC) studies. In this
study, satellite-derived and ground-derived ionospheric observations are
filtered by a Fourier-based band-pass filter, and an experimental
selection of potentially sensitive frequency bands has been carried out.
This work focuses on band-pass filtered ionospheric observations and
seismic activity in the region of the Aegean Sea over a two-year time
period (2020-2021), with particular focus on the entire system of
tectonic plate junctions, which are suspected to be a potential source
of ionospheric disturbances distributed over hundreds of kilometers. The
temporal evolution of seismicity power in the Aegean region is
represented by the record of earthquakes characterized by M  4.5, used
for the estimation of cumulative seismic energy. The ionospheric
response to LAIC is explored in three data types: short inspections of
in situ electron density (Ne) over a tectonic plate boundary by Swarm
satellites, stationary determination of three Ne density profile
parameters by the Athens Digisonde station AT138 (maximum frequency of
the F2 layer: foF2; maximum frequency of the sporadic E layer: foEs; and
frequency spread: ff), and stationary measure of vertical total electron
content (VTEC) interpolated from a UPC-IonSAT Quarter-of-an-hour time
resolution Rapid Global ionospheric map (UQRG) near Athens. The
spectrograms are made with the use of short-term Fourier transform
(STFT). These frequency bands in the spectrograms, which show a notable
coincidence with seismicity, are filtered out and compared to cumulative
seismic energy in the Aegean Sea, to the geomagnetic Dst index, to
sunspot number (SN), and to the solar radio flux (F10.7). In the case of
Swarm, STFT allows for precise removal of long-wavelength Ne signals
related to specific latitudes. The application of STFT to time series of
ionospheric parameters from the Digisonde station and GIM VTEC is
crucial in the removal of seasonal signals and strong diurnal and semi-
diurnal signal components. The time series formed from experimentally
selected wavebands of different ionospheric observations reveal a
moderate but notable correlation with the seismic activity, higher than
with any solar radiation parameter in 8 out of 12 cases. The correlation
coefficient must be treated relatively and with caution here, as we have
not determined the shift between seismic and ionospheric events, as this
process requires more data. However, it can be observed from the
spectrograms that some weak signals from selected frequencies are
candidates to be related to seismic processes.</description>
</item>
<item>
<title> Regional features of ionospheric disturbances during the intense geospace storm of November 4-5, 2023</title>
<link>https://ui.adsabs.harvard.edu/abs/2024RPE....41....7C</link>
<description>Relevance. The ionosphere is the main channel that ensures the
functioning of radio communication, radionavigation, radar, remote radio
sensing, and radio astronomy systems. The parameters of this channel
significantly affect the quality and functionality of both terrestrial
and space technological systems. The channel parameters are shaped by
various factors within the Earthatmosphereionospheremagnetosphere
(EAIM) system. The most influential factor is solar storms, which are
accompanied by solar flares, solar cosmic radiation, and coronal mass
ejections. These events greatly disturb the
atmosphereionospheremagnetosphere radio channels, leading to
disruptions in the operation of radio systems for various purposes.
Therefore, comprehensive research into radio channel disturbances is a
relevant task. The aim of this work is to describe the results of
research on the regional peculiarities of ionospheric disturbances
through the analysis of derivatives from global ionospheric maps,
specifically maps of percentage increases in total electron content
(TEC) values. Methods and Methodology. The primary data used for this
study are global ionospheric maps compiled by the Center for Orbit
Determination in Europe, which are freely available on the website of
The Crustal Dynamic Data Information System. Results. For the first
time, using GNSS technologies, maps of percentage increases in TEC
values in the ionosphere were constructed and studied, which can be
interpreted as an ionospheric disturbance index. The response of TEC to
the powerful geospace storm of November 4-5, 2023, was investigated. It
was found that during most of the main phase of the magnetic storm, the
largest ionospheric disturbances were observed at latitudes
significantly lower than the Arctic and Antarctic Circles, indicating a
reconfiguration of the ionospheremagnetosphere current system, the
emergence of significant currents, and a change in ionospheric weather
conditions.</description>
</item>
<item>
<title> Heliospheric Effect on Solar Activity Parameters during Maximum Phase of Solar Cycle 24 (20122015)</title>
<link>https://ui.adsabs.harvard.edu/abs/2024RAA....24l5001S</link>
<description>The time series of daily data on solar activity proxies, namely the
sunspot number (SSN), sunspot area (SSA), solar radio flux (F10.7),
modified coronal index (MCI), solar flare index (FI), and cosmic ray
intensity (CRI), were analyzed to understand the solar activity
modulations and short-term periodicities therein. Rieger-type and other
short-term periods include the solar rotational period that covers the
maximum activity phase period (maximum phase of solar cycle 24). The
wavelet power spectra and Periodogram of SSN, SSA, F10.7, MCI, FI, and
CRI exhibited a significant short-term period. The heliospheric effects
exist for a particular period (27 days) and they are related to the
solar activity phenomena. The cross-correlation coefficients and time
lags between the CRI and solar activity parameters were estimated to be
200, 46, 281, 39, and 47 days for SSN, SSA, F10.7, MCI, and FI
respectively during the time series 20122015 (maximum phase of solar
cycle 24).</description>
</item>
<item>
<title> Stellar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2024LRSP...21....1K</link>
<description>Magnetic storms on stars manifest as remarkable, randomly occurring
changes of the luminosity over durations that are tiny in comparison to
the normal evolution of stars. These stellar flares are bursts of
electromagnetic radiation from X-ray to radio wavelengths, and they
occur on most stars with outer convection zones. They are analogous to
the events on the Sun known as solar flares, which impact our everyday
life and modern technological society. Stellar flares, however, can
attain much greater energies than those on the Sun. Despite this, we
think that these phenomena are rather similar in origin to solar flares,
which result from a catastrophic conversion of latent magnetic field
energy into atmospheric heating within a region that is relatively small
in comparison to normal stellar sizes. We review the last several
decades of stellar flare research. We summarize multi-wavelength
observational results and the associated thermal and nonthermal
processes in flaring stellar atmospheres. Static and hydrodynamic models
are reviewed with an emphasis on recent progress in radiation-
hydrodynamics and the physical diagnostics in flare spectra. Thanks to
their effects on the space weather of exoplanetary systems (and thus in
our search for life elsewhere in the universe) and their preponderance
in Kepler mission data, white-light stellar flares have re-emerged in
the last decade as a widely-impactful area of study within astrophysics.
Yet, there is still much we do not understand, both empirically and
theoretically, about the spectrum of flare radiation, its origin, and
its time evolution. We conclude with several big-picture questions that
are fundamental in our pursuit toward a greater understanding of these
enigmatic stellar phenomena and, by extension, those on the Sun.</description>
</item>
<item>
<title> Effects of a Solar Flare on Global Propagation of Extremely Low Frequency Waves</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JGRA..12933083O</link>
<description>Solar flares have profound impacts on the lower ionosphere and long-
distance radio propagation. Extremely low frequency (ELF: 33,000 Hz)
waves are challenging to observe and experience unique interactions with
the lower ionosphere. The primary natural sources of ELF waves are
thunderstorm lightnings across the globe. Using a newly developed
azimuth determination technique and improved observation hardware we
show that ELF attenuation in the Earth-Ionosphere spherical cavity
decreases and propagation velocity increases under the influence of an
M-class solar flare. Using a two-parameter model of the lower
ionosphere, the observations are shown to be consistent with increased
electron density and sharper gradients in the D-region resulting from
X-ray radiation. The sharper electron density gradient is primarily
responsible for the propagation velocity increase, suggesting a unique
capability that ELF observations can bring to global remote sensing of
the lower ionosphere under space weather perturbations.</description>
</item>
<item>
<title> Differential responses of total ozone content to solar activity parameters at two Saudi Arabian locations</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JASTP.26506379M</link>
<description>This study examines the correlations between Total Ozone Content (TOC)
at two locations in Saudi ArabiaAbha and Jeddahand various solar
activity indicators (sunspot numbers, solar radio flux) and cosmic rays,
using data spanning from 1979 to 2023. The research employs correlation
analyses and spectral techniques, such as Fast Fourier Transform and
wavelet analysis, to explore these relationships. The results reveal
significant non-zero correlations between changes in TOC at both Saudi
sites and the studied solar activity indicators and cosmic rays, with
these correlations varying in strength and significance across different
solar cycles and seasons. Spectral analysis suggests the presence of
several periodicities in the TOC data from both sites, including cycles
of 3.9 years, 2.63 years, 1.65 years, 1.11.2 years, 325 days (0.88
years), 285293 days (0.780.80 years), 273 days (0.75 years), 249-232
days (0.68 years), and 202-188 days (0.52 years). Notable shared
periodicities between TOC and solar activity and cosmic rays data
include 2.6 years, 3.83.9 years, 1.56 years, 325 days, 273 days, and
166 days. The findings from both correlation and spectral analyses
suggest a potential connection between variations in TOC and solar
activity at the specific locations studied. This aligns with previous
research indicating that increased UV radiation during periods of high
solar activity enhances ozone production, particularly at lower
latitudes, and that increased magnetic activity reduces the influx of
cosmic rays into the heliosphere, impacting atmospheric ionization.</description>
</item>
<item>
<title> On Possible Additional Sources of Solar Protons in the Events of September 410, 2017</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64.1148G</link>
<description>The article considers the period from September 4 to September 10, 2017,
inclusive, during which the last proton events of solar cycle 24
occurred. In order to detect possible additional proton sources and
verify the sources already listed in various catalogs, we apply an
empirical method for predicting proton events to all solar flares
detected during this period. It is based on the threshold criteria of
the parent flares. In addition, we apply an algorithm for automatic
search of proton flares obtained by machine learning. Two variants of
the automatic search algorithm are used: the first one (method 319) does
not take into account the duration of the radio emission, while the
second one (method 189) imposes a condition on its duration (&gt;2 min).
The empirical method shows that, except for the source flares found by
the time of the first arrival of solar protons on Earth, other flares of
this period do not fulfill all the criteria of "protonicity." An
additional test of the automatic method is the detection of proton
flares that we selected by the protonicity criteria but that did not
make it to the training sample. Method 319 considers proton flares X9.3
on September 6, 2017, M1.4 and X1.3 on September 7, 2017, and C8.3 on
September 8, 2017, as proton flares. Method 189 does not consider the
flares of September 7 and 8, 2017, as credible proton sources, which is
consistent with expert empirical estimates of the protonicity criteria.</description>
</item>
<item>
<title> Prediction of Range Error in GPS Signals during X-Class Solar Flares Occurred between JanuaryApril 2023 Using OKSM and RNN</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64..932M</link>
<description>Positioning, navigation and time are the cornerstones of satellite
navigation. These aspects are frequently affected by ionospheric
variations caused by solar flares (SF). In this study, we have attempted
to predict the range error (RE) caused by ionospheric delay in Global
Positioning System (GPS) signals during six different X-class SF that
occurred in the 25th solar cycle using two different approaches, namely,
a recurrent neural network (RNN) and the ordinary Kriging-based
surrogate model (OKSM). The total electron content (TEC) collected from
Hyderabad station along with other input parameter includes the
Planetary A and K index (Ap and Kp), solar sunspot number (SSN),
disturbance storm time index (Dst), and radio flux measured at 10.7 cm
(F10.7) were used for prediction. The OKSM uses the previous six days of
datasets to predict the RE on the seventh day, whereas the RNN model
uses the previous 45 days of datasets to predict the RE on the 46th day.
The performance of both models is evaluated using statistical parameters
such as root mean square error (RMSE), normalized root mean square error
(NRMSE), Pearson's correlation coefficient (CC), and symmetric mean
absolute percentage error (sMAPE). The results indicate that the OKSM
performs well in adverse space weather conditions when compared to RNN.</description>
</item>
<item>
<title> Mechanisms of Zebra Pattern Generation in Solar Radio Emission on the Background of Complex Dynamic Spectra</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64..793C</link>
<description>The discussion about the origin of the zebra pattern has been going on
for more than 50 years. In many papers it is usually postulated that the
double plasma resonance mechanism always works in the presence of fast
particles in the magnetic trap. Due to a number of difficulties
encountered by this mechanism, works on its improvement began to appear,
mainly in a dozen papers by Karlick and Yasnov, where the whole
discussion is based on variability of the ratio of the magnetic field
and density height scales and the assumption of some plasma turbulence
in the source. Here we show possibilities of an alternative model of the
interaction between plasma waves and whistlers. Several phenomena were
selected in which it is clear that the ratio of height scales does not
change in the magnetic loop as the source of the zebra pattern. It is
shown that all the main details of the sporadic zebra pattern in the
phenomenon of August 1, 2010 (and in many other phenomena), can be
explained within the framework of a unified model of zebra patterns and
radio fibers (fiber bursts) in the interaction of plasma waves with
whistlers. The main changes in the zebra pattern stripes are caused by
scattering of fast particles by whistlers leading to switching of the
whistler instability from the normal Doppler effect to the anomalous
one. In the end, possibilities of laboratory experiments are considered
and the solar zebra pattern is compared with similar stripes in the
decameter radio emission of Jupiter.</description>
</item>
<item>
<title> Geomagnetic field variations due to solar tides at the Indian Observatories</title>
<link>https://ui.adsabs.harvard.edu/abs/2024EP&amp;S...76...61D</link>
<description>This study investigates the response of solar (S) tidal signatures on
the horizontal component of the geomagnetic field at two observatories
in India during 19802002 over solar cycles (SC) 2123: Hyderabad (HYB),
located in the low-latitude region, and Ettaiyapuram (ETT), situated at
the magnetic equator. HYB represents the characteristics of solar quiet
(Sq), while ETT is under the equatorial electrojet (EEJ) effect. Our
results show the additional information about ter (S3), and quarta-
diurnal (S4) tidal signatures of Sq and EEJ, along with diurnal (S1) and
semi-diurnal (S2) at both observatories. In Sq solar tide, the average
amplitude of S1 tide is consistently higher than that of EEJ tide by ~
10%. During the same period, the S2, S3, and S4 tidal signatures of Sq
are weaker than EEJ by ~ 2%, 5%, and 2.5%, respectively. During solar
cycle maxima, the amplitude of the Sq tide is higher in SC-21 than in
SC-22 and SC-23 by ~ 13% and 16%, while SC-22 has higher EEJ tidal
amplitudes than other SCs by ~ 9%. We observe that the tidal signatures
of Sq and EEJ closely follow the trend of solar radio flux (F10.7),
except for S4 of Sq. The Pearson correlation coefficients (P) between
F10.7 and Sq/EEJ tidal amplitudes exhibit negative to positive
correlation coefficients during different phases of SCs. The solar tidal
amplitudes of Sq/EEJ (S1-S4) with F10.7 during D, E, and J seasons have
varying correlation coefficients, indicating that each tide has a
distinct response on the geomagnetic field.</description>
</item>
<item>
<title> Electron Cyclotron Maser with Moderately Relativistic Electrons</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...977..260Z</link>
<description>Electron cyclotron maser (ECM) emission is an important coherent
emission mechanism for the direct amplification of electromagnetic waves
by nonthermal electrons in a magnetized plasma. This paper will report
on our recent study on ECM emission by fast electron beams with
moderately relativistic energy. The results show that, similar to the
spontaneous emission by the magnetic cyclotron motion of energetic
electrons in a magnetic field, the coherent emission also exhibits the
characteristic of a gradual transition from harmonic emission to
continuous emission as the energy of the energetic electrons increases
from subrelativistic to relativistic. The effects of the characteristic
beam electrons energy (E&lt;SUB&gt;c&lt;/SUB&gt;) and the plasma-to-cyclotron
frequency ratio (&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;) on the growth rate, the
peak-value frequency, and the spectral width are discussed further.
These results are helpful for us to understand phenomena associated with
astrophysical radio bursts.</description>
</item>
<item>
<title> On the Possible Mechanisms of the SEP Event and Electron Enhancement over the SEP Decay Phase on 2023 August 5</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...977..248F</link>
<description>We carry out this study on the solar energetic particle (SEP) event that
occurred on 2023 August 5 over the ascending phase of the current solar
cycle 25. It is found that the SEP event might have been initiated by
the M1.6 flare, while the SEP peak was caused by the coronal shock
manifested in DH-type II radio burst over the propagation phase of a
halo coronal mass ejection (CME; 1000 km s&lt;SUP&gt;1&lt;/SUP&gt;), thus creating
a mixed SEP event. There were two enhancements of the electron fluxes
lying over the SEP rise and decay phase. It is surprising that, despite
a stronger flare (X1.6) and a faster halo CME (1647 km s&lt;SUP&gt;1&lt;/SUP&gt;),
there was no SEP enhancement during the second enhancement of the
electron fluxes. In order to investigate this, we make an additional
effort to analyze the X1.6 flare based on the availability of the
temporal, spectral, and spatial evolution of the electromagnetic
radiation components. It is observed that the CME shock was aligned with
the flare eruption direction and was close to the western limb (W77),
and thus the radially moving CME shock missed the Earth. In another
development, it is observed that the electron impulsive phase lies over
the type III radio bursts, indicating that the electrons might have
escaped directly during the eruption. The radio flux and radio dynamic
spectra of a higher frequency lie over the rise phase of the soft X-ray
derivative, indicating that a large number of electrons travelled
through magnetic fields.</description>
</item>
<item>
<title> Advection-nonlinear-diffusion Model of Flare Accelerated Electron Transport in Type III Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...976..233K</link>
<description>Electrons accelerated by solar flares and observed as type III solar
radio bursts are not only a crucial diagnostic tool for understanding
electron transport in the inner heliosphere but also a possible early
indication of potentially hazardous space weather events. The electron
beams traveling in the solar corona and heliosphere along magnetic field
lines generate Langmuir waves and quasilinearly relax toward a plateau
in velocity space. The relaxation of the electron beam over the short
distance in contrast to large beam-travel distances observed is often
referred to as Sturrok's dilemma. Here, we develop a new electron
transport model with quasilinear distance/time self-consistently
changing in space and time. This model results in a nonlinear advection-
diffusion equation for the electron beam density with a nonlinear
diffusion term that is inversely proportional to the beam density. The
solution predicts slow super-diffusive (ballistic) spatial expansion of
a fast-propagating electron beam. This model also provides the evolution
of the spectral energy density of Langmuir waves, which determines
brightness temperature of plasma radiation in solar bursts. The model
solution is consistent with the results of numerical simulation using
kinetic equations and can explain some characteristics of type III solar
radio bursts.</description>
</item>
<item>
<title>math&gt; index and its application study on the Chinese Langfang dataset</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..74.6309Y</link>
<description>The 10.7 cm solar radio flux (&lt;mml:math altimg="si23.svg"&gt;&lt;mml:mrow&gt;&lt;mml
:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;10.7&lt;/mml
:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;) is a key indicator of
solar activity. Accurately forecasting of &lt;mml:math altimg="si24.svg"&gt;&lt;m
ml:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:
mn&gt;10.7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; is crucial
for reducing the impact of solar activity on fields such as radio
communication, navigation, and satellite communication. In this work, we
present a novel channel-independent patch time series Transformer
(PatchTST) for &lt;mml:math altimg="si25.svg"&gt;&lt;mml:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow
&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;10.7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;
&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; forecasting. This is the first time
that the PatchTST model is applied to &lt;mml:math altimg="si26.svg"&gt;&lt;mml:m
row&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;1
0.7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; forecasting. We
construct the &lt;mml:math altimg="si27.svg"&gt;&lt;mml:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;
&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;10.7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;
/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt; dataset, which is measured by the
Dominion Radio Astrophysical Observatory (DRAO) in Canada. We compare
the performance of PatchTST, N-Beats, BiGRU, and CNN-BiGRU on DRAO data.
The root mean squared error (RMSE), mean absolute percentage error
(MAPE), and correlation coefficient (R) of our PatchTST model are 4.731,
2.351%, and 0.986, respectively, which outperforms those of the other
models when the prediction length is 1 day. Especially in mid-term
forecasting, the PatchTST model performs much better than those of the
other models. We make uncertainty analyses on these models, and the
PatchTST model exhibits superior adaptability to model uncertainty
compared to the N-Beats, BiGRU, and CNN-BiGRU. The PatchTST model shows
a 62.9% improvement in mean error (ME) and a 40.5% improvement in
standard mean error (STDE) compared to the benchmark data provided by
Space Environment Technologies (SET). This work also shows that our
PatchTST model generalizes well by applying it to other &lt;mml:math altimg
="si28.svg"&gt;&lt;mml:mrow&gt;&lt;mml:msub&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;F&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;
mml:mrow&gt;&lt;mml:mn&gt;10.7&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msub&gt;&lt;/mml:mrow&gt;&lt;/mml:mat
h&gt; observational data originating from Long and Short-band Solar
Precision Flux Radiotelescope (L&amp;S) in China.</description>
</item>
<item>
<title> Automated classification of solar radio burst type II, III and IV for CALLISTO spectra using physical properties during maximum of solar cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..74.6104A</link>
<description>Continuous observation of solar radio bursts (SRBs) throughout the year
using the CALLISTO spectrometer generates a huge volume of spectral
data. This study introduces a burst-classifier algorithm, which is an
automated algorithm, to classify the SRB spectrum into three solar radio
bursts, namely Type II (SRBT II), Type III (SRBT III) and Type IV (SRBT
IV). The proposed algorithm was designed using four characteristic
parameters derived from a collection of training dataset files. The
characteristic parameters were derived from the intensity bursts
observed on frequency channels and timesteps of the spectrum. This
dataset consisted of 50 spectra of SRBT II and SRBT III, along with 40
spectra for SRBT IV, collected during the solar maximum of 2014 (Solar
Cycle 24). After observations and analysis of the training dataset, each
burst type was set up with a threshold. A training dataset of 80 data
spectra from 2013 to 2016 was used to test the algorithm. Accuracy of
the proposed algorithm was calculated using the percentage of true
positives (TP) and false positives (FP). Findings demonstrate an
accuracy of 74 % with 57 out of 80 spectra classified as TP and 23
spectra as FP.</description>
</item>
<item>
<title> Key Characteristics and Trends</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ARep...68.1335P</link>
<description>This paper presents a statistical analysis of doublet type II radio
bursts, specifically the first type II (type II&lt;SUB&gt;1&lt;/SUB&gt;) and the
second type II (type II&lt;SUB&gt;2&lt;/SUB&gt;), during solar cycles 23 and 24. The
study focuses on radio-rich CMEs that are accompanied by type II solar
radio bursts, covering a period of 15 years from November 1997 to
December 2015. The characteristics of these doublet type II radio bursts
were analyzed using data from the Culgoora radio spectrograph. Key
parameters such as lifetime, start frequency, end frequency, bandwidth,
drift rate, and estimated shock speed (ESS) of both the types of radio
burst were examined. During solar cycles 23 and 24, the start
frequencies of first type II bursts were generally higher than those of
the second type II bursts, suggesting different driving mechanisms for
the two types. A good correlation was found between start frequency and
drift rate throughout the study period, with correlation coefficients of
for solar cycle 23 and  for solar cycle 24. This indicates that doublet
type II radio bursts consistently drift from a high start frequency to a
low end frequency, reflecting the rapid propagation of the shock away
from the sun. However, the correlation between other solar parameters,
such as lifetime, bandwidth, drift rate, and ESS was weak, implying that
various drivers or mechanisms might influence the occurrence of these
radio bursts. Additionally, the ESS of the first type II bursts was
observed to be greater than that of the second type II bursts suggesting
that doublet type II radio bursts may originate from eruptions of
different structures.</description>
</item>
<item>
<title> Radio Spectrum Observations and Studies of the Solar Broadband Radio Dynamic Spectrometer (SBRS)</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Univ...10..440H</link>
<description>Solar radio spectral observation is one of the essential approaches for
solar physics research, which helps us study the plasma dynamics in the
solar atmosphere. The Solar Broadband Radio Dynamic Spectrometer (SBRS)
started observing the Sun at Huairou Solar Observing Station in Beijing,
China, in 1999. It has obtained a large amount of high-quality
observation data of solar radio dynamic spectra in the
centimeterdecimeter wavelengths (1.107.60 GHz). In particular, the
observations with high-temporal resolution of millisecond and high-
frequency resolution of MHz display plenty of superfine structures in
the dynamic spectrum, which provide crucial information on the radiation
process of various radio bursts. We review the past history of solar
radio spectral observation and scientific results of SBRS. It is
meaningful and will undoubtedly help us inspire new ideas for future
research. The understanding of the basic plasma processes in solar
plasma could also promote the development of solar physics,
astrophysics, and space weather. To broaden the observation frequency
range, we propose a new spectrometer at millimeter wavelengths (20100
GHz) with ultra-wideband and high timefrequency resolution to study the
physical processes in the solar transition region. This will open a new
window for solar physics research and will provide crucial observational
evidence for exploring a series of major issues in solar physics,
including coronal heating, solar eruptions, and the origin of solar
winds.</description>
</item>
<item>
<title> Solar Radio Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Univ...10..422T</link>
<description>Not Available</description>
</item>
<item>
<title> Studying the Properties of Spacetime with an Improved Dynamical Model of the Inner Solar System</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Univ...10..413P</link>
<description>Physical properties of the Sun (orientation of rotation axis, oblateness
coefficient J2, and change rate of the gravitational parameter ) are
determined using a dynamical model describing the motion of the Sun,
planets, the Moon, asteroids, and Trans-Neptunian objects (TNOs). Among
the many kinds of observations used to determine the orbits and physical
properties of the bodies, the most important for our study are precise
interplanetary ranging data: EarthMercury ranges from MESSENGER
spacecraft and EarthMars ranges from Odyssey and MRO. The findings
allow us to improve the model of the Sun in modern planetary
ephemerides. First, the dynamically determined direction of the Sun's
pole is 2 off the visible axis of rotation of the Sun's surface, which
is corroborated by present knowledge of the Sun's interior. Second, the
change rate of the Sun's gravitational parameter is found to be smaller
(in absolute value) than the nominal value derived from the estimate of
mass loss through radiation and solar wind. Possible interpretations are
discussed.</description>
</item>
<item>
<title> Aurora Observations and Low Latitude Space Weather Effects in Mexico</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2204111G</link>
<description>On 10 May 2024, a severe geomagnetic storm coinciding with Mother's Day
in Mexico lasted over 40 hr and produced polar auroras observable at low
latitudes. This storm, the most intense since 2003, resulted from a
series of solar flares and coronal mass ejections from active region
3664. The event was significant for space weather studies in Mexico,
marking a milestone by enabling comprehensive measurements of its
effects. The Mexico Space Weather Service (SCIESMEX) and the National
Space Weather Laboratory (LANCE) had prepared for such an event since
their inception. LANCE's instrument networks recorded solar
chromospheric images, solar radio bursts, geomagnetic variations,
Schumann resonances, ionospheric disturbances, and energetic particle
flows. They also monitored Geomagnetically Induced Currents (GICs) in
three strategic substations of the national electrical system. This
provided unprecedented insights into the dynamics of severe space
weather events at the North-American low-latitude environment. Citizen
science efforts documented auroras and regional responses, capturing
variations in geomagnetic indices, ionospheric disturbances, cosmic ray
fluxes, GICs, and technological impacts. SCIESMEX worked with the
National Civil Protection System (SINAPROC) to issue warnings, ensuring
public awareness and preparedness. This coordination underscores the
importance of effective communication and collaboration in mitigating
impacts. The May 2024 geomagnetic storm demonstrated the critical role
of preparedness, research, and public education in reducing the effects
of future space weather events in Mexico.</description>
</item>
<item>
<title> Time-varying trends from Arctic ozonesonde time series in the years 19942022</title>
<link>https://ui.adsabs.harvard.edu/abs/2024NatSR..1427683N</link>
<description>Although evidence of recovery in Antarctic stratospheric ozone has been
found, evidence of recovery in Arctic ozone is still elusive, even
though 25 years have passed since the peak in ozone depleting
substances. Here we have used a Dynamic Linear Model to derive time-
varying trends over 20-year periods in the Arctic ozone time series,
measured in-situ by ozonesondes from 6 stations, from 1994 to 2022. The
model accounts for seasonality, external forcing and 1st-order
correlation in the residuals. As proxies for the external forcing, we
have used tropopause pressure (replaced with Arctic Oscillation in the
troposphere), eddy heat flux, the volume of polar stratospheric clouds
multiplied by effective equivalent stratospheric chlorine, and solar
radio flux at 10.7 cm for the 11-year solar cycle. Our results indicate
that the ozone recovery in the lower Arctic stratosphere is not
detectable. Though significant positive trends have been detected prior
to 2017 at some stations, there are no statistically significant
positive trends after 2017. Moreover, at a number of stations the trends
after 2019 are rather negative and significant, varying between  0.30 
0.25 and  1.00  0.85% per decade. Furthermore, the Arctic troposphere
exhibited only statistically significant negative trends over 20-year
periods ending in 2017 or later, varying between  0.31  0.27 and 
1.76  0.41% per decade. These results highlight the importance of
continued monitoring of the Arctic ozone.</description>
</item>
<item>
<title> An Artificial-Intelligence-Assisted Optimization of Imperceptible Multimode Rectenna</title>
<link>https://ui.adsabs.harvard.edu/abs/2024IAWPL..23.3559H</link>
<description>In this letter, we propose and experimentally demonstrate compact, low-
profile, and optically transparent antennas for multiband and multirange
wireless power transfer (WPT) applications. Specifically, we put forward
new types of transparent multiband antennas that can perform the near-
field reactive WPT (13.56 MHz), as well as the far-field radiative WPT
(980 MHz and 2.45 GHz) within a single device. Furthermore, such an
antenna is integrated with compact frequency-scalable rectifying
circuits to form an unseeable multimode WPT device. We show that a
hybrid inductive (13.56 MHz) and radiative (980 MHz and 2.4 GHz) WPT
device can be realized with a modified inverted-F antenna structure
connected to spiral coil virtual ground. To meet the stringent design
requirements of this unobtrusive multiband antenna, a state-of-the-art
machine-learning-assisted global optimization method (parallel-
surrogate-model-assisted hybrid differential evolution for antenna
optimization) is exploited for global optimization. We envision that the
proposed transparent and flexible WPT and energy harvesting devices can
be beneficial for many applications, including ubiquitous wireless
charging based on smart windows and glasses, solar radio frequency
integrated power supply, wearable or textile electronics, and Internet
of Things.</description>
</item>
<item>
<title> Investigating the Behavior and Spatiotemporal Variations of Green-line Emission in the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJS..275....3O</link>
<description>Understanding coronal structure and dynamics can be facilitated by
analyzing green-line emission, which enables the investigation of
diverse coronal structures such as coronal loops, streamers, coronal
holes, and various eruptions in the solar atmosphere. In this study, we
investigated the spatiotemporal behaviors of green-line emissions in
both low and high latitudes across nine solar cycles, ranging from Solar
Cycle 17 to the current Solar Cycle 25, using the modified homogeneous
data set. We employed methodologies such as cross correlation, power
spectral density, and wavelet transform techniques for this analysis. We
found distinct behaviors in green-line energy across various latitudinal
distributions in the solar atmosphere. The trends observed at higher
latitudes differ from those at lower latitudes. The emission behaviors
show a close association with other solar phenomena like solar flares,
sunspots, and coronal mass ejections throughout the solar cycles. The
observed variations exhibit harmonic periods. The emission activity is
significantly higher in the low latitudes, accounting for over 70% of
the emissions, while the higher latitudes contribute less than 30%. The
emissions exhibit asymmetric behavior between the northern and southern
hemispheres, leading to a 44 yr cycle of solar hemispheric dominance
shifts. Various factors, such as Alfvn waves, solar magnetic fields,
sunspots, differential rotation, and reconnection events, influence the
observed differences in behavior between lower and higher latitudes,
suggesting the existence of potential underlying phenomena contributing
to deviations in properties, intensity, temporal dynamics, and
spatiotemporal lifetime.</description>
</item>
<item>
<title> Direct Measurements of Synchrotron-emitting Electrons at Near-Sun Shocks</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...976L...7J</link>
<description>In this study, we present the first-ever direct measurements of
synchrotron-emitting heliospheric traveling shocks, intercepted by the
Parker Solar Probe (PSP) during its close encounters. Given that much of
our understanding of powerful astrophysical shocks is derived from
synchrotron radiation, these observations by PSP provide an
unprecedented opportunity to explore how shocks accelerate relativistic
electrons and the conditions under which they emit radiation. The
probe's unparalleled capabilities to measure both electromagnetic fields
and energetic particles with high precision in the near-Sun environment
has allowed us to directly correlate the distribution of relativistic
electrons with the resulting photon emissions. Our findings reveal that
strong quasi-parallel shocks emit radiation at significantly higher
intensities than quasi-perpendicular shocks due to the efficient
acceleration of ultrarelativistic electrons. These experimental results
are consistent with theory and recent observations of supernova remnant
shocks and advance our understanding of shock physics across diverse
space environments.</description>
</item>
<item>
<title> Estimating the Total Energy Content in Escaping Accelerated Solar Electron Beams</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...976..128J</link>
<description>Quantifying the energy content of accelerated electron beams during
solar eruptive events is a key outstanding objective that must be
constrained to refine particle acceleration models and understand the
electron component of space weather. Previous estimations have used in
situ measurements near the Earth, and consequently suffer from electron-
beam propagation effects. In this study, we deduce properties of a rapid
sequence of escaping electron beams that were accelerated during a solar
flare on 2013 May 22 and produced type III radio bursts, including the
first estimate of energy density from remote-sensing observations. We
use extreme-ultraviolet observations to infer the magnetic structure of
the source active region NOAA 11745, and Nanay Radioheliograph imaging
spectroscopy to estimate the speed and origin of the escaping electron
beams. Using the observationally deduced electron-beam properties from
the type III bursts and cotemporal hard X-rays, we simulate electron-
beam properties to estimate the electron number density and energy in
the acceleration region. We find an electron density (above 30 keV) in
the acceleration region of 10&lt;SUP&gt;2.5&lt;/SUP&gt; cm&lt;SUP&gt;3&lt;/SUP&gt; and an
energy density of 2  10&lt;SUP&gt;5&lt;/SUP&gt; erg cm&lt;SUP&gt;3&lt;/SUP&gt;. Radio
observations suggest the particles travelled a very short distance
before they began to produce radio emission, implying a radially narrow
acceleration region. A short but plausibly wide slab-like acceleration
volume of 10&lt;SUP&gt;26&lt;/SUP&gt;10&lt;SUP&gt;28&lt;/SUP&gt; cm&lt;SUP&gt;3&lt;/SUP&gt; atop the
flaring loop arcade could contain a total energy of
10&lt;SUP&gt;23&lt;/SUP&gt;10&lt;SUP&gt;25&lt;/SUP&gt; erg (100 beams), which is comparable to
energy estimates from previous studies.</description>
</item>
<item>
<title> Study on the Temporal Evolution of the Radial Differential Rotation of Solar Corona Using Radio Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...976...94X</link>
<description>The daily measurements of the disk-integrated solar radio flux, observed
by the Radio Solar Telescope Network, at 245, 410, 610, 1415, 2695,
4995, and 8800 MHz during the time interval of 1989 January 1 to 2019
December 17, are used to investigate the temporal evolution of radial
differential rotation of the solar corona using the methods of ensemble
empirical mode decomposition (EEMD) and wavelet analysis. Overall, the
results reveal that over the 30 yr period, the rotation rates for the
observed solar radio flux within the frequency range of 2458800 MHz
show an increase with frequency. This verifies the existence of the
radial differential rotation of the solar corona over long timescales of
nearly three solar cycles. Based on the radio emission mechanism, to
some extent, the results can also serve as an indicator of how the
rotation of the solar upper atmosphere varies with altitude within a
specific range. From the temporal variation of rotation cycle lengths of
radio flux, the coronal rotation at different altitudes from the low
corona to approximately 1.3 R &lt;SUB&gt;&lt;/SUB&gt; exhibits complex temporal
variations with the progression of the solar cycle. However, in this
altitude range, over the past 30 yr from 1989 to 2019, the coronal
rotation consistently becomes gradually slower as the altitude
increases. Finally, the EEMD method can extract rotation cycle signals
from these highly randomized radio emissions, and so it can be used to
investigate the rotation periods for the radio emissions at higher or
lower frequencies.</description>
</item>
<item>
<title> Spectral Characteristics of FundamentalHarmonic Pairs of Interplanetary Type III Radio Bursts Observed by PSP</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...975L..37C</link>
<description>Based on the observations by the Parker Solar Probe (PSP) during its
encounter phases of approaching the Sun, I. C. Jebaraj et al. found that
fundamentalharmonic (F-H) pairs constitute a majority of interplanetary
(IP) type III radio bursts. In the present Letter, spectral
characteristics of the IP F-H pairs are identified and analyzed further.
The observations were made with the Radio Frequency Spectrometer (RFS)
experiment on the PSP spacecraft in its encounter phase from the first
to the ninth orbit as it traveled from 0.17 to 0.074 au from the Sun.
The result shows that the occurrence rate of F-H pairs rises
significantly with the rise in the number of IP type III radio bursts
detected by the PSP or the enhancement in the time resolution of the RFS
instrument. In particular, we compare the relationship between F and H
spectral characteristics, such as the frequency-drift rate, emission
intensity, relative bandwidth, duration, and fine structure. The results
will be helpful for us to understand the physics underlying the
generation and evolution of the IP F-H pairs as well as other IP type
III radio bursts.</description>
</item>
<item>
<title> A statistical study</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..74.5263D</link>
<description>In this paper, we present for the first time a comprehensive statistical
study between type II radio bursts from the metric (m) to the
dekamerichectometric (DH) domain and their associated solar and space
weather (SW) phenomena, namely, solar flares (SFs), sunspot (SN)
configurations, filament eruptions, coronal mass ejections (CMEs), their
interplanetary (IP) counterparts (ICMEs) and shocks, in situ detected
particles and geomagnetic storms (GSs). The m-only and m + DH radio
signatures are identified from dynamic spectra provided by the ground-
based RSTN stations distributed over the globe together with Wind/WAVES
satellite data. The DH-only type IIs are adopted from a ready catalog
based on Wind/WAVES spacecraft data. We perform the temporal and spatial
association between the radio emission and the listed above activity
events during solar cycle (SC) 24, separately for the three sub-
categories, m-only, m + DH and DH-only type IIs. A quantitative
assessment on the occurrence rates is presented as a function of the
strength of the specific SW phenomena: highest rates are obtained with
CMEs, SFs, filament eruptions, and SN configurations, whereas a much
weaker relationship is found with ICMEs, IP shocks, energetic particles,
and GSs. The potential of the obtained rates to be used in empirical or
physics-based models for SW forecasting is discussed.</description>
</item>
<item>
<title> Novel scaling laws to derive spatially resolved flare and CME parameters from sun-as-a-star observables</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...691L...8M</link>
<description>Coronal mass ejections (CMEs) are often associated with X-ray (SXR)
flares powered by magnetic reconnection in the low corona, while the CME
shocks in the upper corona and interplanetary (IP) space accelerate
electrons often producing the type II radio bursts. The CME and the
reconnection event are part of the same energy release process as
highlighted by the correlation between reconnection flux
(&lt;SUB&gt;rec&lt;/SUB&gt;) that quantifies the strength of the released magnetic
free energy during the SXR flare, and the CME kinetic energy that drives
the IP shocks leading to type II bursts. Unlike the Sun, these physical
parameters cannot be directly inferred in stellar observations. Hence,
scaling laws between unresolved sun-as-a-star observables, namely SXR
luminosity (L&lt;SUB&gt;X&lt;/SUB&gt;) and type II luminosity (L&lt;SUB&gt;R&lt;/SUB&gt;), and
the physical properties of the associated dynamical events are crucial.
Such scaling laws also provide insights into the interconnections
between the particle acceleration processes across low-corona to IP
space during solar-stellar "flare-CME-type II" events. Using long-term
solar data in the SXR to radio waveband, we derived a scaling law
between two novel power metrics for the flare and CME-associated
processes. The metrics of "flare power" (P&lt;SUB&gt;flare&lt;/SUB&gt; =
(L&lt;SUB&gt;X&lt;/SUB&gt;&lt;SUB&gt;rec&lt;/SUB&gt;)) and "CME power" (P&lt;SUB&gt;CME&lt;/SUB&gt; =
(L&lt;SUB&gt;R&lt;/SUB&gt;V&lt;SUB&gt;CME&lt;/SUB&gt;&lt;SUP&gt;2&lt;/SUP&gt;)), where V&lt;SUB&gt;CME&lt;/SUB&gt; is
the CME speed, scale as P&lt;SUB&gt;flare&lt;/SUB&gt;  P&lt;SUB&gt;CME&lt;/SUB&gt;&lt;SUP&gt;0.76 
0.04&lt;/SUP&gt;. In addition, L&lt;SUB&gt;X&lt;/SUB&gt; and &lt;SUB&gt;rec&lt;/SUB&gt; show power-
law trends with P&lt;SUB&gt;CME&lt;/SUB&gt; with indices of 1.12  0.05 and 0.61 
0.05, respectively. These power laws help infer the spatially resolved
physical parameters, V&lt;SUB&gt;CME&lt;/SUB&gt; and &lt;SUB&gt;rec&lt;/SUB&gt;, from disk-
averaged observables, L&lt;SUB&gt;X&lt;/SUB&gt; and L&lt;SUB&gt;R&lt;/SUB&gt; during solar-
stellar flare-CME-type II events.</description>
</item>
<item>
<title> A type II radio burst associated with solar filamentfilament interaction</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...691A...4Z</link>
<description>Aims. Solar radio type II bursts are often associated with coronal
shocks driven by solar eruptions. In this study, we report a type II
burst associated with filamentfilament interaction. Methods. Combining
the high-quality multiwavelength observations from CHASE, SDO, STEREO,
and CALLISTO, we conducted a detailed study of the type II burst
associated with filamentfilament interaction. Results. On 2023
September 11, an erupting filament (F1) likely disturbed a nearby long
filament (F2), causing F2 to subsequently erupt. As a result of possible
magnetic reconnection between ejective materials from the two filaments,
loop-like structures formed perpendicular to them. Subsequently, the
expansion of these loop-like structures triggered a strong coronal mass
ejection (CME). Interestingly, a type II burst appeared on the solar
spectrum around the time when the loop-like structures formed and the
CME appeared above the occulting disk of STEREO/COR1. By converting the
frequency of the type II burst to the coronal height using polarization
brightness data recorded by the COR1 coronagraph and the spherically
symmetric polynomial approximation technique, we determined the
formation height of the type II burst to be around 1.45 R&lt;SUB&gt;&lt;/SUB&gt;,
with a speed of approximately 440 km s&lt;SUP&gt;1&lt;/SUP&gt;. This is comparable
to the observed height of the CME (1.43 R&lt;SUB&gt;&lt;/SUB&gt;), although
slightly lower in speed (540 km s&lt;SUP&gt;1&lt;/SUP&gt;). Conclusions. All these
results indicate that the type II burst was closely associated with
filamentfilament interactions and was possibly excited by the
accompanying CME at the flank. We suggest that the filamentfilament
interactions played an important role in producing the type II burst by
acting as a piston to trigger a strong CME.</description>
</item>
<item>
<title> Extreme Space Weather Impacts on GNSS Timing Signals for Electricity Grid Management</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2203770E</link>
<description>Extreme space weather events can have serious impacts on critical
infrastructure, including Global Navigation Satellite Systems (GNSS).
The use of GNSS, particularly as sources of accurate timing signals, is
becoming more widespread, with one example being the measurement of
electricity grid frequency and phase information to aid grid management
and stability. Understanding the likelihood of extreme space weather
impacts on GNSS timing signals is therefore becoming vital to maintain
national electricity grid resilience. This study determines critical
intensity thresholds above which the complete failure of a GNSS based
timing system may occur. Solar radio bursts are identified as a simple
example to investigate in more detail. The probability of occurrence of
an extreme space weather event with an intensity equal to or greater
than the critical intensity is estimated. Both a power law and extreme
value theory were used to evaluate recurrence probabilities based on
historical event frequencies. The probability was estimated to be
between 3%-12% per decade to cause the complete failure of any GNSS-
based timing system.</description>
</item>
<item>
<title> Nonlinear Evolution of the Electron Two-Stream Instability</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299..146B</link>
<description>Solar type V radio bursts are associated with type III bursts. Several
processes have been proposed to interpret the association, electron
distribution, and emission. We present the observation of a unique type
V event observed by e-CALLISTO on 7 May 2021. The type V radio emission
follows a group of U bursts. Unlike the unpolarized U bursts, the type V
burst is circularly polarized, leaving room for a different emission
process. Its starting edge drifts to higher frequency four times slower
than the descending branch of the associated U burst. The type V
processes seem to be ruled by electrons of lower energy. The
observations conform to a coherent scenario where a dense electron beam
drives the two-stream instability (causing type III emission) and, in
the nonlinear stage, becomes unstable to another instability, previously
known as the electron firehose instability (EFI). The secondary
instability scatters some beam electrons into velocities perpendicular
to the magnetic field and produces, after particle loss, a trapped
distribution prone to electron cyclotron masering (ECM). A reduction in
beaming and the formation of an isotropic halo are predicted for
electron beams continuing to interplanetary space, possibly observable
by Parker Solar Probe and Solar Orbiter.</description>
</item>
<item>
<title> Galileo and BeiDou AltBOC Signals and Their Perspectives for Ionospheric TEC Studies</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Senso..24.6472C</link>
<description>For decades, GNSS code measurements were much noisier than phase ones,
limiting their applicability to ionospheric total electron content (TEC)
studies. Ultra-wideband AltBOC signals changed the situation. This study
revisits the Galileo E5 and BeiDou B2 AltBOC signals and their potential
applications in TEC estimation. We found that TEC noises are comparable
for the single-frequency AltBOC phase-code combination and those of the
dual-frequency legacy BPSK/QPSK phase combination, while single-
frequency BPSK/QPSK TEC noises are much higher. A two-week high-rate
measurement campaign at the ACRG receiver revealed a mean 100 sec TEC
RMS (used as the noise proxy) of 0.26 TECU, 0.15 TECU, and 0.09 TECU for
the BeiDou B2(a+b) AltBOC signal and satellite elevations 0-30, 30-60,
and 60-90, correspondingly, and 0.22 TECU, 0.14 TECU, and 0.09 TECU for
the legacy B1/B3 dual-frequency phase combination. The Galileo E5(a+b)
AltBOC signal corresponding values were 0.25 TECU, 0.14 TECU, and 0.09
TECU; for the legacy signals' phase combination, the values were 0.19
TECU, 0.13 TECU, and 0.08 TECU. The AltBOC (for both BeiDou and Galileo)
SNR exceeds those of BPSK/QPSK by 7.5 dB-Hz in undisturbed conditions.
Radio frequency interference (the 28 August 2022 and 9 May 2024 Solar
Radio Burst events in our study) decreased the AltBOC SNR 5 dB-Hz more
against QPSK SNR, but, due to the higher initial SNR, the threshold for
the loss of the lock was never broken. Today, we have enough BeiDou and
Galileo satellites that transmit AltBOC signals for a reliable single-
frequency vTEC estimation. This study provides new insights and evidence
for using Galileo and BeiDou AltBOC signals in high-precision
ionospheric monitoring.</description>
</item>
<item>
<title> Ionospheric Absorption Variation Based on Ionosonde and Riometer Data and the NOAA D-RAP Model over Europe During Intense Solar Flares in September 2017</title>
<link>https://ui.adsabs.harvard.edu/abs/2024RemS...16.3975B</link>
<description>A novel method was developed based on the amplitude data of the EM waves
measured by Digisondes to calculate and investigate the relative
ionospheric absorption changes. The effect of 13 solar flares (&gt;C8) that
occurred from 4 to 10 September 2017 were studied at three European
Digisonde stations (Juliusruh (54.63N, 13.37E), Prhonice (49.98N,
14.55E) and San Vito (40.6N, 17.8E)). The present study compares the
results of the amplitude method with the absorption changes measured by
the Finnish Riometer Network and determined by the NOAA D-RAP model
during the same events. The X-class flares caused 1.5-2.5 dB of
attenuation at 30-32.5 MHz based on the riometer data, while the
absorption changes were between 10 and 15 dB in the 2.5-4.5 MHz
frequency range according to the amplitude data. The impact caused by
energetic particles after the solar flares are clearly seen in the
riometer data, while among the Digisonde stations it can be observed
only at Juliusruh in some certain cases. Comparing the results of the
amplitude method with the D-RAP model it seems evident that the observed
absorption values almost always exceed the values given by the model
both at 2.5 MHz and at 4 MHz during the investigated period. According
to the comparison between the riometer data with the D-RAP, generally,
the model underestimates the absorption values obtained from the
riometers during solar flares except at the highest latitude stations,
while D-RAP overestimates the impact during the particle events.</description>
</item>
<item>
<title> Trends in Ionospheric Solar Activity Indices</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64..647D</link>
<description>The article presents the first results of identifying trends in annual
average ionospheric indices IG&lt;SUB&gt;12&lt;/SUB&gt; and T&lt;SUB&gt;12&lt;/SUB&gt;, which
are obtained after excluding from IG&lt;SUB&gt;12&lt;/SUB&gt; and T&lt;SUB&gt;12&lt;/SUB&gt; the
dependence of these indices on solar activity indices. In this case,
solar activity indices are F10 and F30solar radio emission fluxes at
10.7 and 30 cm. It was found that for the interval of 19572023, all
analyzed linear trends are negative, i.e., quantities IG&lt;SUB&gt;12&lt;/SUB&gt;
and T&lt;SUB&gt;12&lt;/SUB&gt; decrease over time, and these trends are
significant. In absolute value, they are maximum for IG&lt;SUB&gt;12&lt;/SUB&gt;,
taking into account the IG&lt;SUB&gt;12&lt;/SUB&gt; dependence on F10&lt;SUB&gt;12&lt;/SUB&gt;,
and minimum for T&lt;SUB&gt;12&lt;/SUB&gt;, taking into account the T&lt;SUB&gt;12&lt;/SUB&gt;
dependence on F30&lt;SUB&gt;12&lt;/SUB&gt;. Account for the nonlinearity of trends
shows that, e.g., after 2010, they intensified. Relations are presented
that make it possible, based on data from trends of the ionospheric
indices (IG&lt;SUB&gt;12&lt;/SUB&gt; or T&lt;SUB&gt;12&lt;/SUB&gt;), to judge the nature of
the  foF2 trend over a specific point. For this, using the IRI model
for foF2, a coefficient was obtained that gives the relationship between
the trends of the ionospheric index and  foF2 over this point.
Comparison with experimental data at mid-latitudes revealed that trends
of the ionospheric indices make it possible to correctly determine the
sign of the  foF2 trend and the general tendency for this trend change,
but the calculated value of the trend over a specific point may differ
markedly from the experimental data.</description>
</item>
<item>
<title> Temporally Resolved Type III Solar Radio Bursts in the Frequency Range 313 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...974L..18V</link>
<description>Radio observations from space allow to characterize solar radio bursts
below the ionospheric cutoff, which are otherwise inaccessible, but
suffer from low, insufficient temporal resolution. In this Letter we
present novel, high-temporal resolution observations of type III solar
radio bursts in the range 313 MHz. A dedicated configuration of the
Radio and Plasma Waves (RPW) High Frequency Receiver (HFR) on the Solar
Orbiter mission, allowing for a temporal resolution as high as 0.07 s
(up to 2 orders of magnitude better than any other spacecraft
measurements), provides for the very first time resolved measurements of
the typical decay time values in this frequency range. The comparison of
data with different time resolutions and acquired at different radial
distances indicates that discrepancies with decay time values provided
in previous studies are only due to the insufficient time resolution not
allowing to accurately characterize decay times in this frequency range.
The statistical analysis on a large sample of 500 type III radio bursts
shows a power low decay time trend with a spectral index of 0.75  0.03
when the median values for each frequency are considered. When these
results are combined with previous observations, referring to
frequencies outside the considered range, a spectral index of 1.00 
0.01 is found in the range 0.05300 MHz, compatible with the presence
of radio-wave scattering between 1 and 100 R &lt;SUB&gt;&lt;/SUB&gt;.</description>
</item>
<item>
<title> Implications for Turbulence and Electron Acceleration</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...973...96A</link>
<description>The excess broadening of high-temperature spectral lines, long observed
near the tops of flare arcades, is widely considered to result from
magnetohydrodynamic turbulence. According to different theories, plasma
turbulence is also believed to be a candidate mechanism for particle
acceleration during solar flares. However, the degree to which this
broadening is connected to the acceleration of nonthermal electrons
remains largely unexplored outside of recent work, and many observations
have been limited by limited spatial resolution and cadence. Using the
Interface Region Imaging Spectrometer, we present spatially resolved
observations of loop-top (LT) broadenings using hot (11 MK) Fe XXI
1354.1  line emission at 9 s cadence during the 2022 March 30 X1.3
flare. We find nonthermal velocities upward of 65 km s&lt;SUP&gt;1&lt;/SUP&gt; that
decay linearly with time, indicating the presence and subsequent
dissipation of plasma turbulence. Moreover, the initial Fe XXI signal
was found to be cospatial and cotemporal with microwave emission
measured by the Expanded Owens Valley Solar Array, placing a population
of nonthermal electrons in the same region as the LT turbulence.
Evidence of electron acceleration at this time is further supported by
hard X-ray measurements from the Spectrometer/Telescope for Imaging
X-rays on board Solar Orbiter. Using the decay of nonthermal broadenings
as a proxy for turbulent dissipation, we found the rate of energy
dissipation to be consistent with the power of nonthermal electrons
deposited into the chromosphere, suggesting a possible connection
between turbulence and electron acceleration.</description>
</item>
<item>
<title> Real-time automated detection of multi-category solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369...99D</link>
<description>Accurate real-time solar radio burst (SRB) detection is crucial for
solar physics research and space weather forecasting. Currently, most
studies on solar radio burst detection focus on single-category
identification and simple discrimination of bursts. There are limited
existing studies on multi-category detection. This paper proposes a
real-time multi-category solar radio burst detection method to meet the
requirements of real-time detection, detection accuracy, and
classification accuracy in solar radio bursts. First, solar radio burst
spectrums were collected from e-CALLISTO. The spectrums are labeled
using LabelImg, and a dataset containing solar radio bursts of Type II,
Type III, Type IIIs, Type IV, and Type V was established. Second, a
full-dimensional dynamic convolution was introduced in the backbone
module of the YOLOv8n model, enhancing the model's feature extraction
capability. Third, a multi-scale feature fusion network based on
ConvNeXt was created to prevent feature information loss and optimize
the loss function. The experimental results show that the proposed
method achieves an average detection accuracy of 82.4% on the
established solar radio burst dataset. Compared with the original
YOLOv8n model, the accuracy increased by 3.5%. Additionally, the model
operates at 140.9 frames per second, with each frame representing a
spectrum of 15 minutes duration. Thus, the improved YOLOv8n model
enhances the detection accuracy and speed of solar radio bursts,
enabling automatic detection and localization of solar radio bursts of
Type II, Type III, Type IIIs, Type IV, and Type V.</description>
</item>
<item>
<title> C6.2 class flare parameters inferred with a 3D geometry of flare database</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..74.4210C</link>
<description>We analysed a GOES C6.2 class solar flare that occurred on 27 October
2003 at the heliographic position S20E29. Utilising a database developed
from a simplified 3D magnetic loop model, we inferred a set of geometric
and physical parameters to characterise the flare. This model, based on
general properties of known solar flares and adjusted for instrument
resolution, was used to replicate observations from the Nobeyama Radio
Polarimeter (NoRP) spectra and the Nobeyama Radioheliograph (NoRH)
brightness maps. We identified a possible range of parameters by
comparing observed spectra and brightness distribution maps with
modelled counterparts. The analysis involved computing a weighted mean
of the one hundred best-fit model parameters, ranked by increasing
&lt;mml:math altimg="si48.svg"&gt;&lt;mml:mrow&gt;&lt;mml:msup&gt;&lt;mml:mrow&gt;&lt;mml:mi&gt;&lt;/mml
:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;2&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msup&gt;&lt;/mml:m
row&gt;&lt;/mml:math&gt; values.Across six discrete time intervals representing
the gradual, impulsive, and decay phases of the flare, we observed
slight variations in values for ten analysed parameters, with notable
exceptions at the burst maxima, including an energy spectral index of
approximately &lt;mml:math altimg="si49.svg"&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:mo&gt;&lt;m
ml:mn&gt;2.34&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, a photospheric magnetic field
strength of around &lt;mml:math altimg="si50.svg"&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;&lt;/mml:
mo&gt;&lt;mml:mn&gt;2&lt;/mml:mn&gt;&lt;mml:mspace width="0.12em"&gt;&lt;/mml:mspace&gt;&lt;mml:mn&gt;308
&lt;/mml:mn&gt;&lt;mml:mi&gt;G&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;, and a non-thermal
electron density of about &lt;mml:math altimg="si51.svg"&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;
&lt;/mml:mo&gt;&lt;mml:msup&gt;&lt;mml:mrow&gt;&lt;mml:mn&gt;10&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;m
ml:mn&gt;7.11&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msup&gt;&lt;mml:msup&gt;&lt;mml:mrow&gt;&lt;mml:mi mat
hvariant="italic"&gt;cm&lt;/mml:mi&gt;&lt;/mml:mrow&gt;&lt;mml:mrow&gt;&lt;mml:mo&gt;-&lt;/mml:mo&gt;&lt;mml
:mn&gt;3&lt;/mml:mn&gt;&lt;/mml:mrow&gt;&lt;/mml:msup&gt;&lt;/mml:mrow&gt;&lt;/mml:math&gt;. In general,
our results replicated the soft-hard-soft behaviour in the gradual-peak-
decay phases of a solar flare. Therefore, we infer that the physical
parameters (magnetic field strength, energy spectral index, and non-
thermal electron density) were accurately recovered. However, fitting
geometric parameters such as inclination, asymmetry, azimuth, loop
radius, loop height, and footpoint separation proved challenging due to
the limited resolution of the instruments, which affects the precise
determination of loop-like flare geometries.</description>
</item>
<item>
<title> Origin of the type III radiation observed near the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690L...6M</link>
<description>Aims. We investigate processes associated with the generation of type
III radiation using Parker Solar Probe measurements. Methods. We
measured the amplitudes and phase velocities of electric and magnetic
fields and their associated plasma density fluctuations. Results. 1.
There are slow electrostatic waves near the Langmuir frequency and at as
many as six harmonics, the number of which increases with the amplitude
of the Langmuir wave. Their electrostatic nature is shown by
measurements of the plasma density fluctuations. From these density
fluctuations and the electric field magnitude, the k-value of the
Langmuir wave is estimated to be 0.14 and k&lt;SUB&gt;d&lt;/SUB&gt; = 0.4. Even
with the large uncertainty in this quantity (more than a factor of two),
the phase velocity of the Langmuir wave was &lt; 10 000 km/s. 2. The
electromagnetic wave near the Langmuir frequency has a phase velocity
lower than 50 000 km/s. 3. We cannot determine whether there are
electromagnetic waves at the harmonics of the Langmuir frequency. If
they existed, their magnetic field components would be below the noise
level of the measurement. 4. The rapid (less than one millisecond)
amplitude variations typical of the Langmuir wave and its harmonics are
artifacts resulting from the addition of two waves, one of which has
small frequency variations that arise because the wave travels through
density irregularities. None of these results are expected in or
consistent with the conventional model of the three-wave interaction of
two counter-streaming Langmuir waves that coalesce to produce the type
III wave. They are consistent with a new model in which electrostatic
antenna waves are produced at the harmonics by radiation of the Langmuir
wave, after which at least the first harmonic wave evolved through
density irregularities such that its wave number decreased and it became
the type III radiation.</description>
</item>
<item>
<title> Magnetic structure, confinement, and escape into the heliosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690A.382K</link>
<description>Context. Filament eruptions and coronal mass ejections (CMEs) reveal
large-scale instabilities of magnetic structures in the solar corona.
Some of them are accompanied by radio emission, which at decimetric and
longer wavelengths is a signature of electron acceleration that may be
different from the acceleration in impulsive flares. The radio emission
is part of the broadband continua at decimetre and metre wavelengths
called type IV bursts. Aims. In this article we investigate a
particularly well-observed combination of a filament eruption seen in H
and at extreme ultraviolet (EUV) wavelengths and a moving type IV burst
on 2021 August 24. The aim is to shed light on the relationship between
the large-scale erupting magnetic structure and the acceleration and
transport of non-thermal electrons. Methods. We used imaging
observations of a moving radio source and associated burst groups with
the refurbished Nanay Radioheliograph and whole-Sun radio spectrography
from different ground-based and space-borne instruments, in combination
with X-ray, radio, and in situ electron observations at tens of keV from
Solar Orbiter and EUV imaging by SDO/AIA. The radio sources are located
with respect to the erupting magnetic structure traced by the filament
(EUV 30.4 nm), and the timing of the electrons detected in situ is
compared with the timing of the different radio emissions. Results. We
find that the moving radio source is located at the top of the erupting
magnetic structure outlined by the filament, which we interpret as a
magnetic flux rope. The flux rope erupts in a strongly non-radial
direction, guided by the overlying magnetic field of a coronal hole. The
electrons detected at Solar Orbiter are found to be released mainly in
two episodes, 1040 minutes after the impulsive phase. The releases
coincide with two groups of radio bursts, which originate respectively
on the flank and near the top of the erupting flux rope. Conclusions.
The observation allows an unusually clear association between a moving
type IV radio burst, an erupting magnetic flux rope as core structure of
a CME, and particle releases into the heliosphere. Non-thermal electrons
are confined in the flux rope. Electrons escape to the heliosphere
mainly in two distinct episodes, which we relate to magnetic
reconnection between the flux rope and ambient open field lines.</description>
</item>
<item>
<title> Slowly positively drifting bursts generated by large-scale magnetic reconnection</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690A.241Z</link>
<description>Context. The slowly positively drifting bursts (SPDBs) are rarely
observed in radio emission of solar flares. Aims. To understand how the
SPDBs are generated, we studied the radio observations at 6005000 MHz
together with the imaging observations made in ultraviolet (UV) and
extreme ultraviolet (EUV) during the SPDB-rich C8.7 flare of 2014 May 10
(SOL2014-05-10T0702). Methods. Because the SPDBs propagate towards
locations of higher plasma density, we studied their associations with
individual flare kernels, located either within the flare core itself,
or distributed at longer distances, but connected to the flaring region
by large-scale hot loops. For each kernel we constructed light curves
using 1600  and 304  observations and compared these light curves with
the temporal evolution of radio flux at 1190 MHz, representing all
observed groups of SPDBs. We also analysed the UV/EUV observations to
understand the evolution of magnetic connectivity during the flare.
Results. The flare starts with a growing hot sigmoid observed in 131 .
As the sigmoid evolves, it extends to and interacts with a half dome
present within the active region. The evolving sigmoid reconnects at the
respective hyperbolic flux tube, producing large-scale magnetic
connections and an EUV swirl. Three groups of SPDBs are observed during
this large-scale magnetic reconnection, along with a group of narrow-
band type III bursts. The light curves of a kernel corresponding to the
footpoint of spine line analogue show good agreement with the radio flux
at 1190 MHz, indicating that the SPDBs are produced by the large-scale
magnetic reconnection at the half dome. In addition, one of the kernels
appeared in the neighbouring active region and also showed a similar
evolution to the radio flux, implying that beams of accelerated
particles can synchronize radio and UV/EUV light curves across
relatively large distances.</description>
</item>
<item>
<title> Modelling non-radially propagating coronal mass ejections and forecasting the time of their arrival at Earth</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690A.137V</link>
<description>We present the study of two solar eruptive events observed on December 7
2020 and October 28 2021. Both events were associated with full halo
coronal mass ejections (CMEs) and flares. These events were chosen
because they show a strong non-radial direction of propagation in the
low corona and their main propagation direction observed in the inner
heliosphere is not fully aligned with the Sun-Earth line. This
characteristic makes them suitable for our study, which aims to inspect
how the non-radial direction of propagation in the low corona affects
the time of CMEs' arrival at Earth. We reconstructed the CMEs using
SOHO/LASCO and STEREO/COR observations and modelled them with the 3D MHD
model EUHFORIA and the cone model for CMEs. In order to compare the
accuracy of forecasting the CME and the CME-driven shock arrival time at
Earth obtained from different methods, we also used so-called type II
bursts, radio signatures of associated shocks, to find the velocities of
the CME-driven shocks and forecast the time of their arrival at Earth.
Additionally, we estimated the CME arrival time using the 2D CME
velocity obtained from the white light images. Our results show that the
lowest accuracy of estimated CME Earth arrival times is found when the
2D CME velocity is used (time difference between observed and modelled
arrival time, t  29 h and 39 h, for the two studied events,
respectively). The velocity of the type II radio bursts provides
somewhat better  but still not very accurate  results (t  +21 h and
29 h, for the two studied events, respectively). Employing, as an input
to EUHFORIA, the CME parameters obtained from the graduated cylindrical
shell (GCS) fittings at consequently increasing heights, results in a
strongly improved accuracy of the modelled CME and shock arrival time;
t changes from 20 h to 10 min in the case of the first event, and from
12 h to 30 min in the case of the second one. This improvement shows
that when we increased the heights of the GCS reconstruction we
accounted for the change in the propagation direction of the studied
CMEs, which allowed us to accurately model the CME flank encounter at
Earth. Our results show the great importance of the change in the
direction of propagation of the CME in the low corona when modelling
CMEs and estimating the time of their arrival at Earth.</description>
</item>
<item>
<title> Effect of temperature anisotropy formed by fast electron beams moving in the flare loop on its excited electron-cyclotron maser instability</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690A..96T</link>
<description>Context. The electron-cyclotron maser instability (ECMI) is a
significant coherent radio emission mechanism widely utilized in various
astrophysical radio phenomena. It is well known that the velocity
anisotropic distribution of energetic electrons, which leads to an
inverted perpendicular population in the vertical direction with
f&lt;SUB&gt;b&lt;/SUB&gt;/v&lt;SUB&gt;&lt;/SUB&gt; &gt; 0, can provide the free energy necessary
for the ECMI. Aims. The initial velocity distribution of energetic
electrons leaving the acceleration region is typically isotropic or
beam-like. However, as these energetic electrons travel along the
magnetic field as fast electron beams (FEBs) in magnetic plasma, various
velocity anisotropic distributions can emerge. In this paper, we examine
the impact of temperature anisotropy formed by beam electrons traveling
along a flare loop on the ECMI. Methods. By neglecting the energy loss
of energetic electrons as they traverse the corona and invoking the
conservation of energy and magnetic moments, we established the
relationship between momentum dispersion and the magnetic field.
Utilizing the magnetic field model of the flare loop, we calculated the
evolution of momentum dispersion and the growth rates of the ECMI as
FEBs precipitate along the flare loop. Results. The results demonstrate
that the temperature anisotropy arising as FEBs descend along the flare
loop significantly impacts the ECMI. The maximum growth rates of the
excited modes exhibit a gradual increase initially and then decline
rapidly after reaching a critical height for &lt;SUB&gt;0&lt;/SUB&gt; = 0.2c and
0.15c. The results also show that the growth rates of the O2 mode are
one order of magnitude smaller than those of the O1 and X2 modes. This
indicates that the harmonic radiation is X-mode polarized. Notably, the
temperature anisotropy of FEBs as they precipitate along the flare loop
with different magnetic field models or at different heights has similar
effects on the ECMI.</description>
</item>
<item>
<title> Long-period energy releases during a C2.8 flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...690A..39L</link>
<description>Context. The study of quasi-periodic pulsations (QPPs) is a key
diagnostic of intermittent or periodic energy releases during solar
flares. Aims. We investigated the intermittent energy-releasing
processes by analyzing the long-period pulsations during a C2.8 flare on
2023 June 3. Methods. The solar flare was simultaneously observed by the
solar X-ray detector on board the Macau Science Satellite-1B, the
Geostationary Operational Environmental Satellite, the Chinese H Solar
Explorer, the Expanded Owens Valley Solar Array, the Atmospheric Imaging
Assembly, and the Extreme Ultraviolet Variability Experiment for the
Solar Dynamics Observatory. Results. The C2.8 flare shows three
successive and repetitive pulsations in soft X-ray (SXR) and high-
temperature extreme ultraviolet (EUV) emissions, which may imply three
episodes of energy releases during the solar flare. The QPP period is
estimated to be as long as 7.5 minutes. EUV imaging observations
suggest that these three pulsations come from the same flare area
dominated by the hot loop system. Conversely, the flare radiation in
wavelengths of radio/microwave, low-temperature EUV, ultraviolet (UV),
and H only reveals the first pulsation, which may be associated with
nonthermal electrons accelerated by magnetic reconnection. The other two
pulsations in wavelengths of SXR and high-temperature EUV might be
caused by the loop-loop interaction. Conclusions. Our observations
indicate that the three episodes of energy releases during the C2.8
flare are triggered by different mechanisms, namely the accelerated
electron via magnetic reconnection, and the loop-loop interaction in a
complicated magnetic configuration.</description>
</item>
<item>
<title> MEMPSEP-III. A Machine Learning-Oriented Multivariate Data Set for Forecasting the Occurrence and Properties of Solar Energetic Particle Events Using a Multivariate Ensemble Approach</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2203765M</link>
<description>We introduce a new multivariate data set that utilizes multiple
spacecraft collecting in-situ and remote sensing heliospheric
measurements shown to be linked to physical processes responsible for
generating solar energetic particles (SEPs). Using the Geostationary
Operational Environmental Satellites (GOES) flare event list from Solar
Cycle (SC) 23 and part of SC 24 (1998-2013), we identify 252 solar
events (&gt;C-class flares) that produce SEPs and 17,542 events that do
not. For each identified event, we acquire the local plasma properties
at 1 au, such as energetic proton and electron data, upstream solar wind
conditions, and the interplanetary magnetic field vector quantities
using various instruments onboard GOES and the Advanced Composition
Explorer spacecraft. We also collect remote sensing data from
instruments onboard the Solar Dynamic Observatory, Solar and
Heliospheric Observatory, and the Wind solar radio instrument WAVES. The
data set is designed to allow for variations of the inputs and feature
sets for machine learning (ML) in heliophysics and has a specific
purpose for forecasting the occurrence of SEP events and their
subsequent properties. This paper describes a data set created from
multiple publicly available observation sources that is validated,
cleaned, and carefully curated for our ML pipeline. The data set has
been used to drive the newly-developed Multivariate Ensemble of Models
for Probabilistic Forecast of SEPs (MEMPSEP; see MEMPSEP-I (Chatterjee
et al., 2024, &lt;A HREF="https://doi.org/10.1029/2023SW003568"&gt;https://doi
.org/10.1029/2023SW003568&lt;/A&gt;) and MEMPSEP-II (Dayeh et al., 2024, &lt;A HR
EF="https://doi.org/10.1029/2023SW003697"&gt;https://doi.org/10.1029/2023SW
003697&lt;/A&gt;) for accompanying papers).</description>
</item>
<item>
<title> Comparative Study of Solar Rotation of Transition Region and Corona using Solar Irradiance and Radio Flux</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299..130K</link>
<description>We study the temporal variation of solar rotation profiles based on
solar irradiance at 93.5 nm and solar radio flux at 10.7 cm originating
from the transition region and lower corona, respectively. The
autocorrelation technique is used to calculate the period in periodic
time series data. The sidereal rotation periods for normalized and
detrended data are studied for 2011  2021. The sidereal rotation
periods for solar irradiance and radio flux for 2011  2021 vary from
22.75 to 26.17 days and 19.42 to 28.14 days, respectively. The mean of
the sidereal rotation periods for solar irradiance and radio flux are
24.76 and 23.76 days, respectively. The mean sidereal rotation period
for solar irradiance is higher than the mean sidereal rotation period
for solar radio flux. The sidereal rotation period for solar irradiance
is greater than or equal to the sidereal rotation period for solar radio
flux for almost all the years between 2011 and 2021. It is found that
the lower corona rotates faster than the transition region during 2011 
2021, i.e., the lower corona is found to be moving 4% faster than the
transition region during 2011  2021. We found a linear relationship
between the normalized daily irradiance and radio flux with a
correlation coefficient of 0.986. Using cross-correlation analysis, we
investigated a phase relationship between solar irradiance and radio
flux and found no time lag between solar irradiance and radio flux.</description>
</item>
<item>
<title> A Discussion of First Proton Arrival Times in Wide-Spread Solar Energetic Particle Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299..126P</link>
<description>This work analyzes the appearance of wide-spread deka-MeV solar
energetic proton (SEP) events, in particular the arrival of the first
protons within  4.5  45 MeV measured at EarthSun L1, and their
relationship with their relative solar source longitude. The definition
of "wide-spread SEP event" for this study refers to events that are
observed as a 25 MeV proton intensity increase at near 1 AU locations
that are separated by at least 130&lt;SUP&gt;&lt;/SUP&gt; in solar longitude. Many
of these events are seen at all three of the spacecraft, STEREO (Solar-
Terrestrial Relations Observatory) A, STEREO B, and SOHO (Solar and
Heliospheric Observatory), and may therefore extend far beyond
130&lt;SUP&gt;&lt;/SUP&gt; in longitude around the Sun. A large subset of these
events have already been part of a study by Richardson et al. (Solar
Phys., 289, 3059, 2014). The event source region identifications draw
from this study; more recent events have also been added. Our focus is
on answering two specific questions: (1) What is the maximum longitude
over which SEP protons show energy dispersion, i.e., a clear sign of
arrival of higher-energy protons before those of lower energy? (2) What
implications can be drawn from the ensemble of events observed regarding
either direct magnetic connectivity to shocks and/or cross-field
transport from the site of the eruption in the onset phase of the event?</description>
</item>
<item>
<title> Heating manifestations at the onset of the 29 June 2012 flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024STP....10c..11M</link>
<description>Analysis of GOES data for the SOL2012-06-29T04:09 flare, class C4.6,
shows a thermal character of the energy release for several minutes
before the impulsive stage. Plasma heating to temperatures above 10 MK
leads to the appearance of plasma jets along open field lines and in
large loops. This work examines the relationship between the heated
plasma and the flare structure and its dynamics, using observations in
the X-ray, extreme ultraviolet (EUV), and radio-wave ranges. Particular
attention is drawn to the detection of narrow-band fine temporal
structures of radio emission before and after the impulsive stage of the
flare in dynamic spectra. In the initial stage, broadband pulses in the
decimeter range are observed which can be associated with the formation
of thermal fronts in the jets. A series of super-bright drifting bursts
in the centimeter range occurs after the end of the impulsive energy
release in the flare kernel. Using data from the Siberian Solar Radio
Telescope (5.7 GHz), we managed to localize the position of the source
of the fine structure of drifting bursts at the remote footpoint of the
large-scale flare loop.</description>
</item>
<item>
<title> A Novel Two-dimensional Low-redundancy Array Design for Solar Radio Imaging</title>
<link>https://ui.adsabs.harvard.edu/abs/2024RAA....24i5016Z</link>
<description>The radioheliograph is an extensive array of antennas operating on the
principle of aperture synthesis to produce images of the Sun. The image
acquired by the telescope results from convoluting the Sun's true
brightness distribution with the antenna array's directional pattern.
The imaging quality of the radioheliograph is affected by a multitude of
factors, with the performance of the "dirty beam" being simply one
component. Other factors such as imaging methods, calibration
techniques, clean algorithms, and more also play a significant influence
on the resulting image quality. As the layout of the antenna array
directly affects the performance of the dirty beam, the design of an
appropriate antenna configuration is critical to improving the imaging
quality of the radioheliograph. Based on the actual needs of observing
the Sun, this work optimized the antenna array design and proposed a
two-dimensional low-redundancy array. The proposed array was compared
with common T-shaped arrays, Y-shaped arrays, uniformly spaced circular
arrays, and three-arm spiral arrays. Through simulations and
experiments, their performance in terms of sampling point numbers, UV
coverage area, beam-half width, sidelobe level, and performance in the
absence of antennas are compared and analyzed. It was found that each of
these arrays has its advantages, but the two-dimensional low-redundancy
array proposed in this paper performs best in overall evaluation. It has
the shortest imaging calculation time among the array types and is
highly robust when antennas are missing, making it the most suitable
choice.</description>
</item>
<item>
<title> System for control of the power of an on-board signal generator of an unmanned aerial vehicle</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MeasT..67..460Z</link>
<description>We consider the issues of calibration of the transmission coefficient of
an antenna system of the ground station used for monitoring of the
energy characteristics of signals from global navigation satellite
systems. We present the most commonly used method intended for
calibration according to the solar radio-emission of the transmission
coefficient of large-aperture reflector antenna systems used as basic in
the construction of ground control stations. We describe the advantages
and disadvantages of the method of calibration according to the radio-
emission. To eliminate the disadvantages of calibration based on solar
radio-emission (the limited range of working elevation angles and the
necessity of using third-party data on the spectral intensity of solar
radio-emission), it is proposed to consider an alternative approach,
namely, the calibration based on the use of an artificial source of
radio-emission placed on board of an unmanned aerial vehicle. The
specific features of this approach, namely, the necessity of operation
in the near-field zone of the investigated antenna system and the motion
of an artificial source of radio-emission in a plane parallel to the
aperture plane of the antenna system, are indicated. We develop a block
diagram of the payload of an unmanned aerial vehicle for measuring in
the near-field zone of the analyzed antenna system. We present the
results of investigations of the characteristics of a payload signal
generator of an unmanned aerial vehicle. We propose a solution, which
eliminates the error in specifying the output power of the signal
generator (the difference between the nominal and actual signal power)
according to the results of measurement. The necessity of using a
control signal power meter and a bandpass filter as components of the
payload is demonstrated. A system for monitoring of the output power of
signal generator is designed. The components of the payload satisfying
the restrictions imposed on the weight and size characteristics are
selected. The possibility of remote connection of an operator to the
payload equipment of an unmanned aerial vehicle is realized. We also
describe the prospects of subsequent development of the payload model.</description>
</item>
<item>
<title> Relationship between microwave and metre ranges during an impulsive solar flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.533.1453S</link>
<description>An analysis of solar flares with simple temporal structures can help us
to understand the features and mechanisms of energy and particle
propagation. A weak impulsive solar flare that occurred on 2021 June 3
provided such opportunity. For the purposes of the study, we used
microwave observations with spatial resolution from the Siberian
Radioheliograph (3-6 GHz) combined with various spectral radio and X-ray
data. Flare topology analysis revealed a configuration consisting of a
small loop or dome-like structure associated with a compact bright
source, and a long high loop system associated with the diffuse source.
This indicates a compact and relatively low-lying site of acceleration
and initial energy release. The radio metre and the microwave emission
demonstrated a peak-to-peak correlation in three of the four bursts. The
delays obtained from comparing microwave and metre radio ranges are in
good agreement with the delays from the metre dynamic spectrum analysis,
but the different radio bursts had different delays. We found that the
electron energies derived from metre dynamic spectrum analysis are lower
than those shown by hard X-ray emissions. According to the results of
theoretical simulations, this can be explained by the expansion of
magnetic loops with altitude. The difference in drift velocities for
various radio bursts can be the result of the different size of the loop
where the electron beams are propagated. This can be a feature related
to the configuration type of the studied flare.</description>
</item>
<item>
<title> Unraveling the Origins of an Extreme Solar Eruptive Event with Hard X-Ray Imaging Spectroscopy</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...972...48V</link>
<description>Hard X-ray (HXR) observations are crucial for understanding the
initiation and evolution of solar eruptive events, as they provide a key
signature of flare-accelerated electrons and heated plasma. The
potential of high-cadence HXR imaging for deciphering the erupting
structure, however, has not received adequate attention in an era of
extreme ultraviolet (EUV) imaging abundance. An extreme solar eruptive
event on 2022 September 5 observed on the solar far side by both Parker
Solar Probe and Solar Orbiter provides the opportunity to showcase the
power of HXR imaging in the absence of high-cadence EUV imaging. We
investigate the evolution of flare energy release through HXR timing,
imaging, and spectral analyses using data from the
Spectrometer/Telescope for Imaging X-rays (STIX) on board Solar Orbiter.
STIX provides the highest cadence imaging of the energy release sites
for this far-side event and offers crucial insight into the nature of
energy release, timing of flare particle acceleration, and evolution of
the acceleration efficiency. We find that this is a two-phase eruptive
event, rather than two distinct eruptions, as has been previously
suggested. The eruption begins with an initial peak in flare emission on
one side of the active region (AR), marking the rise/destabilization of
a loop system followed by notable episodes of energy release across the
AR and an eruptive phase associated with a very fast coronal mass
ejection, type III radio bursts, and solar energetic particles. We
demonstrate that high-cadence HXR imaging spectroscopy is indispensable
for understanding the formation of powerful, space-weather relevant
eruptions.</description>
</item>
<item>
<title> Time Profile Study of Type III Solar Radio Bursts Using Parker Solar Probe</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...972....2T</link>
<description>Solar type III radio bursts are crucial indicators of energetic electron
activity in the solar corona and interplanetary space. Our assessment of
43 interplanetary type III bursts, recorded by the FIELDS instrument on
board the Parker Solar Probe during Encounters 05 to 11, has led to
significant and complex findings. We have analyzed time profile features
across a frequency range of 190.5 MHz, revealing dependencies on
frequency and providing insights into duration, burst speeds,
bandwidths, and drift rates. This novel analysis has unveiled a spectral
index of 0.63  0.04 for rise, 0.69  0.03 for decay time, and 0.68 
0.03 for the total duration. We have determined the average electron
beam velocities for front, middle, and back as 0.15c, 0.13c, and 0.08c,
respectively. Our findings show that faster electron beams generate
emissions with shorter duration. The average ratio of the front-to-back
velocity is 1.87, and the ratio of front-to-middle velocity is 1.23. We
have also discovered a strong relationship between burst duration with
rise, peak, and decay times, particularly pronounced with decay time
(correlation coefficient = 0.95). This indicates that the entire
temporal profile, including rise, peak, and decay phases, collectively
contributes to event duration and is not solely influenced by external
factors like plasma conditions or electron beam dynamics but also by
internal burst processes. These complex findings shed light on the
physical mechanisms governing burst dynamics, revealing intricate
interactions between electron beam characteristics and observed temporal
and spectral traits of type III solar radio bursts.</description>
</item>
<item>
<title> Observations and interpretation</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...689A.345K</link>
<description>Context. Shock waves in the solar corona are associated with solar
flares and coronal mass ejections (CMEs). Type II solar bursts are radio
signatures of shock waves in the solar corona. They are driven by solar
flares or CMEs. Despite extensive studies, the intricate spectral
patterns observed in type II solar bursts occasionally pose new
challenges for the theory of electron acceleration in shocks. Aims. We
study a newly identified feature in type II solar bursts called spectral
cleaving. This feature is characterized by the actual branching of a
type II radio emission lane in radio spectral data. Methods. We analyzed
the type II burst exhibiting spectral cleaving in high-fidelity dynamic
spectra obtained using the URAN-2 radio telescope (8.2533 MHz; Poltava
region, Ukraine) on 2011 February 14. The high-resolution spectrograms
were examined to ascertain its spectral morphology. Results. Our
research represents the first recognition of spectral cleaving as a
peculiarity of type II bursts that is yet to be classified. This effect
occurs due to the shift (or migration) of radio source(s) along a shock
front, which in turn is caused by changes in the magnetic field
orientation ahead of the propagating shock front. Conclusions. The
spectral cleaving observed in solar type II bursts reveals a distinct
phenomenon that indicates complex interactions between shock waves and
magnetic fields in the solar corona. This discovery enhances our
understanding of the mechanisms behind solar radio emissions and
emphasizes the need for further observational studies to verify these
findings.</description>
</item>
<item>
<title> Periods and Frequency Drifts of Groups of the Decimetric Spikes in Two Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299..113K</link>
<description>We studied the radio emission occurring as narrowband decimetric spikes
observed during the 10 May 2022 and 26 August 2022 flares. In the radio
spectra, these spikes were distributed in groups that occurred quasi-
periodically with the periods 5.1 s in the 10 May 2022 flare and 9.1 s
in the 26 August 2022 flare. In some parts of these groups, even
subgroups of spikes distributed with the quasi-periods of 0.19 s (10 May
2022 flare), and 0.17 s and 0.21 s (26 August 2022 flare) were found.
Some of these subgroups even drifted to higher or lower frequencies,
which was observed for the first time. At the time of the dm-spikes
observation, a pair of reconnecting loops are identified in the SDO/AIA
EUV observations of the 10 May 2022 flare, one of which is interpreted
as belonging to a small erupting filament. We propose that these loops
reconnect in the dynamic quasi-periodic regime (the period 0.19 s) and
this reconnection is modulated by an oscillation of one of the
interacting loops (the period 5.1 s). Accelerated electrons from this
process are trapped in reconnecting plasma outflows, and thus the
drifting groups of spikes are generated. The 26 August 2022 flare is a
complex event with several systems of bright loops; nevertheless, it
also shows a disintegrating erupting filament similar to the 10 May 2022
flare, meaning that the dm-spikes are likely generated by similar
reconnection processes.</description>
</item>
<item>
<title> The Multifaceted M1.7 GOES-class Flare Event of 21 April 2023 in AR13283</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299..109E</link>
<description>On 21 April 2023, a significant M1.7 solar flare erupted from Active
Region 13283, accompanied by a filament eruption and a full-halo Coronal
Mass Ejection, which reached Earth on 23 April, triggering a severe
geomagnetic storm, with Kp reaching 8 (G4) and Dst plummeting to 212 nT
together with a sharply distinguished long-lasting negative double-dip
behavior of the z-component of the interplanetary magnetic field. This
event led to remarkable auroral displays, even at mid-latitudes in
Europe. The flare-induced filament eruption caused distinct intensity
dimming in the solar corona, observed in specific EUV wavelengths. We
observed the dimming region growing at its fastest rate before the flare
reached its peak of intensity. Notably, the proximity of the flare to a
large southern coronal hole influenced the expansion and propagation of
the coronal mass ejection toward Earth, probably impacting the solar
wind speed and density. Additionally, we observed a sudden expansion of
the coronal hole during the flare, leading us to speculating that the
adjacent flare may have further stimulated the flow of solar-wind
particles along the open magnetic-field lines. In accordance with the
severe Dst-index disturbance, we also report changes in the potential of
the pipeline of an Italian energy infrastructure company with respect to
the surrounding soil as well as double-dip variation in the H-component
of the terrestial magnetic field observed locally (reminiscent to what
reported in Dst-index and IMF B&lt;SUB&gt;z&lt;/SUB&gt;) temporal profiles,
confirming the effects of the geomagnetic storm at Italy mid-latitudes.
Several solar radio events have been observed too. Therefore this study
provides insights into the dynamic solar phenomena and their potential
geomagnetic implications.</description>
</item>
<item>
<title> Verification of the Empirical Model of Ionization of the Lower Ionosphere during Solar Flares of Different Classes</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64..521R</link>
<description>The results of measuring VLF signal parameters propagating in the Earth-
D-region of the ionosphere waveguide to assess changes in the state of
the lower ionosphere as a result of the impact of X-ray radiation of
solar flares make it possible to obtain qualitative data on the nature
and magnitude of the impact. Obtaining accurate data on the relationship
between changes in electron concentration and flare parameters and
reliable prediction of the conditions of LF radio signal propagation
during strong geophysical disturbances is complicated by the lack of
complete information on the frequency spectrum of X-ray radiation for a
particular flare and data on the ionization rate of the ionosphere for
flares of different classes. The technique of determining the X-ray
spectrum in a wide range of wavelengths and calculating the ionization
coefficients of the lower ionosphere as a function of the ionizing
radiation parameters of flares, presented by Ryakhovsky et al. (2023),
makes it possible to improve the accuracy in estimating variations in
the parameters of the lower ionosphere. The present paper is devoted to
verifying the performance of the developed empirical model of lower
ionization of the lower ionosphere at the solar flare front and
comparing the results with experimental data on the variation of VLF
radio parameters.</description>
</item>
<item>
<title> lista completa de eventos observados en TNR</title>
<link>https://ui.adsabs.harvard.edu/abs/2024BAAA...65...21M</link>
<description>In the present work, a database of low frequency radio events is
described, analyzing all dynamic spectra from the instrument Thermal
Noise Receiver, belonging to the Radio and Plasma Wave Investigation
(WAVES) suite aboard the NASA Wind spacecraft. This database expands the
one built in a previous work, and encompasses the years 1994-2021,
covering more than two full solar cycles. The radio events are also
linked to the detection of other interplanetary structures such as shock
waves and interplanetary coronal mass ejections. We found a total of 320
events, out of which 136 had not been previously catalogued. Moreover,
121 shock waves that arrived to Earth's vicinity could be associated
with these radiofrequency events.</description>
</item>
<item>
<title> Efecto Neupert Anlisis para fulguraciones del Ciclo Solar 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2024BAAA...65....9C</link>
<description>The Neupert effect empirically states that, for many solar flares, the
soft X-ray (SXR) time derivative nearly fits the hard X-ray (HXR) or
microwave time profiles. This simple relationship supports flare models
in which the HXR emission is non-thermal bremsstrahlung by accelerated
electrons as they gradually lose their energy in the lower corona and
chromosphere, and the SXR emission is thermal bremsstrahlung from plasma
heated by the same electrons. We analize this effect for the most
energetic flares (classified as M or X) during the Solar Cycle 24, using
SXR observations and microwave data (MW), taking into account that the
energetic electrons responsible for HXR emission at chromospheric levels
are the same that, at low corona levels, produce MW radiation by
gyrosynchrotron emission. We observe for the first time that, at higher
MW frequencies, the Neupert effect works better.</description>
</item>
<item>
<title> Giant Postflare Loops in Active Regions with an Extremely Strong Coronal Magnetic Field</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...971..122A</link>
<description>We report for the first time the detection of thermal freefree emission
from post-flare loops at 34 GHz in images from the Nobeyama
Radioheliograph. We studied eight loops, seven of which were from
regions with an extremely strong coronal magnetic field reported by
Fedenev et al. Loop emission was observed in a wide range of wavelength
bands, up to soft X-rays, confirming their multitemperature structure
and was associated with noise storm emission in metric . The comparison
of the 17 GHz emission with that at 34 GHz, after a calibration
correction of the latter, showed that the emission was optically thin at
both frequencies. We describe the structure and evolution of the loops
and we computed their density, obtaining values for the top of the loops
between 1 and 6  10&lt;SUP&gt;10&lt;/SUP&gt; cm&lt;SUP&gt;3&lt;/SUP&gt;, noticeably varying
from one loop to another and in the course of the evolution of the same
loop system; these values have only a weak dependence on the assumed
temperature, 2  10&lt;SUP&gt;6&lt;/SUP&gt; K in our case, as we are in the
optically thin regime. Our density values are above those reported from
EUV observations, which go up to about 10&lt;SUP&gt;10&lt;/SUP&gt; cm&lt;SUP&gt;3&lt;/SUP&gt;.
This difference could be due to the fact that different emitting regions
are sampled in the two domains and/or due to the more accurate
diagnostics in the radio range, which do not suffer from inherent
uncertainties arising from abundances and non-LTE excitation/ionization
equilibria. We also estimated the magnetic field in the loop tops to be
in the range of 1030 G.</description>
</item>
<item>
<title> A Comprehensive Catalog and Statistical Results</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...971...86M</link>
<description>Decameter hectometric (DH; 114 MHz) type IV radio bursts are produced
by flare-accelerated electrons trapped in postflare loops or the moving
magnetic structures associated with the coronal mass ejections (CMEs).
From a space weather perspective, it is important to systematically
compile these bursts, explore their spectrotemporal characteristics, and
study the associated CMEs. We present a comprehensive catalog of DH type
IV bursts observed by the Radio and Plasma Wave Investigation
instruments on board the Wind and Solar TErrestrial RElations
Observatory spacecraft covering the period of white-light CME
observations by the Large Angle and Spectrometric Coronagraph on board
the Solar and Heliospheric Observatory mission between 1996 November and
2023 May. The catalog has 139 bursts, of which 73% are associated with a
fast (&gt;900 km s&lt;SUP&gt;1&lt;/SUP&gt;) and wide (&gt;60) CME, with a mean CME speed
of 1301 km s&lt;SUP&gt;1&lt;/SUP&gt;. All DH type IV bursts are white-light CME-
associated, with 78% of the events associated with halo CMEs. The CME
source latitudes are within 45. Seventy-seven events had multiple-
vantage-point observations from different spacecraft, letting us explore
the impact of the line of sight on the dynamic spectra. For 48 of the 77
events, there were good data from at least two spacecraft. We find that,
unless occulted by nearby plasma structures, a type IV burst is best
viewed when observed within a 60 line of sight. Also, bursts with a
duration above 120 minutes have source longitudes within 60. Our
inferences confirm the inherent directivity in the type IV emission.
Additionally, the catalog forms a Sun-as-a-star DH type IV burst
database.</description>
</item>
<item>
<title> Energetic Electrons Accelerated and Trapped in a Magnetic Bottle above a Solar Flare Arcade</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...971...85C</link>
<description>Where and how flares efficiently accelerate charged particles remains an
unresolved question. Recent studies revealed that a "magnetic bottle"
structure, which forms near the bottom of a large-scale reconnection
current sheet above the flare arcade, is an excellent candidate for
confining and accelerating charged particles. However, further
understanding its role requires linking the various observational
signatures to the underlying coupled plasma and particle processes. Here
we present the first study combining multiwavelength observations with
data-informed macroscopic magnetohydrodynamics and particle modeling in
a realistic eruptive flare geometry. The presence of an above-the-loop-
top magnetic bottle structure is strongly supported by the observations,
which feature not only a local minimum of magnetic field strength but
also abruptly slowing plasma downflows. It also coincides with a compact
above-the-loop-top hard X-ray source and an extended microwave source
that bestrides the flare arcade. Spatially resolved spectral analysis
suggests that nonthermal electrons are highly concentrated in this
region. Our model returns synthetic emission signatures that are well
matched to the observations. The results suggest that the energetic
electrons are strongly trapped in the magnetic bottle region due to
turbulence, with only a small fraction managing to escape. The electrons
are primarily accelerated by plasma compression and facilitated by a
fast-mode termination shock via the Fermi mechanism. Our results provide
concrete support for the magnetic bottle as the primary electron
acceleration site in eruptive solar flares. They also offer new insights
into understanding the previously reported small population of flare-
accelerated electrons entering interplanetary space.</description>
</item>
<item>
<title> Radio Signature of the Strong Compression between a Streamer and a Coronal Hole Boundary</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...970L..35A</link>
<description>We present evidence of the first detection of the radio signature at
metric wavelengths of the strong compression between a helmet streamer
(HS) and the boundary of a coronal hole (CH) using radio observations
from the Callisto MEXICO-LANCE and ALASKA-HAARP systems and white-light
observations obtained by the STEREO-A/COR1-COR2 coronagraphs. The event
occurred very close to the Sun (3.4 solar radii) and produced an
intense and unusually broad drifting radio feature at metric wavelengths
after a downward-drifting band of emission related to a metric Type II
radio burst. The compression is caused by the interaction between an
expanding structure (coronal mass ejection/shock) and the HS against the
CH boundary. Observations in white light show a sharp compressive
feature that propagates radially outward, while STEREO-A/EUVI images
show loop oscillations at the same position angle, indicating that the
interaction occurs across a range of heights. The loop oscillations
cease when the compressive front loses its sharp boundary. This
transition indicates a reduction of the density compression at the front
and the cessation of the radio emission.</description>
</item>
<item>
<title> A detection of the 22P3/222S1/2 fine-structure transition of hydrogen in the radio spectrum of the Sun?</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369...86L</link>
<description>The hyperfine transition of atomic hydrogen at a wavelength of about 21
cm is an essential tool for studies of interstellar gas. It has been
argued that also fine-structure transitions of hydrogen could be
detected in astronomical sources. Our aim is to detect the fine-
structure transition 22P3/222S1/2 of hydrogen at 10 GHz in the radio
spectrum of the Sun, with a spectral resolution which enables a detailed
study of the line profile. The Sun was observed with the 13.7 m radio
telescope at the Metshovi Radio Observatory, in Finland. We detect
emission from two of the three hyperfine components of the transition.
The width of the components is 15 MHz, much less than the expected
natural line width of 100 MHz (broadened solely by the uncertainty
principle). At red-shifted Doppler velocities, the lines show enhanced
emission and possibly self-absorption. If the absorption happens at the
chromosphere, our observations challenge the traditional view that
chromospheric temperature increases gradually towards higher altitudes.
Our unconventional results have to be confirmed by further observations.
This transition would be the only known spectral line in the Sun at
radio frequencies.</description>
</item>
<item>
<title> A comparative study of solar activity parameters during the period 20092012 and 20202023 (ascending phase of solar cycles 24 and 25)</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369...78S</link>
<description>In this paper, we performed solar synodic period (27 days) and
heliospheric effect for selected solar activity parameters: sunspot
number (SSN), sunspot area (SSA), modified coronal index (MCI), solar
radio flux (F10.7), chromospheric composite Mg II index and Galactic
cosmic rays (GCRs), during the ascending phase of solar cycles 24 and 25
(20092012 and 2020 to 2023). The Wavelet analyses of daily data of SSN,
SSA, MCI, Mg II, and F10.7, reveal a solar rotational period of 27
days. The R Robper method is used to validate the observed periods; near
one solar rotational period during the ascending phase of solar cycles
24 and 25. We observed cross-correlation and time lag for solar activity
parameters (SSN, SSA, MCI, Mg II, and F10.7) with GCRs during the
ascending phase of solar cycles 24 and 25 (20092012 and 2020 to 2023).
We found the highest time lag for SSA is 300 days, and for SSN is 270
days during the ascending phase of solar cycle 25. We also found the
highest cross-correlation values are 0.998 and 0.996 for chromospheric
composite Mg II index with Galactic cosmic rays (GCRs) during the
ascending phase of solar cycle 24 and 25 respectively. We found the
chromospheric composite Mg II index is a good indicator of solar
activity indices and it is strongly correlated to SSN.</description>
</item>
<item>
<title> Algorithms and Resources for the Monitoring of Very-Low-Frequency Signal Deviations Due to Solar Activity Using a Web-Based Software-Defined Radio-Distributed Network</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Senso..24.4596I</link>
<description>This work presents the development and testing of an experimental web-
based SDR (software-defined radio) monitoring system for indirect solar
activity detection, which has the ability to estimate and potentially
predict various events in space and on earth, including solar flares,
coronal mass ejections, and geomagnetic storms. The proposed system can
be used to investigate the effect of solar activity on the propagation
of very-low-frequency (VLF) signals. The advantages and benefits of the
given approach are as follows: increasing measurement accuracy and
eventual solar activity identification by combining measurements from
multiple spatially distributed SDRs. The verification process involves
carrying out several experiments comparing data from the GOES satellite
system and the Dunksin SuperSID system with information received by the
SDR monitoring system. Then, utilizing Pearson correlation coefficients,
the measured data from the SDRs, along with those from the GOES
satellite system and the Dunsing monitoring station, are investigated.
At the time of a solar flare, the correlation value is above 90% for
most of the stations used. Combining the signal-to-noise ratio via
summation also shows an improvement in the results, with a correlation
above 98%.</description>
</item>
<item>
<title> GUI for the e-CALLISTO data</title>
<link>https://ui.adsabs.harvard.edu/abs/2024NewA..10902194H</link>
<description>Solar radio bursts are sudden peaks in the low-frequency radio emissions
originating from the sun. These emissions, while revealing important
insights into underlying physical mechanisms in solar physics, can also
help predict space weather events that could have adverse effects on
satellite communications and the global energy grid. A thorough
understanding of this phenomena demands the collection and analysis of
solar emission data over vast geographical and time scales. In this
regard, the e-CALLISTO network plays a major role through having already
archived more than 20 years worth of solar radio burst data. Leveraging
on the advances in data analysis techniques, this data can be used to
review the statistical significance of burst properties of type II and
type III solar radio bursts and hence more importantly the magnetic
field measurements of the active regions. In order to process the
e-CALLISTO data, a software containing several data reduction processes
is introduced to optimize the data analysis via a graphical user
interface (GUI). The program is capable of reading out data from any
CALLISTO receiving station, while offering visualization capabilities
such as the color-corrected spectrum view, the plot of frequencies of
the highest intensity, the individual frequency spectrum, the solar
burst isolation portal, the fitting model for the radio burst, and the
drift rate curve of the burst. These are achieved through using the raw
"fits" files of spectra to perform background RFI reduction, identify
and isolate solar radio burst regions, model the peak frequency
variation using curve fitting, and thereby determine the frequency drift
rates. The method can be directly applied to Type II and III solar
bursts while providing space for tailoring and modification. In this
work, the slow drift type II radio bursts were fitted by exponential
decay and the fast drift type III radio bursts were approximated as
linear decay. Hence, the frequency drift rates were computed for type II
and type III radio bursts. The application is used to analyze several
Type II and Type III solar radio bursts and depending on the bust type
shock speed and electron velocity were determined. The GUI interface
eliminates the time-consuming subjective manual analysis of e-CALLISTO
data thereby making the analysis of solar radio bursts a routine and
rapid process.</description>
</item>
<item>
<title> Quasi-periodic oscillations in rotating and deformed space-times</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.531.3876B</link>
<description>Quasi-periodic oscillation (QPOs) analysis is important for
understanding the dynamical behaviour of many astrophysical objects
during transient events such as gamma-ray bursts, solar flares, magnetar
flares, and fast radio bursts. In this paper, we analyse QPO data in
low-mass X-ray binary (LMXB) systems, using the Lense-Thirring, Kerr,
and approximate Zipoy-Voorhees metrics. We demonstrate that the
inclusion of spin and quadrupole parameters modifies the well-
established results for the fundamental frequencies in the Schwarzschild
space-time. We interpret the QPO data within the framework of the
standard relativistic precession model, allowing us to infer the values
of the mass, spin, and quadrupole parameters of neutron stars in LMXBs.
We explore recent QPO data sets from eight distinct LMXBs, assess their
optimal parameters, and compare our findings with results in the
existing literature. Finally, we discuss the astrophysical implications
of our findings.</description>
</item>
<item>
<title> Development of a VLF receiver based on Red Pitaya for space weather studies</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JASTP.26006239A</link>
<description>A new VLF (Very low Frequency) receiver has been developed by the
Peruvian Space Agency (CONIDA) for space weather studies. The receiver
has been designed based on a Red Pitaya board which performs an SDR
(Software Defined Radio) to digitize, process and store the signal. The
receiver is composed of a vertical antenna, a preamplifier to filter and
amplify the incoming VLF signals from several transmitters located
around the world. The receiver is able to cover a bandwidth from 1 up to
50 kHz and it has been developed in such a way as to be cost-effective,
autonomous and solar-powered, making it suitable for installation in
multiple locations with different geographic conditions. We show the
performance of the receiver, the typical daily pattern of the lower
ionosphere for the NAA VLF signal, as observed in Peru, and the first
solar flares observed. The VLF amplitude curves recorded are validated
by comparing them with data from SAVNET (The South American VLF Network)
receiver installed in Peru. In a first effort to investigate the impact
of solar flares on the lower ionosphere, we conducted a statistical
analysis between VLF amplitude perturbations and 18  solar X-rays flux
provided by GOES satellites, resulting in a linear relationship.</description>
</item>
<item>
<title> Ionospheric TEC modeling using COSMIC-2 GNSS radio occultation and artificial neural networks over Egypt</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JAGeo..18..359S</link>
<description>The ionospheric delay significantly impacts GNSS positioning accuracy.
To address this, an Artificial Neural Network (ANN) was developed using
the high-quality COSMIC-2 ionospheric profile dataset to predict the
Total Electron Content (TEC). ANNs are adept at addressing both linear
and nonlinear challenges. For this research, eight distinct ANNs were
cultivated. These ANNs were designed with the following inputs Year,
Month, Day, Hour, Latitude, and Longitude. Along with solar and
geomagnetic parameters such as the F10.7 solar radio flux index, the
Sunspot Number (SSN), the Kp index, and the ap index. The goal was to
discern the most influential parameters on ionosphere prediction. After
pinpointing these key parameters, an enhanced model utilizing a
pioneering technique of a secondary ANN was employed with the main ANN
to predict TEC values for events in 2023. The study's findings indicate
that solar parameters markedly enhance the model's accuracy. Notably,
the augmented model featuring a prelude secondary network achieved a
stellar correlation coefficient of 0.99. Distributionally, 41 % of
predictions aligned within the (-1 TEC 1) TECU spectrum, 28 % nestled
within the (1&lt; TEC 2) and (-2 TEC &lt;-1) TECU ambit, while a
substantial 30 % spanned the broader (2&lt; TEC 5) and (-5 TEC &lt;-2)
TECU range. In essence, this research underscores the potential of
incorporating solar parameters and advanced neural network techniques to
refine ionospheric delay predictions, thus boosting GNSS positioning
precision.</description>
</item>
<item>
<title> Probing turbulence in solar flares from SDO/AIA emission lines</title>
<link>https://ui.adsabs.harvard.edu/abs/2024FrASS..1183746X</link>
<description>Multiple pieces of evidence have revealed the important role of
turbulence in physical processes in solar eruptions, from particle
acceleration to the suppression of conductive cooling. Radio
observations of density variation have established a Kolmogorov-like
spectrum for solar wind density disturbance. Close to the Sun,
measurements from extreme ultraviolet (EUV) bands have been used to
examine turbulence in the solar atmosphere. The Atmospheric Imaging
Assembly onboard the Solar Dynamics Observatory (SDO/AIA) has been
frequently used for diagnosing plasma properties due to its complex
coverage of temperature response. We compute structure functions (SFs)
using SDO/AIA emission measurements for two example of plasma sheets.
With the relationship of v  b  n and I(n0+n)2n (v, b, n, and
I are turbulent velocity, magnetic field, number density, and
intensity, respectively, and n0 is the background density), SFs of I
can be regarded as a proxy for those of the turbulent v and b fields in
the plasma sheet. We show that by properly accounting for the radial
dependence of the emission line intensity, an SF method is capable of
probing the presence of turbulence from SDO/AIA emission lines. Compared
to in situ observations, performing SFs on EUV emissions is advantageous
in studying turbulence behavior in the wave-vector space, and it opens a
new window for investigating turbulence from massive SDO/AIA
observations.</description>
</item>
<item>
<title> Progress of GECAM Observation Research</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ChJSS..44..668W</link>
<description>Gravitational wave high-energy Electromagnetic Counterpart All-sky
Monitor (GECAM) is a constellation with four instruments (launch date):
GECAM-A/B (10 December 2020), GECAM-C (27 July 2022) and GECAM-D (13
March 2024), which are dedicated to monitoring gamma-ray transients in
all-sky. The primary science objectives of GECAM include Gamma-Ray
Bursts (GRBs), Soft Gamma-ray Repeaters (SGRs), high energy counterparts
of Gravitation Wave (GW) and Fast Radio Burst (FRB), Solar Flares
(SFLs), as well as Terrestrial Gamma-ray Flashes (TGFs) and Terrestrial
Electron Beams (TEBs). A series of observations and research have been
made since the launch of GECAM-A/B. GECAM observations provide new
insights into these high-energy transients, demonstrating the unique
role of GECAM in the "multi-wavelength, multi-messenger" era.</description>
</item>
<item>
<title> Unveiling the Interplanetary Solar Radio Bursts of the 2024 Mother's Day Solar Storm</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...970L..13K</link>
<description>We report on a comprehensive study of interplanetary type III radio
bursts linked to X-class solar flares from NOAA active region 13664,
which instigated the intense 2024 Mother's Day solar storm, marked by a
geomagnetic storm of 412 nT, the strongest in over two decades.
Utilizing novel localization techniques with direction-finding data from
STEREO-A, we identify an average eastward drift of 13.42  11.63 in
radio source locations relative to GOES observations. Our analysis
reveals a significant correlation between solar flare intensity and
longitude (Kendall's tau = 0.535) and a strong correlation between radio
flux at 1 MHz and GOES 18  soft X-ray flux (Kendall's tau = 0.648).
The timing analysis shows that peak soft X-ray fluxes typically follow
electron beam liftoff by 3.24  4.42 minutes. These insights into solar
radio burst propagation and localization enhance our understanding of
solarterrestrial interactions and improve space weather forecasting
capabilities.</description>
</item>
<item>
<title> Localizing Quasiperiodic Pulsations in Hard X-Ray, Microwave, and Ly Emissions of an X6.4 Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...970...77L</link>
<description>We report the simultaneous observations of quasiperiodic pulsations
(QPPs) in wavelengths of hard X-ray (HXR), microwave, Ly, and
ultraviolet (UV) emissions during the impulsive phase of an X6.4 flare
on 2024 February 22 (SOL2024-02-22T22:08). The X6.4 flare shows three
repetitive and successive pulsations in HXR and microwave wavebands, and
they have an extremely large modulation depth. The onset of flare QPPs
is almost simultaneous with the start of magnetic cancellation between
positive and negative fields. The wavelet power spectra suggest the
presence of double periods, which are centered at 200 and 95 s,
respectively. The long-period QPP can also be detected in Ly and UV
wavebands at the flare area, and it could be observed in the adjacent
sunspot. Our observations indicate that the flare QPPs are most likely
triggered by accelerated electrons that are associated with periodic
magnetic reconnections. The long period at 200 s is probably modulated
by the slow magnetoacoustic wave originating from the neighboring
sunspot, while the short period at 95 s could be regarded as its second
harmonic mode.</description>
</item>
<item>
<title> Study of Particle Acceleration Using Fine Structures and Oscillations in Microwaves from the Electron Cyclotron Maser</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...970...17S</link>
<description>The accelerated electrons during solar flares produce radio bursts and
nonthermal X-ray signatures. The quasi-periodic pulsations (QPPs) and
fine structures in spatialspectraltemporal space in radio bursts
depend on the emission mechanism and the local conditions, such as
magnetic fields, electron density, and pitch-angle distribution. Radio
burst observations with high-frequency time resolution imaging provide
excellent diagnostics. In converging magnetic field geometries, the
radio bursts can be produced via the electron cyclotron maser (ECM).
Recently, using observations made by the Karl G. Jansky Very Large Array
(VLA) at 12 GHz, Yu et al. reported a discovery of long-lasting
auroral-like radio bursts persistent over a sunspot and interpreted them
as ECM-generated emission. Here we investigate the detailed second and
subsecond temporal variability of this continuous ECM source. We study
the association of 5 s period QPPs with a concurrent GOES C1.5-class
flare, utilizing VLA's imaging spectroscopy capability with an extremely
high temporal resolution (50 ms). We use the density and magnetic field
extrapolation model to constrain the ECM emission to the second harmonic
O-mode. Using the delay of QPPs from X-ray emission times, combined with
X-ray spectroscopy and magnetic extrapolation, we constrain the energies
and pitch angles of the ECM-emitting electrons to 48 keV and &gt;26. Our
analysis shows that the loss-cone diffusion continuously fuels the ECM
via Coulomb collisions and magnetic turbulence between a length scale of
5 and 100 Mm. We conclude that the QPP occurs via the LotkaVolterra
system, where the electrons from solar flares saturate the continuously
operating ECM and cause temporary oscillations.</description>
</item>
<item>
<title> Recurrent Nova V2487 Oph Had Superflares in 1941 and 1942 with Radiant Energies of 10&lt;SUP&gt;42.5+1.6&lt;/SUP&gt; erg</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...969...34S</link>
<description>V2487 Ophiuchi (V2487 Oph) is a recurrent nova with classical nova
eruptions in 1900 and 1998, and it is also the most extreme known
superflare star. These superflares are roughly hour-long flares with
amplitudes and optical energies reaching up to 1.10 mag and
10&lt;SUP&gt;39.21&lt;/SUP&gt; erg, respectively, with the superflares recurring
once a day. The V2487 Oph superflares are certainly operating with the
same mechanism as all the other types of superflare stars, where
magnetic loops are twisted and stretched until reconnection occurs,
whereupon ambient electrons are accelerated to relativistic energies and
then emit bremsstrahlung radiation from X-ray to radio. V2487 Oph is
unique among known superflare stars in that one of the loop footprints
is in an accretion disk. This exact mechanism was theoretically
predicted by M. R. Hayashi and colleagues in 1996. Now, I have found two
superflares recorded on Harvard archival photographs from 1941 and 1942.
These two superflares have B-magnitude amplitudes of &gt;1.83 and &gt;2.00 mag
and total radiated energies of 10&lt;SUP&gt;42.4&lt;/SUP&gt; and 10&lt;SUP&gt;42.5&lt;/SUP&gt;
erg, respectively, with bolometric corrections. Each has emitted
energies of 30 billion Carringtons, in units of the most energetic
solar flare. Further, I find superflares in Zwicky Transient Factory
light curves, so V2487 Oph has been superflaring from 1941 to 2023. For
the observed number distribution of dN/dE = 4E &lt;SUP&gt;2&lt;/SUP&gt; superflares
per year, for E in units of 10&lt;SUP&gt;41&lt;/SUP&gt; erg, the emitted energy in
superflare light is 10&lt;SUP&gt;42.1&lt;/SUP&gt; erg in each year, or
10&lt;SUP&gt;44.1&lt;/SUP&gt; erg from 1941 to 2023.</description>
</item>
<item>
<title> Electron Cyclotron Maser Emission and the Brightest Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...969....3W</link>
<description>This paper investigates the incidence of coherent emission in solar
radio bursts, using a revised catalog of 3800 solar radio bursts
observed by the Nobeyama Radio Polarimeters from 1988 to 2023. We focus
on the 1.0 and 2.0 GHz data, where radio fluxes of order 10&lt;SUP&gt;10&lt;/SUP&gt;
Jy have been observed. Previous work has suggested that these bursts are
due to electron cyclotron maser (ECM) emission. In at least one well-
studied case, the bright emission at 1 GHz consists of narrowband spikes
of millisecond duration. Coherent emission at 1 GHz can be distinguished
from traditional incoherent gyrosynchrotron flare emission based on the
radio spectrum: Gyrosynchrotron emission at 1 GHz usually has a spectrum
rising with frequency, so bursts in which 1 GHz is stronger than higher-
frequency measurements are unlikely to be incoherent gyrosynchrotron.
Based on this criterion, it is found that for bursts exceeding 100 sfu,
three-quarters of all bursts at 1 GHz and half of all 2 GHz bursts have
a dominant coherent emission component, assumed to be ECM. The majority
of the very bright bursts at 1 GHz are highly circularly polarized,
consistent with a coherent emission mechanism, but not always 100%
polarized. The frequency range from 1 to 2 GHz is heavily utilized for
terrestrial applications, and these results are relevant for
understanding the extreme flux levels that may impact such applications.
Further, they provide a reference for comparison with the study of ECM
emission from other stars and potentially exoplanets.</description>
</item>
<item>
<title> type II radio emission on 27th of September 2001</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369...70A</link>
<description>This study focus on atypical Type II radio bursts observed in
conjunction with three simultaneous coronal mass ejections (CMEs) on
September 27, 2001. These CMEs originated from a single active region
(AR) and were linked to relatively weak solar flares. Analysis of the
CME sequences revealed distinct periods of interplanetary (IP) Type II
radio emissions, characterized by pronounced increases in intensity. The
first radio enhancement, lasting 20 minutes, exhibited very low density
and frequency (1.651.5 MHz) at a height range of (7.88.2) solar radii
(). Subsequently, the second radio signature persisted for 40 minutes
with a frequency range of (900700) kHz and a height range of
(10.912.6) . The third radio signature spanned 1 hour and 20 minutes,
featuring a frequency range of (660390) kHz and a height range of
(13.218.6) . The fourth enhancement extended over 3 hours, ranging from
(550250) kHz in frequency and (14.625.0)  in height. We concluded that
the initial low-density radio signature resulted from a shock wave
generated by reconnection of magnetic field lines, without an intense
flare or extreme ultraviolet imaging telescope (EIT) wave. This shock
wave then accelerated subsequent CMEs. Alternatively, the radio burst
could have formed in the wake of the initial slow CME, creating a low-
density environment. The second radio enhancement coincided with the
accelerated propagation of CME1's core and was attributed to enhanced
radio emission resulting from the Type II shock encountering filament
material. The third radio enhancement aligned with the concept of a CME
bow shock, indicating that the shock was positioned at the leading front
of the CME. This enhancement occurred when the shock met remnant
material from earlier CMEs, yet the shock continued propagating at a
constant speed. The fourth enhancement progressed to higher frequencies
due to the merging of CME1's core with CME2, propagating along CME3's
path. This comprehensive analysis provides valuable insights into the
complex dynamics and interactions associated with these unique Type II
radio bursts and their correlation with coronal mass ejections.</description>
</item>
<item>
<title> Low-Frequency Solar Radio Type II Bursts And Their Association With Space Weather Events During The Ascending Phase Of Solar Cycle 25</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AnGeo..42..313N</link>
<description>Type II solar radio bursts are signatures of the coronal shocks and,
therefore, particle acceleration events in the solar atmosphere and
interplanetary space. Type II bursts can serve as a proxy to provide
early warnings of incoming solar storm disturbances, such as geomagnetic
storms and radiation storms, which may further lead to ionospheric
effects. In this article, we report the first observation of 32 type II
bursts by measuring various plasma parameters that occurred between May
2021 and December 2022 in solar cycle 25. We further evaluated their
accompanying space weather events in terms of ionospheric total electron
content (TEC) enhancement using the rate of TEC index (ROTI). In this
study, we find that at heliocentric distance 12 R, the shock and the
Alfvn speeds are in the range 5041282 and 368826 km1, respectively.
The Alfvn Mach number is of the order of 1.2MA1.8 at the above-
mentioned heliocentric distance. In addition, the measured magnetic
field strength is consistent with the earlier reports and follows a
single power law B(r)=6.07r-3.96G. Based on the current analysis, it is
found that 19 out of 32 type II bursts are associated with immediate
space weather events in terms of radio blackouts and polar cap
absorption events, making them strong indications of space weather
disruption. The ROTI enhancements, which indicate ionospheric
irregularities, strongly correlate with GOES X-ray flares, which are
associated with the type II radio bursts recorded. The diurnal
variability in ROTI is proportional to the strength of the associated
flare class, and the corresponding longitudinal variation is attributed
to the difference in longitude. This article demonstrates that since
type II bursts are connected to space weather hazards, understanding
various physical parameters of type II bursts helps to predict and
forecast the space weather.</description>
</item>
<item>
<title> First determination of the angular dependence of rise and decay times of solar radio bursts using multi-spacecraft observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...687L..12C</link>
<description>A large arsenal of space-based and ground-based instruments is dedicated
to the observation of radio emissions, whether they originate within our
solar system or not. Radio photons interact with anisotropic density
fluctuations in the heliosphere which can alter their trajectory and
influence the properties that are deduced from observations. This is
particularly evident in solar radio observations, where anisotropic
scattering leads to highly directional radio emissions. Consequently,
observers at varying locations will measure different properties,
including different source sizes, source positions, and intensities.
However, it is not known whether the measurements of the decay time of
solar radio bursts are also affected by the observer's position. Decay
times are dominated by scattering effects, and so are frequently used as
proxies of the level of density fluctuations in the heliosphere, making
the identification of any location-related dependence crucial. We
combine multi-vantage observations of interplanetary Type III bursts
from four non-collinear, angularly separated spacecraft with simulations
to investigate the dependence of the decay- and rise-time measurements
on the separation of the observer from the source. We propose a function
to characterise the entire time profile of radio signals, allowing for
the simultaneous estimation of the peak flux, decay time, and rise time,
while demonstrating that the rise phase of radio bursts is non-
exponential, having a non-constant growth rate. We determine that the
decay and rise times are independent of the observer's position,
identifying them as the only properties that remain unaffected and thus
do not require corrections for the observer's location. Moreover, we
examine the ratio between the rise and decay times and find that it does
not depend on the frequency. Therefore, we provide the first evidence
that the rise phase is also significantly impacted by scattering
effects, adding to our understanding of the plasma emission process.</description>
</item>
<item>
<title> The solar cycle 25 multi-spacecraft solar energetic particle event catalog of the SERPENTINE project</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...687A..72D</link>
<description>Context. The solar energetic particle analysis platform for the inner
heliosphere (SERPENTINE) project, funded through the H2020-SPACE-2020
call of the European Union's Horizon 2020 framework program, employs
measurements of the new inner heliospheric spacecraft fleet to address
several outstanding questions on the origin of solar energetic particle
(SEP) events. The data products of SERPENTINE include event catalogs,
which are provided to the scientific community. &lt;BR /&gt; Aims: In this
paper, we present SERPENTINE's new multi-spacecraft SEP event catalog
for events observed in solar cycle 25. Observations from five different
viewpoints are utilized, provided by Solar Orbiter, Parker Solar Probe,
STEREO A, BepiColombo, and the near-Earth spacecraft Wind and SOHO. The
catalog contains key SEP parameters for 25-40 MeV protons, ~1 MeV
electrons, and ~100 keV electrons. Furthermore, basic parameters of
associated flares and type II radio bursts are listed, as are the
coordinates of the observer and solar source locations. &lt;BR /&gt; Methods:
An event is included in the catalog if at least two spacecraft detect a
significant proton event with energies of 25-40 MeV. The SEP onset times
were determined using the Poisson-CUSUM method. The SEP peak times and
intensities refer to the global intensity maximum. If different viewing
directions are available, we used the one with the earliest onset for
the onset determination and the one with the highest peak intensity for
the peak identification. We furthermore aimed to use a high time
resolution to provide the most accurate event times. Therefore, we opted
to use a 1-min time resolution, and more time averaging of the SEP
intensity data was only applied if necessary to determine clean event
onsets and peaks. Associated flares were identified using observations
from near Earth and Solar Orbiter. Associated type II radio bursts were
determined from ground-based observations in the metric frequency range
and from spacecraft observations in the decametric range. &lt;BR /&gt;
Results: The current version of the catalog contains 45 multi-spacecraft
events observed in the period from November 2020 until May 2023, of
which 13 events were found to be widespread (observed at longitudes
separated by at least 80 from the associated flare location) and four
could be classified as narrow-spread events (not observed at longitudes
separated by at least 80 from the associated flare location). Using
X-ray observations by GOES/XRS and Solar Orbiter/STIX, we were able to
identify the associated flare in all but four events. Using ground-based
and space-borne radio observations, we found an associated type II radio
burst for 40 events. In total, the catalog contains 142 single event
observations, of which 20 (45) have been observed at radial distances
below 0.6 AU (0.8 AU). It is anticipated that the catalog will be
extended in the future. &lt;P /&gt;Available at &lt;A href="https://doi.org/10.52
81/zenodo.10732268"&gt;https://doi.org/10.5281/zenodo.10732268&lt;/A&gt;</description>
</item>
<item>
<title> A Catalog of Metric Type II Radio Bursts Detected by RSTN During Solar Cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...75L</link>
<description>In this study, we compile a catalog of metric type II radio bursts using
the Radio Solar Telescope Network (RSTN) to study the occurrence,
associations, and properties of the emission and their parent solar
activity phenomena. According to the intensity and clarity of the radio
emission features, we have divided the m-type II radio bursts into two
qualitative categories, namely certain and uncertain. We analyzed RSTN
data in Solar Cycle 24 (2009  2019), which is freely available from
four worldwide stations: Learmonth, Sanvito, Sagamore Hills, and
Palehua. Through careful visual inspection, we have collected all metric
type II bursts detected in the range of 25  180 MHz. The relationships
between these bursts and solar eruptive events, such as solar flares and
coronal mass ejections (CMEs), are studied, and the results are
presented and discussed. The outcomes could be used to reveal the
occurrence of solar and space-weather activities based on the ground-
based radio perspective. The newly assembled catalog of metric type II
and associated solar events will be made freely available to the solar
scientific community.</description>
</item>
<item>
<title> Radio emission from SN 1181 hosting a white dwarf merger product</title>
<link>https://ui.adsabs.harvard.edu/abs/2024PASJ...76..475K</link>
<description>The remnant of the historical supernova 1181 is claimed to be associated
with a white dwarf merger remnant J005311. The supernova remnant (SNR)
shock, and a termination shock expected to be formed by the intense wind
of J005311, are potential sites for radio emission via synchrotron
emission from shock-accelerated electrons. In this paper, we estimate
the radio emission from these two shocks, and find the peak radio flux
to be 0.1-10 mJy (at 0.01-1 GHz) in the outer SNR shock and 0.01-0.1 mJy
(at 1-10 GHz) in the inner termination shock. We also search for radio
emission from this source in the archival data of the Karl G. Jansky
Very Large Array (VLA) Sky Survey at 3 GHz, the NRAO VLA Sky Survey at
1.4 GHz and the Canadian Galactic Plane Survey at 408 MHz, finding no
significant detection. While targeted observations with higher
sensitivity are desired, we particularly encourage those at higher
frequency and angular resolution to probe the inner termination shock
and its evolution.</description>
</item>
<item>
<title> Semantic Segmentation of Solar Radio Spikes at Low Frequencies</title>
<link>https://ui.adsabs.harvard.edu/abs/2024OJAp....7E..51M</link>
<description>Solar radio spikes are short lived, narrow bandwidth features in low
frequency solar radio observations. The timing of their occurrence and
the number of spikes in a given observation is often unpredictable. The
high temporal and frequency of resolution of modern radio telescopes
such as NenuFAR mean that manually identifying radio spikes is an
arduous task. Machine learning approaches to data exploration in solar
radio data is on the rise. Here we describe a convolutional neural
network to identify the per pixel location of radio spikes as well as
determine some simple characteristics of duration, spectral width and
drift rate. The model, which we call SpikeNet, was trained using an
Nvidia Tesla T4 16GB GPU with ~100000 sample spikes in a total time of
2.2 hours. The segmentation performs well with an intersection over
union in the test set of ~0.85. The root mean squared error for
predicted spike properties is of the order of 23%. Applying the
algorithm to unlabelled data successfully generates segmentation masks
although the accuracy of the predicted properties is less reliable,
particularly when more than one spike is present in the same 64 X 64
pixel time-frequency range. We have successfully demonstrated that our
convolutional neural network can locate and characterise solar radio
spikes in a number of seconds compared to the weeks it would take for
manual identification.</description>
</item>
<item>
<title> Scaling and universality in the temporal occurrence of repeating FRBs</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.531L..57D</link>
<description>Fast Radio Bursts (FRBs) are energetic phenomena that have significant
implications for understanding fundamental physics and the Universe.
Recent observations of FRB 121102, FRB 20220912A, and FRB 20201124A by
the Five-hundred-meter Aperture Spherical Telescope showed high-burst
rates and distinctive energy distribution and temporal properties. In
this study, we examine these observations to investigate the scale
invariance of the waiting times between bursts for intervals longer than
approximately 1 s. Our analysis revealed a unified scaling law for these
longer intervals, which is similar to the behaviour of solar flares.
This discovery inspires us to suggest a dual analogy of the FRB scenario
across the entire time intervals: with earthquake dynamics at subsecond
scales and with solar flare dynamics beyond the one-second threshold.
This threshold potentially aligns with the dynamic time-scale of neutron
star crusts, offering insight of the occurrence of FRBs into the
internal processes of neutron stars.</description>
</item>
<item>
<title> on alert for high energy transients</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ExA....57...24B</link>
<description>We present Daksha, a proposed high energy transients mission for the
study of electromagnetic counterparts of gravitational wave sources, and
gamma ray bursts. Daksha will comprise of two satellites in low earth
equatorial orbits, on opposite sides of the Earth. Each satellite will
carry three types of detectors to cover the entire sky in an energy
range from 1 keV to &gt;1 MeV. Any transients detected on-board will be
announced publicly within minutes of discovery. All photon data will be
downloaded in ground station passes to obtain source positions, spectra,
and light curves. In addition, Daksha will address a wide range of
science cases including monitoring X-ray pulsars, studies of magnetars,
solar flares, searches for fast radio burst counterparts, routine
monitoring of bright persistent high energy sources, terrestrial gamma-
ray flashes, and probing primordial black hole abundances through
lensing. In this paper, we discuss the technical capabilities of Daksha,
while the detailed science case is discussed in a separate paper.</description>
</item>
<item>
<title> Features of the Spectra of Microwave Sources above Sunspots Inferred from Observations with RATAN-600</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AstBu..79..304O</link>
<description>The flux density spectra of cyclotron sources above the sunspots were
obtained by observations with RATAN-600 in the range of 1.710 cm with
high spectral () resolution and their spectral indices were estimated.
The spectral index was then utilized to determine the magnitude of the
magnetic field at the base of the transition region on the Sun. By
analyzing the relationship between the emisson flux density of the
sources and the magnetic field it was found that the observed
characteristics of sunspot-associated sources did not align with
predictions from a simplified radiation model commonly used for data
interpretation. Specifically, there was an excess flux density in the
spectrum of ordinary mode radiation compared to what was expected.</description>
</item>
<item>
<title> Plasma Motions and Compressive Wave Energetics in the Solar Corona and Solar Wind from Radio Wave Scattering Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...968...72A</link>
<description>Radio signals propagating via the solar corona and solar wind are
significantly affected by compressive waves, impacting the properties of
solar bursts as well as sources viewed through the turbulent solar
atmosphere. While static fluctuations scatter radio waves elastically,
moving, turbulent, or oscillating density irregularities act to broaden
the frequency of the scattered waves. Using a new anisotropic density
fluctuation model from the kinetic scattering theory for solar radio
bursts, we deduce the plasma velocities required to explain observations
of spacecraft signal frequency broadening. The inferred velocities are
consistent with motions that are dominated by the solar wind at
distances 10 R &lt;SUB&gt;&lt;/SUB&gt;, but the levels of frequency broadening for
10 R &lt;SUB&gt;&lt;/SUB&gt; require additional radial speeds (100300) km
s&lt;SUP&gt;1&lt;/SUP&gt; and/or transverse speeds (2070) km s&lt;SUP&gt;1&lt;/SUP&gt;. The
inferred radial velocities also appear consistent with the sound or
proton thermal speeds, while the speeds perpendicular to the radial
direction are consistent with nonthermal motions measured via coronal
Doppler-line broadening, interpreted as Alfvnic fluctuations. Landau
damping of parallel propagating ion-sound (slow MHD) waves allows an
estimate of the proton heating rate. The energy deposition rates due to
ion-sound wave damping peak at a heliocentric distance of (13) R
&lt;SUB&gt;&lt;/SUB&gt; are comparable to the rates available from a turbulent
cascade of Alfvnic waves at large scales, suggesting a coherent picture
of energy transfer, via the cascade or/and parametric decay of Alfvn
waves to the small scales where heating takes place.</description>
</item>
<item>
<title> A Possible Indication of the Insufficiency of Homogeneous Models</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...968...55K</link>
<description>The geo-effectiveness of coronal mass ejections (CMEs) is determined
primarily by their magnetic fields. Modeling of gyrosynchrotron (GS)
emission is a promising remote sensing technique to measure the CME
magnetic field at coronal heights. However, faint GS emission from CME
flux ropes is hard to detect in the presence of bright solar emission
from the solar corona. With high dynamic-range spectropolarimetric meter
wavelength solar images provided by the Murchison Widefield Array, we
have detected faint GS emission from a CME out to 8.3 R &lt;SUB&gt;&lt;/SUB&gt;,
the largest heliocentric distance reported to date. High-fidelity
polarimetric calibration also allowed us to robustly detect circularly
polarized emission from GS emission. For the first time in the
literature, Stokes V detection has jointly been used with Stokes I
spectra to constrain GS models. One expects that the inclusion of
polarimetric measurement will provide tighter constraints on the GS
model parameters. Instead, we found that homogeneous GS models, which
have been used in all prior works, are unable to model both the total
intensity and circular polarized emission simultaneously. This strongly
suggests the need for using inhomogeneous GS models to robustly estimate
the CME magnetic field and plasma parameters.</description>
</item>
<item>
<title> A Multipeak Solar Flare with a High Turnover Frequency of the Gyrosynchrotron Spectra from the Loop-top Source</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...968....5W</link>
<description>The origin of multiple peaks in light curves of various wavelengths
remains illusive during flares. Here we discuss the flare of
SOL2023-05-09T03:54M6.5 with six flux peaks as recorded by a tandem of
new microwave and hard X-ray (HXR) instruments. According to its
microwave spectra, the flare represents a high-turnover-frequency (&gt;15
GHz) event. The rather-complete microwave and HXR spectral coverage
provides a rare opportunity to uncover the origin of such an event
together with simultaneous EUV images. We concluded that (1) the
microwave sources originates around the top section of the flaring loops
with a trend of source spatial dispersion with frequency; (2) the
visible movement of the microwave source from peak to peak originates
from the process of new flaring loops appearing sequentially along the
magnetic neutral line; (3) the optically thin microwave spectra are hard
with the indices ( &lt;SUB&gt;tn&lt;/SUB&gt;) varying from 1.2 to 0.4, and the
turnover frequency always exceeds 15 GHz; (4) higher turnover/peak
frequency corresponds to stronger peak intensity and harder optically
thin spectra. Using the FokkerPlanck and GX Simulator codes we obtained
a good fit to the observed microwave spectra and spatial distribution of
the sources at all peaks, if assuming the radiating energetic electrons
have the same spatial distribution and single-power-law spectra but with
the number density varying in a range of 30%. We conclude that the
particle acceleration in this flare happens in a compact region nearing
the loop-top. These results provide new constraints on the acceleration
of energetic electrons and the underlying flare intermittent
reconnection process.</description>
</item>
<item>
<title> Mechanisms of Fundamental Electromagnetic Wave Radiation in the Solar Wind</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...967L..20K</link>
<description>Large-scale and long-term two-dimensional particle-in-cell simulations
performed for parameters relevant to type III solar radio bursts have
provided new results on the generation mechanisms of fundamental
electromagnetic waves radiated at the plasma frequency  &lt;SUB&gt; p &lt;/SUB&gt;.
The paper first considers the nonlinear wave interaction process of
electromagnetic decay (EMD) in a homogeneous solar wind plasma with an
electron-to-ion temperature ratio T &lt;SUB&gt; e &lt;/SUB&gt;/T &lt;SUB&gt; i &lt;/SUB&gt; &gt; 1.
The dynamics of ion-acoustic waves (dispersion, spectra, growth/damping)
is studied, and signatures confirming the three-wave interactions
(cross-bicoherence, correlations between waves' phases and between
waves' growths, resonance conditions) are provided. The decisive role
played in EMD by the backscattered Langmuir waves coming from the
electrostatic decay (ESD) is demonstrated. EMD can be triggered by ion
acoustic waves coming from the two cascades of the faster and more
intense ESD. The same study is then performed in a solar wind plasma
with random density fluctuations. In this case, EMD is not suppressed
but develops only within plasma regions of reduced or quasi-uniform
density. It coexists with linear mode conversion (LMC) of Langmuir waves
into electromagnetic radiation, which is the fastest and most prominent
process, as well as with ESD. LMC can lead to enhanced occurrence of EMD
in the early stage. Moreover, the impact of T &lt;SUB&gt; e &lt;/SUB&gt;/T &lt;SUB&gt; i
&lt;/SUB&gt; on electromagnetic energy growth and saturation is shown to be
rather weak. Ion-acoustic waves are heavily damped at T &lt;SUB&gt; e &lt;/SUB&gt; 
T &lt;SUB&gt; i &lt;/SUB&gt;, so that EMD is overcome by nonlinear induced
scattering on thermal ions. In actual solar wind plasmas, EMD should be
more easily observed in plasma regions weakly perturbed by the
background density turbulence and where ion temperature is decreased.</description>
</item>
<item>
<title> Deep learning-based prediction of CME-driven shock standoff distances in metric type II radio emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369...57K</link>
<description>Type II radio emissions are events mostly found to be associated with
coronal mass ejections (CMEs) and accelerated by the CME-driven shock in
the heliosphere. This study reports on the estimation of the CME-shock
standoff distance at the commencement of metric type II radio emissions
by combining the CME-deprojected speed and spectral features of radio
bursts using a robust TensorFlow Deep-Learning Sequential (TFDLS)
technique. The dataset of 96 CMEs at the commencement of type II radio
bursts was used between Solar cycle 24 and the ascending phase of Solar
Cycle 25. The measured root mean squared error (RMSE) was 0.145 (Rs),
with an average height difference of 0.096 Rs between the observed and
predicted CME-shock heights. Five (5) CMEs/radio bursts energetic events
associated with solar flares were selected from the test data, and the
CME shock stand-off heights were forecasted using the TFDLS and flare-
onset (FL) methods. The data were used to compare the leading-edge (LE)
and dynamic spectra (DS) methods. The RMSE measured between the FL and
LE was 0.35 Rs, and the RMSE estimated between the TFDLS and LE
approaches was 0.04 Rs. The RMSE between FL and DS was 0.34. Rs, and the
RMSE between the TFDLS and the DS was 0.04 Rs. We also used the findings
gained from the five selected events and compared them to the 3D shock-
fitting (3D-SF) approach. The RMSE found between the TFDLS and the 3D-SF
was 0.18 Rs, while the RMSE estimated between the FL and the 3D-SF was
0.23 Rs. This shows that the TFDLS has satisfactory performance and can
be used as an alternative technique.</description>
</item>
<item>
<title> An Assessment of Solar Cycle 25 progress through observation of SRBs and associated Geomagnetic Storms</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..73.6274N</link>
<description>Geomagnetic storms are severe aspects of Space Weather. They originate
due to solar transient emissions such as coronal mass ejections (CMEs),
whose energetic materials propagate in the Interplanetary medium and are
coupled with the magnetosphere system. CME driven Geomagnetic storms are
often associated with solar radio bursts (SRBs), particularly type II
and type IV bursts. In this study, we present the preliminary results of
solar radio observations and their associated geomagnetic activity
during solar cycle 25 (SC 25) from January 2020 to June 2023, focusing
on the cycle's first four intense geomagnetic storms. The study used
various radio telescopes, mainly the compound astronomical low-frequency
low-cost instrument for spectroscopy and transportable observatory
(CALLISTO), as well as OMNI data and the World Data Center for
Geomagnetism. During the study period, it was found that 23 solar radio
bursts diagnosed the geomagnetic storms with Dst &lt;-50nT from 35
reported, including three severe storms of the SC 25. The time delay
between the solar radio bursts and the arrival of CMEs and/or HSS near
the Earth's magnetosphere is estimated with an average value of 79 h
within the [48120 h] range for 23 geomagnetic storms associated with
solar radio bursts. Among 35 geomagnetic storms recorded, five are
recurring geomagnetic storms associated with coronal high-speed streams
(HSS), while CMEs cause the rest with average speeds of 750 km/s. The
current SC 25 recognizes four major storms within the scope of the
study. On 21 April 2023, a type II radio burst followed by a type IV
burst diagnosed the first severe geomagnetic storm on 24 April 2023. The
second severe storm was unusual and detected in the absence of the
precursor as a solar radio burst. The SRBs of type II burst and type IV
burst extending in IP medium on 1 November 2021 tracked the third major
storm of the cycle while the group of type III radio bursts, type II and
type IV bursts on 24 February 2023, predicted the major storm on 27
February 2023. These major geomagnetic storms are linked to CMEs that
show expanding flux ropes, which are signatures of type II and moving
type IV radio bursts identified. Furthermore, the detected SRBs and
related major geomagnetic storms are proof of high solar and magnetic
activity of the ascending phase of SC 25. The SC 25 has been
characterized overall, and its current progress is being tracked using
observations of SRBs and magnetic activity during its rising phase.</description>
</item>
<item>
<title> Generation of relativistic electrons at the termination shock in the solar flare region</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...686A.207M</link>
<description>Context. Solar flares are accompanied by an enhanced emission of
electromagnetic waves from the radio up to the -ray range. The
associated hard X-ray and microwave radiation is generated by energetic
electrons. These electrons play an important role, since they carry a
substantial part of the energy released during a flare. The flare is
generally understood as a manifestation of magnetic reconnection in the
corona. The so-called standard CSHKP model is one of the most widely
accepted models for eruptive flares. The solar flare event on September
10, 2017 offers us a unique opportunity to study this model. The
observations from the Expanded Owens Valley Solar Array (EOVSA) show
that 1.6  10&lt;SUP&gt;4&lt;/SUP&gt; electrons with energies &gt; 300 keV are
generated in the flare region. &lt;BR /&gt; Aims: There are signatures in
solar radio and extreme ultraviolet (EUV) observations as well as
numerical simulations that a "termination shock" (TS) appears in the
magnetic reconnection outflow region. Electrons accelerated at the TS
can be considered to generate the loop-top hard X-ray sources. In
contrast to previous studies, we investigate whether the heating of the
plasma at the TS provides enough relativistic electrons needed for the
hard X-ray and microwave emission observed during the solar X8.2 flare
on September 10, 2017. &lt;BR /&gt; Methods: We studied the heating of the
plasma at the TS by evaluating the jump in the temperature across the
shock by means of the Rankine-Hugoniot relationships under coronal
circumstances measured during the event on September 10, 2017. The part
of relativistic electrons was calculated in the heated downstream
region. &lt;BR /&gt; Results: In the magnetic reconnection outflow region, the
plasma is strongly heated at the TS. Thus, there are enough energetic
electrons in the tail of the electron distribution function (EDF) needed
for the microwave and hard X-ray emission observed during the event on
September 10, 2017. &lt;BR /&gt; Conclusions: The generation of relativistic
electrons at the TS is a possible mechanism of explaining the enhanced
microwave and hard X-ray radiation emitted during flares.</description>
</item>
<item>
<title> Estimating the lateral speed of a fast shock driven by a coronal mass ejection at the location of solar radio emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...686A.159N</link>
<description>Context. Fast coronal mass ejections (CMEs) can drive shock waves
capable of accelerating electrons to high energies. These shock-
accelerated electrons act as sources of electromagnetic radiation, often
in the form of solar radio bursts. Recent findings suggest that radio
imaging of solar radio bursts can provide a means to estimate the
lateral expansion of CMEs and associated shocks in the low corona. &lt;BR
/&gt; Aims: Our aim is to estimate the expansion speed of a CME-driven
shock at the locations of radio emission using 3D reconstructions of the
shock wave from multiple viewpoints. &lt;BR /&gt; Methods: In this study, we
estimated the 3D location of radio emission using radio imaging from the
Nanay Radioheliograph and the 3D location of a CME-driven shock. The 3D
shock was reconstructed using white-light and extreme ultraviolet images
of the CME from the Solar Terrestrial Relations Observatory, Solar
Dynamics Observatory, and the Solar and Heliospheric Observatory. The
lateral expansion speed of the CME-driven shock at the electron
acceleration locations was then estimated using the approximate 3D
locations of the radio emission on the surface of the shock. &lt;BR /&gt;
Results: The radio bursts associated with the CME were found to reside
at the flank of the expanding CME-driven shock. We identified two
prominent radio sources at two different locations and found that the
lateral speed of the shock was between 800 and 1000 km s&lt;SUP&gt;1&lt;/SUP&gt; at
these locations. Such a high speed during the early stages of the
eruption already indicates the presence of a fast shock in the low
corona. We also found a larger ratio between the radial and lateral
expansion speed compared to values obtained higher up in the corona. &lt;BR
/&gt; Conclusions: We estimated for the first time the 3D expansion speed
of a CME-driven shock at the location of the accompanying radio
emission. The high shock speed obtained is indicative of a fast
acceleration during the initial stage of the eruption. This acceleration
leading to lateral speeds in the range of 8001000 km s&lt;SUP&gt;1&lt;/SUP&gt; is
most likely one of the key parameters contributing to the presence of
metric radio emissions, such as type II radio bursts.</description>
</item>
<item>
<title> Properties of Type-II Radio Bursts in Relation to Magnetic Complexity of the Solar Active Regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...74B</link>
<description>Type-II radio bursts are believed to occur as a result of the shock
driven by flares or coronal mass ejections (CMEs). While the shock waves
are important for the acceleration of electrons necessary for the
generation of the radio emission, the exact nature of the shock and
coronal conditions necessary to produce type-II radio emission is still
under debate. In this investigation, we probe the relationship of
kinematic characteristics of the type-II radio bursts with the magnetic-
field complexity (M&lt;SUB&gt;j&lt;/SUB&gt;) of the active regions visible on the
photosphere. Our investigation of 64 type-II solar radio bursts, which
are associated with flares and CMEs, reveals that M&lt;SUB&gt;j&lt;/SUB&gt; is
linearly correlated in the logarithmic scale with the starting frequency
(f&lt;SUB&gt;s&lt;/SUB&gt;) and drift-rate (f/t) of type-II radio burst. Further,
M&lt;SUB&gt;j&lt;/SUB&gt; exhibits a linear correlation with the shock height (r)
and electron density (\documentclass[12pt]{minimal} \usepackage{amsmath}
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\setlength{\oddsidemargin}{-69pt} \begin{document}$n_{\rm
e}$\end{document}) in logarithmic scale. This indicates that high
frequency (f&lt;SUB&gt;s&lt;/SUB&gt; 100\documentclass[12pt]{minimal}
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\begin{document}${\rm MH_{z}}$\end{document}) bursts, which occur at the
reconnection site near the solar surface, are produced from a strong
magnetically complex region. Further, strong and complex magnetic-field
regions produce shocks of higher speeds. Based on the derived plasma
parameters of the radio bursts and their relationship with f&lt;SUB&gt;s&lt;/SUB&gt;
as well as with M&lt;SUB&gt;j&lt;/SUB&gt;, we propose that the high-frequency type-
II bursts were generated in a special situation when the shock is
produced due to magnetic reconnection occurring in the low-lying coronal
loops. We conclude that type-II radio bursts can occur even in the inner
corona as well as in the outer corona; however, it depends on the
magnetic complexity of the active region in which the event occurs.</description>
</item>
<item>
<title> Coronal Signatures of Flare Generated Fast-Mode Wave at EUV and Radio Wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...63V</link>
<description>This paper presents a detailed study of the type II solar radio burst
that occurred on 06 March 2014 using combined data analysis. It is a
classical radio event consisting of type III radio burst and a following
type II radio burst in the dynamic spectrum. The type II radio burst is
observed between 235  130 MHz (120  60 MHz) in harmonic (fundamental)
bands with the life time of 5 minutes between 09:26  09:31 UT. The
estimated speed of type II burst by applying two-fold Saito model is 
650 km s&lt;SUP&gt;1&lt;/SUP&gt;. An extreme ultraviolet (EUV) wave is observed
with Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics
Observatory (SDO). The very close temporal onset association of the EUV
wave and flare energy release indicates that the EUV wave is likely
produced by a flare pressure pulse. The eruption is also accompanied by
a weak coronal mass ejection (CME) observed with the coronagraphs
onboard the Solar and Heliospheric Observatory (SOHO) and the twin Solar
Terrestrial Relations Observatory (STEREO). The plane of sky speed of
the CME was  252 km s&lt;SUP&gt;1&lt;/SUP&gt; in the SOHO/LASCO-C2 and  280 km
s&lt;SUP&gt;1&lt;/SUP&gt; in the STEREO-B/SECCHI-COR1 images. The EUV wave has two
wave fronts, one expanding radially outward and the other one moving
along the flare loop arcade. The source position of the type II burst
imaged by the Nanay Radio Heliograph (NRH) shows that it was associated
with the outward moving EUV wave. The CME is independent of the shock
wave as confirmed by the location of NRH radio sources below the CME's
leading edge. Therefore the type II radio burst is probably ignited by
the flare. This study shows the possibility of EUV wave and coronal
shock triggered by flare pressure pulse, generating the observed type II
radio burst.</description>
</item>
<item>
<title> A Statistical Investigation of the Neupert Effect in Solar Flares Observed with ASO-S/HXI</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...57L</link>
<description>The Neupert effect refers to the strong correlation between the soft
X-ray (SXR) light curve and the time-integrated hard X-ray (HXR) or
microwave flux, which is frequently observed in solar flares. In this
article, we therefore utilized the newly launched Hard X-ray Imager
(HXI) on board the Advanced Space-based Solar Observatory to investigate
the Neupert effect during solar flares. By checking the HXR light curves
at 20  50 keV, a sample of 149 events that cover the flare impulsive
phase were selected. Then, we performed a crosscorrelation analysis
between the HXR fluence (i.e., the time integral of the HXR flux) and
the SXR 1  8  flux measured by the Geostationary Operational
Environmental Satellite. All the selected flares show high correlation
coefficients (&gt;0.90), which seem to be independent of the flare location
and class. The HXR fluences tend to increase linearly with the SXR peak
fluxes. Our observations indicate that all the selected flares obey the
Neupert effect.</description>
</item>
<item>
<title> Radio-astronomical monitoring of active regions in the microwave range in the service of forecasting solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MPLA...3950069P</link>
<description>One of the key factors of space weather is solar flare activity, the
monitoring and prediction of which is an important task of specialized
dedicated groups of space experts and solar astronomers. Solar flare
forecasts are based on identifying and detecting the so-called
precursors, specific processes in solar activity events that occur
before flares. Collecting data for space weather analysis and prediction
comes down to several types of measurements performed by more than a
dozen spacecraft. Ground-based observations and monitoring nowadays are
becoming more or less complimentary. One of the reasons for this is the
limitation of observation time with ground-based telescopes due to
adverse Earth weather conditions. However, solar radio astronomy is
immune to almost any weather activity, and the main question here is
what new quality it can bring. Observational data accumulated in the
20th century show that solar radio bursts can be associated with flare
activity. In addition, the existing network of solar radio telescopes is
already well established. As an example, in this paper, we describe the
possibilities of a fully steerable 32-meter radio telescope of Ventspils
International Radio Astronomy Centre (VIRAC), Latvia, which can be
useful for searching for new precursors of solar flares.</description>
</item>
<item>
<title> The Characteristic Properties of Solar Activity in Solar Cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2024KPCB...40..105K</link>
<description>Solar cycle 24 began in December 2008 and ended in December 2019.
Maximum of solar cycle 24 occurred in April 2014. Magnetic field
intensity has been reported via data from the Wilcox Solar Observatory.
Sunspot numbers are reported via the data from WDC-SILSO, Royal
Observatory of Belgium. Sunspot area distribution was determined using
the data from the Max Planck Institute. Flare Index intensity is
indicated, and the data recorded by the Kandilli Observatory at Bogazici
University is presented. Hemisphere asymmetries in terms of sunspots and
solar flare index are calculated. The number of solar flares that occur
at the highest intensity (X-class) during this cycle are presented, the
data for which from the NOAA/SWPC. The characteristics of Coronal Mass
Ejections are given, as determined using the LASCO coronagraph operating
on the SOHO mission. Solar radio flux distribution and comparison with
previous cycles was studied using data from Space Weather Canada.</description>
</item>
<item>
<title> Periodicities observed in the solar and geomagnetic indexes and in SABER thermospheric infrared power measurements</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JASTP.25806234N</link>
<description>We analyze periodic features in the F10.7 cm solar radio flux and the Ap
geomagnetic index to examine solar-terrestrial coupling in Earth's
atmosphere above 100 km. The coupling is indicated by the same periodic
features observed in the global infrared power radiated by Nitric Oxide
(NO) and Carbon Dioxide (CO&lt;SUB&gt;2&lt;/SUB&gt;). The infrared power data have
been measured by the SABER instrument on the NASA TIMED satellite since
January 2002. A strong dominant feature for the length of the solar
cycle (11 years) can be observed in all the datasets. The length of
this periodicity can vary from 9.95 years to 12.25 years for different
solar cycles. Periodic features larger than the length of the solar
cycle are also observed in the F10.7 and Ap index (22 years and 44
years). A strong 180-day periodic feature can be observed in the Ap
index which corresponds to the well-known Russell-McPherron effect.
Additionally, the NO power and the Ap index exhibit statistically
significant periodic features for shorter periods (e.g., 27, 13.5 and 9
days). This similarity indicates a strong link between the
thermosphere's infrared energy budget and the geomagnetic conditions of
the upper atmosphere.</description>
</item>
<item>
<title> Electron cyclotron maser instability by evolving fast electron beams in the flare loops</title>
<link>https://ui.adsabs.harvard.edu/abs/2024FrASS..1104145T</link>
<description>The electron cyclotron maser instability (ECMI) stands as a pivotal
coherent radio emission mechanism widely implicated in various
astrophysical phenomena. In the context of solar activity, ECMI is
primarily instigated by energetic electrons generated during solar
eruptions, notably flares. These electrons, upon leaving the
acceleration region, traverse the solar atmosphere, forming fast
electron beams (FEBs) along magnetic field lines. It is widely accepted
that as these FEBs interact with the ambient plasma and magnetic fields,
they give rise to radio and hard X-ray emission. Throughout their
journey in the plasma, FEBs undergo modifications in their energy
spectrum and velocity spatial distribution due to diverse energy loss
mechanisms and changes in ambient plasma parameters. In this study, we
delve into the impact of the evolving energy spectrum and velocity
anisotropic distribution of FEBs on ECMI during their propagation in
flare loops. Our findings indicate that if we solely consider the
progressively flattened lower energy cutoff behavior as FEBs descend
along flare loops, the growth rates of ECMI decrease accordingly.
However, when accounting for the evolution of ambient magnetic plasma
parameters, the growth rates of ECMI increase as FEBs delve into denser
atmosphere. This underscores the significant influence of the energy
spectrum and velocity anisotropy distribution evolution of FEBs on ECMI.
Our study sheds light on a more comprehensive understanding of the
dynamic spectra of solar radio emissions.</description>
</item>
<item>
<title> Development of a 90600 MHz Meter-wave Solar Radio Spectrometer</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJS..272...21C</link>
<description>Radio observation is important for understanding coronal mass ejections
(CMEs), coronal shock waves, and high-energy electron acceleration.
Here, we developed a new Chashan broadband solar radio spectrometer at a
meter wavelength for observing the (super)fine structure of the solar
radio burst spectrum. In the signal-receiving unit, we adopt an antenna
system consisting of a 12 m large-aperture parabolic reflector and dual-
line polarized logarithmic periodic feed source, as well as a high-
precision Sun-tracking turntable system, all of which ensure the high-
precision acquisition of solar radiation signals. For the digital
receiver, we use a high-speed analog-to-digital converter with a
sampling rate of 1.25 GSPS to directly sample the signal amplified and
filtered by the analog receiver, simplifying the structure of the analog
receiver, and design a 16k-point fast Fourier transform algorithm in the
field programmable gate array to perform timefrequency transformation
on the sampled signals. The default frequency and temporal resolution of
the system are 76.294 kHz and 0.839 ms (up to 0.21 ms), respectively.
The noise coefficient of the system is less than 1 dB, the dynamic range
is more than 60 dB, and the sensitivity is as high as 1 sfu. We have
observed a large number of radio bursts, including type I radio storms,
hundreds of type III, 20 type II, and 15 type IV bursts in the past
year. These high-quality data are useful in the further study of CMEs
and associated particle acceleration and the origins of solar radio
bursts.</description>
</item>
<item>
<title> A Joint Microwave and Hard X-Ray Study toward Understanding the Transport of Accelerated Electrons During an Eruptive Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...966..208M</link>
<description>The standard flare model, despite its success, is limited in
comprehensively explaining the various processes involving nonthermal
particles. One such missing ingredient is a detailed understanding of
the various processes involved during the transport of accelerated
electrons from their site of acceleration to different parts of the
flare region. Here we use simultaneous radio and X-ray observations from
the Expanded Owens Valley Solar Array and the Spectrometer/Telescope for
Imaging X-rays on board the Solar Orbiter, respectively, from two
distinct viewing perspectives, to study the electron transport
processes. Through detailed spectral modeling of the coronal source
using radio data and footpoint sources using X-ray spectra, we compare
the nonthermal electron distribution at the coronal and footpoint
sources. We find that the flux of the nonthermal electrons precipitated
at the footpoint is an order of magnitude smaller than that trapped in
the looptop, consistent with earlier works that primarily used X-ray for
their studies. In addition, we find that the electron spectral indices
obtained from X-ray footpoints are significantly softer than the
spectral hardness of the nonthermal electron distribution in the corona.
We interpret these differences based on transport effects and the
difference in sensitivity of microwave and X-ray observations to
different regimes of electron energies. Such an understanding is crucial
for leveraging different diagnostic methods of nonthermal electrons
simultaneously to achieve a more comprehensive understanding of the
electron acceleration and transport processes of solar flares.</description>
</item>
<item>
<title> Intensity Calibration for the Mingantu Spectral Radioheliograph Images</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AcASn..65...28Z</link>
<description>The Mingantu Spectral Radioheliograph (MUSER), a new generation of solar
dedicated radio imaging spectroscopic telescope, has realized high-time,
high-angular, and high-frequency resolution imaging of the Sun in the
0.4--15 GHz ultra-broadband frequency range. The radio brightness
temperature is an important parameter to describe the solar physical
process. It plays a very important role in the study of different radio
radiation mechanisms, solar magnetic field and the acceleration of non-
thermal particles in the solar burst process. Therefore, the image of
radioheliograph must be calibrated for brightness temperature. This
paper introduces a method suitable for radioheliograph image intensity
calibration. The solar radio image contains the structural information
of the solar disk. The radio radius and intensity of the quiet solar
disk in the image can be obtained by fitting the first kind of Bessel
function with the visibilities of short baselines of the
radioheliograph. Then, the Rayleigh-Jeans law and the daily solar radio
flux can be used to calculate the calibration factor $G_{\rm c}$ of the
daily image, so as to realize the calibration of the MUSER image
intensity. Applying this method to the actual observation data of MUSER,
including different situations such as the quiet sun and solar radio
bursts, the error of the daily calibration factor $G_{\rm c}$ is within
10\% of its value, and the obtained bright temperature of the quiet sun
has a high correlation with the result obtained by other people. These
indicate the feasibility and effectiveness of this method.</description>
</item>
<item>
<title> Batch Measurement and Calibration Method of DSRT Three-axis Low Frequency Antenna Pointing Error</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AcASn..65...26T</link>
<description>Daocheng Solar Radio Telescope (DSRT) is an important part of the Solar
Interplanetary exploration subsystem of the second phase of The Chinese
Meridian Project. It operates in the 150\;MHz to 450\;MHz frequency band
and provides high-resolution spatial and temporal images of solar
eruption brightness and temperature. Aiming at the high precision
pointing measurement of the DSRT antenna and the requirement of batch
calibration and correction of pointing errors, this paper establishes
the 3-parameter, antenna encoder zero point offset pointing error model
by quaternion rotation transformation method according to the unique
three-axis mount system of DSRT. In this paper, the drift scanning
method based on radio source is proposed to obtain the radiation pattern
of 16 antennas and determine the boresight according to the two-
dimensional power pattern to accurately measure the pointing error of
the DSRT antenna. Finally, the least square method is used to get the
model parameters, and the antenna control software is used to adjust the
encoder zero point of each axis, and then the adjustment results are
verified. The results show that the pointing calibration method is
reliable and effective. The pointing accuracy of 16 antennas after
correction is within 0.5$^\circ$, which is significantly better than the
pointing error of 3.5$^\circ$ before calibration, and the error is less
than one-tenth of HBPW (half power beam width) under the maximum working
frequency of the DSRT antenna.</description>
</item>
<item>
<title> Changes in the solar atmosphere during the decay of the Modern Maximum</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...685A.170M</link>
<description>Context. The Sun experienced a period of unprecedented activity during
the 20th century, now called the Modern Maximum (MM). The decay of the
MM after its maximum in cycle 19 has changed the Sun, the heliosphere,
and the planetary environments in many ways. However, studies disagree
on whether this decay has proceeded synchronously in different solar
parameters or not. &lt;BR /&gt; Aims: One of the related key issues is if the
relation between two long parameters of solar activity, the sunspot
number and the solar 10.7 cm radio flux, has remained the same during
this decay. A recent study argues that there is an inhomogeneity in the
10.7 cm radio flux in 1980, which leads to a step-like jump ("1980
jump") in this relation. If true, this result would reduce the
versatility of possible long-term studies of the Sun during the MM. Here
we aim to show that the relation between sunspot number and 10.7 cm
radio flux does indeed vary in time, not due to an inhomogeneous radio
flux but due to physical changes in the solar atmosphere. &lt;BR /&gt;
Methods: We used radio flux measurements made in Japan at four different
wavelengths, and studied their long-term relation with the sunspot
number and the 10.7 cm radio flux during the decay of MM. We also used
two other solar parameters, the MgII index and the number of solar
active regions, in order to study the nature of the observed long-term
changes in more detail. &lt;BR /&gt; Results: We find that the 1980 jump is
only the first of a series of 1-2-year "humps" that mainly occur during
solar maxima. All five radio fluxes depict an increasing trend with
respect to the sunspot number from the 1970s to 2010s. These results
exclude the interpretation of the 1980 jump as an inhomogeneity in the
10.7 cm flux, and reestablish the 10.7 cm flux as a homogeneous measure
of solar activity. The fluxes of the longer radio waves are found to
increase with respect to the shorter waves, which suggests a long-term
change in the solar radio spectrum. We also find that the MgII index of
solar UV irradiance and the number of active regions also increased with
respect to the sunspot number, further verifying the difference in the
long-term evolution in chromospheric and photospheric parameters. &lt;BR /&gt;
Conclusions: Our results provide evidence for important structural
changes in solar magnetic fields and the solar atmosphere during the
decay of the MM, which have not been reliably documented so far. We also
emphasize that the changing relation between the different (e.g.,
photospheric and chromospheric) solar parameters should be taken into
account when using the sunspot number or any single parameter in long-
term studies of solar activity.</description>
</item>
<item>
<title> Solar Radio Burst Prediction Based on a Multimodal Model</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...49W</link>
<description>Solar radio bursts are intense radio radiation sources that occur during
the energy-release process and represent a hot topic in solar-physics
and space-weather research. In this paper, we present a multimode
prediction model for daily solar radio bursts. The model uses deep
learning and machine learning to obtain data information from different
dimensions and to establish the relationship between the characteristics
of the solar active region on the solar surface and solar radio bursts.
For this model, we use data from the Solar and Heliospheric Observatory
(SOHO)/Michelson Doppler Imager (MDI) total solar magnetic map, the
Royal Observatory of Belgium World Data Centre in Brussels, and NOAA
sunspot parameters (including number, area, and type of sunspots) as
inputs. The output results are then compared with the list of solar
radio bursts recorded by the Radio Solar Telescope Network (RSTN) to
determine whether solar radio bursts are present and to determine the
key parameters for determining radio bursts. Based on 5449 days of
observational data, we find that the prediction accuracy of the model is
0.898  0.011, and that the number of sunspots is a key parameter in
determining the occurrence of solar radio bursts. Specifically, when the
number of sunspots is greater than 15, the probability of occurrence of
solar radio bursts is greater than 90%. We have identified the key
parameters and thresholds for determining solar radio bursts and
highlighted the key parameters for space-weather prediction. In
addition, the prediction model can also be used for predicting in other
fields.</description>
</item>
<item>
<title> Forecasting Medium-Term F10.7 Using the Deep-Learning Informer Model</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...47Z</link>
<description>The daily 10.7-cm solar radio flux (F10.7) is one of the most important
solar activity indices and has been widely applied in various space
environment modeling as a crucial parameter. In this study, we adopt a
deep-learning Informer model, based on the transformer architecture to
predict the medium-term F10.7 index, which uses 48 historical daily
F10.7 indices as input to directly forecast the following 1  27 days'
F10.7 index. The model is demonstrated to be effective and to have
superior performance compared with other widely-used forecasting
techniques: two statistical methods provided by British Geological
Survey (BGS), Space Weather Prediction Center (SWPC), and a multiflux
neural network method provided by Collecte Localisation Satellites
(CLS). In comparison, the Informer model significantly improves the
forecast accuracy for the prediction horizon larger than 6 days,
especially during the solar activity descending phase and at the solar
activity minimum. For its effectiveness, accurate prediction capability
and the advantage in F10.7 forecasting with longer horizon, the Informer
could be potentially used as a candidate model for space weather
operational forecasting.</description>
</item>
<item>
<title> The arrival time and energy of FRBs traverse the time-energy bivariate space like a Brownian motion</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SciBu..69.1020Z</link>
<description>The origin of fast radio bursts (FRBs), the brightest cosmic explosion
in radio bands, remains unknown. We introduce here a novel method for a
comprehensive analysis of active FRBs' behaviors in the time-energy
domain. Using "Pincus Index" and "Maximum Lyapunov Exponent", we were
able to quantify the randomness and chaoticity, respectively, of the
bursting events and put FRBs in the context of common transient physical
phenomena, such as pulsar, earthquakes, and solar flares. In the
bivariate time-energy domain, repeated FRB bursts' behaviors deviate
significantly (more random, less chaotic) from pulsars, earthquakes, and
solar flares. The waiting times between FRB bursts and the corresponding
energy changes exhibit no correlation and remain unpredictable,
suggesting that the emission of FRBs does not exhibit the time and
energy clustering observed in seismic events. The pronounced
stochasticity may arise from a singular source with high entropy or the
combination of diverse emission mechanisms/sites. Consequently, our
methodology serves as a pragmatic tool for illustrating the congruities
and distinctions among diverse physical processes.</description>
</item>
<item>
<title> Solar radio spectrogram segmentation algorithm based on improved fuzzy C-means clustering and adaptive cross filtering</title>
<link>https://ui.adsabs.harvard.edu/abs/2024PhyS...99d5005L</link>
<description>Solar radio spectrograms contain essential information, such as the
duration type; therefore, recognizing and detecting solar radio
spectrograms are significant for the further study of solar radio. With
the upgrading of solar radio observation, considering the equipment that
has already generated amounts of data, researchers have begun to use
machine learning methods to recognize and detect solar radio
spectrograms to resolve the weaknesses of manual identification, such as
time consumption. However, the spectrograms are characterized by noise
or insignificant outburst features, which affect the recognition and
detection of solar radio spectrograms. In contrast, extracting the burst
region separately and the more distinctive spectrogram features will
help identify and detect it. Therefore, to remove the burst domain of
the radio spectrogram better, this paper combines the idea of image
segmentation and proposes a solar radio spectrogram segmentation
algorithm based on improved fuzzy C-means (FCM) clustering and adaptive
cross filtering for the extraction of the burst domain of solar radio
spectrograms. This algorithm has multiple processing steps. The first
step is solar radio spectrogram segmentation with the improved FCM based
on the kernel-induced distance by incorporating spatial constraints
combined with random walk and adaptive affiliation linking (RWAKFCM_S).
The second step is adaptive cross filtering, eliminating the noise
clustered in bursts. The results show the following. (1) The RWAKFCM_S
proposed in this paper has better anti-noise and segmentation
performance than other methods in the synthetic, natural, and solar
radio spectrogram segmentation experiments; it can also overcome the
problems of noise sensitivity when segmenting spectrograms by
traditional FCM. (2) The RWAKFCM_S can satisfy the high accuracy and
rate of solar radio spectrogram segmentation demands. (3) The adaptive
cross filtering proposed in this paper can eliminate noise clustered in
the eruption domain. (4) The proposed method enables burst region
extraction.</description>
</item>
<item>
<title> Spatial structure of resonance cavities in sunspots</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.529..967S</link>
<description>We present a study of wave processes in sunspots from active regions
NOAA 11131 on 2010 December 10 and NOAA 12565 on 2016 July 14 observed
by SDO/AIA in the 1600, 304, and 171  temperature channels. To study
the spatial structure of the resonance cavities previously found by Jess
et al., we applied spectral data processing techniques such as pixelized
wavelet filtering and mode decomposition. For the first time, we found
stable regions as waveguides of the oscillations in the sunspot umbra,
occupying specific frequency ranges without spatial overlap. The sizes
of these regions depend on the frequency oscillations, and the maximum
frequency coincides with the values of the harmonics of the main
oscillation mode. Frequency drifts were observed in the band occupied by
these regions, with different spectral slopes depending on the location
of the sources in the sunspot umbra. We suggest that the observed
distribution of wave sources in the umbra is a set of resonant cavities
where successive amplification of oscillations at selected multiple
harmonics is observed. The distribution of sources at low frequencies
indicates the influence of the atmospheric cut-off due to the
inclinations of the magnetic field lines.</description>
</item>
<item>
<title> Sources of Solar Protons in the Events of February 24-25 and July 16-17, 2023</title>
<link>https://ui.adsabs.harvard.edu/abs/2024CosRe..62..133S</link>
<description>From the beginning of January 2021 to the end of August 2023, the
radiation monitor of the Spektr-RG spacecraft registered three
enhancements in the count rate, which exceed the background variations
during the solar activity cycle and have a comparable maximum value.
These enhancements are associated with solar proton events (SPEs) from
the flares X1.0 on October 28, 2021; M6.3 on February 25, 2023; and M5.7
on July 17, 2023. Using the example of these events, as well as smaller
SPEs from the flares M3.7 on February 24, 2023, and M4.0 on July 16,
2023, threshold criteria for "proton" flares are discussed. In powerful
SPEs, the contribution of solar protons to the radiation dose can exceed
the total contribution of galactic cosmic rays (GCR) over a sufficiently
long period of time. Therefore, such SPEs are sources of increased
radiation hazard and require prediction based on real-time observations.
It was shown that, in these five flares, thresholds were overcome
according to three criteria: plasma temperature &gt;12 MK (soft X-ray
source), duration (&gt;5 min) of microwave or hard X-ray (HXR) radiation
(electron acceleration &gt;100 keV), and height of flare development
process &gt;60 Mm (radio emission at plasma frequencies &lt;610 MHz). The
arrival of the first solar protons &gt;100 MeV to the Earth's orbit was
expected no earlier than 10 min relative to the beginning of HXR or
microwave radiation, i.e., could have been predicted in advance. To
study the relationship between solar flares and SPEs, we used data from
the anticoincidence shield of the spectrometer on INTEGRAL (ACS SPI),
which is an effective but uncalibrated detector of HXR &gt;100 keV and
protons &gt;100 MeV, as well as patrol observations of radio emission at
fixed frequencies (Radio Solar Telescope Network). It is noted that the
X2.2 (N25E64) flare on February 17, 2023 satisfied all three "protonity"
criteria and could become the source of a powerful SPE near the Earth in
a case of favorable location on the Sun. In the M8.6 (N27W29) flare on
February 28, 2023, the third criterion was not met, and it did not lead
to an SPE as expected (it developed in a plasma with a density &gt;2.5 
10&lt;SUP&gt;10&lt;/SUP&gt; cm&lt;SUP&gt;-3&lt;/SUP&gt; and plasma frequency &gt;1415 MHz).</description>
</item>
<item>
<title> Comparison of Solar Multifrequency Microwave Data with Other Solar Indices for Understanding Solar and Stellar Microwave Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...965..170S</link>
<description>Thermal microwave emissions detected from stellar atmospheres contain
information on stellar activity. However, even for the Sun, the
relationship between multifrequency microwave data and other activity
indices remains unclear. We investigated the relationships among the
thermal microwave fluxes with 1, 2, 3.75, and 9.4 GHz, their circular
polarizations, and several activity indices recorded during recent solar
cycles and observed that these relationships can be categorized into two
groups. In the first group, the relationship between the microwave
fluxes and solar indices, which are strongly related to the active
regions, can be well-fitted by using a linear function. In the second
group, the fitting function is dependent on frequency. Specifically, the
microwave fluxes at 1 and 2 GHz can be well-fitted to the total unsigned
magnetic and extreme ultraviolet fluxes by employing a power-law
function. The trend changes around 3.75 GHz, and the trend for the 9.4
GHz fluxes can be fitted by using a linear function. For the first time,
we present the relationship between circular polarization and solar
indices. Moreover, we extrapolated these relationships of the solar
microwave fluxes to higher values and compared them with the solar-type
stars. We found that  Eri, whose microwave emission originates from
thermal plasma, follows the extrapolated relationship. However, to date,
only one star's emission at 110 GHz has been confirmed as thermal
emission. More solar-type stars should be observed with future radio
interferometers to confirm that relationships based on solar data can be
applied to stellar microwave data.</description>
</item>
<item>
<title> The Slipping Magnetic Reconnection and Damped Quasiperiodic Pulsations in a Circular Ribbon Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...965..137H</link>
<description>The study of circular ribbon (CR) flares is important to understand the
three-dimensional magnetic reconnection in the solar atmosphere. We
investigate the slipping brightenings and damped quasiperiodic
pulsations in a CR flare by multiwavelength observations. During the
flaring process, two extreme ultraviolet brightenings (SP1 and SP2) slip
synchronously along the ribbon in a counterclockwise direction. The
ribbon and fans between them show synchronous enhancement with the
microwave and hard X-ray (HXR) CR source. In the magnetohydrostatic
extrapolation results and observations, the dome and outer spine display
an evident counterclockwise twisting feature. We propose the slipping
reconnection occurs between the fan and outer spine in the null point,
which covers the region from SP1 to SP2. The fan of SP1 shows the
strongest twist and produces the most efficient reconnection. The ribbon
after SP1 becomes weak due to the destruction of the fan configuration.
The fan of SP2 is in the front of the slipping motion, which initiates
new reconnection and brightens the local ribbon. The twisting of the
dome continuously promotes new reconnection in the null point, which
brightens the ribbon in sequence to display a counterclockwise slipping
feature. Thus, the twist of the dome may trigger and dominate the
slipping reconnection, and the rotation of the central positive pole
could be one possible cause of the twist. After the peak, the microwave
and HXR emission shows damped oscillations at a period of 15 s. The
collapse of the fanspine structure may lead to the standing kink
oscillations of the fan to modulate the reconnection and particle
acceleration process.</description>
</item>
<item>
<title> Imaging a Large Coronal Loop Using Type U Solar Radio Burst Interferometry</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...965..107Z</link>
<description>Solar radio U-bursts are generated by electron beams traveling along
closed magnetic loops in the solar corona. Low-frequency (&lt;100 MHz)
U-bursts serve as powerful diagnostic tools for studying large-sized
coronal loops that extend into the middle corona. However, the positive
frequency drift component (descending leg) of U-bursts has received less
attention in previous studies, as the descending radio flux is weak. In
this study, we utilized LOFAR interferometric solar imaging data from a
U-burst that has a significant descending leg component, observed
between 10 and 90 MHz on 2020 June 5th. By analyzing the radio source
centroid positions, we determined the beam velocities and physical
parameters of a large coronal magnetic loop that reached just about 1.3
R &lt;SUB&gt;&lt;/SUB&gt; in altitude. At this altitude, we found the plasma
temperature to be around 1.1 MK, the plasma pressure around 0.20 mdyn,
cm&lt;SUP&gt;2&lt;/SUP&gt;, and the minimum magnetic field strength around 0.07 G.
The similarity in physical properties determined from the image suggests
a symmetric loop. The average electron beam velocity on the ascending
leg was found to be 0.21c, while it was 0.14c on the descending leg.
This apparent deceleration is attributed to a decrease in the range of
electron energies that resonate with Langmuir waves, likely due to the
positive background plasma density gradient along the downward loop leg.</description>
</item>
<item>
<title> Electrostatic Wave Decay in the Randomly Inhomogeneous Solar Wind</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...964L..30K</link>
<description>Despite a few space observations where Langmuir and ion acoustic waves
are expected to participate in the mechanism of electrostatic decay,
this is to date believed to be the main and fastest nonlinear wave
process in the solar wind. However, in such a plasma where random
density fluctuations are ubiquitous, the question of whether nonlinear
wave processes play a significant role in Langmuir wave turbulence
generated by electron beams associated with type III solar radio bursts
remains still open. This paper provides several answers by studying,
owing to two-dimensional challenging particle-in-cell simulations, the
dynamics and the properties of the ion acoustic waves excited by such
Langmuir wave turbulence and the role they play in the electrostatic
decay. The impact on this process of plasma background density
fluctuations and electron-to-ion temperature ratio is studied. Moreover,
it is shown that, for a typical solar wind plasma with an average level
of density fluctuations of a few percent of the ambient density and a
temperature ratio of the order of 1, nonlinear induced scattering off
ions occurs, with small intensity low-frequency quasi-modes and only in
localized plasma regions where density is depleted or weakly perturbed
by low-frequency turbulence.</description>
</item>
<item>
<title> Episodic Energy Release during the Main and Post-impulsive Phases of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...964..174W</link>
<description>When and where the magnetic field energy is released and converted in
eruptive solar flares remains an outstanding topic in solar physics. To
shed light on this question, here we report multiwavelength observations
of a C9.4-class eruptive limb flare that occurred on 2017 August 20. The
flare, accompanied by a magnetic flux rope eruption and a white light
coronal mass ejection, features three post-impulsive X-ray and microwave
bursts immediately following its main impulsive phase. For each burst,
both microwave and X-ray imaging suggest that the nonthermal electrons
are located in the above-the-loop-top region. Interestingly, contrary to
many other flares, the peak flux of the three post-impulsive microwave
and X-ray bursts shows an increase for later bursts. Spectral analysis
reveals that the sources have a hardening spectral index, suggesting a
more efficient electron acceleration into the later post-impulsive
bursts. We observe a positive correlation between the acceleration of
the magnetic flux rope and the nonthermal energy release during the
post-impulsive bursts in the same event. Intriguingly, different from
some other eruptive events, this correlation does not hold for the main
impulse phase of this event, which we interpret as energy release due to
the tether-cutting reconnection before the primary flux rope
acceleration occurs. In addition, using footpoint brightenings at
conjugate flare ribbons, a weakening reconnection guide field is
inferred, which may also contribute to the hardening of the nonthermal
electrons during the post-impulsive phase.</description>
</item>
<item>
<title> Solar Type J Radio Bursts and the Associated Coronal Loop</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...964..108F</link>
<description>The solar type J radio burst is a variant of type III bursts, which are
a probe for understanding solar energetic electrons and local electron
density. This study investigates a type J burst event on 2017 September
9. We have combined the data from the extreme-ultraviolet (EUV) imaging
and the EUV Imaging Spectrometer (EIS) to analyze the event. Within 4
minutes several type J bursts with similar morphology occur. Two of
them, with clear fundamental and second harmonic bands, are studied in
detail. We find a delay of 2  0.5 s between their different harmonic
bands. During type J bursts, only one coronal loop brightens
significantly at its northern footpoint, in correlation with the
continuous injection of erupting jets into the loop. The EUV intensity
of the brightening footpoint is correlated with the radio flux at 245
and 410 MHz, with correlation coefficients of 0.2 and 0.4, respectively.
These observations suggest that the type J bursts should originate from
this coronal loop. By analyzing the electron number density distribution
along the coronal loop diagnosed from the EIS data and the time
evolution of the plasma frequency calculated from the type J burst, we
determine that the velocities of the energetic electrons exciting the
two type Js are 0.10  0.02c and 0.12  0.02c. Our results confirm
previous studies on type J bursts.</description>
</item>
<item>
<title> Long-term variations in the mesopause region derived from OH*(3,1) rotational temperature observations at Wuppertal, Germany, from 1988 - 2022</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..73.3398K</link>
<description>We analysed the time series of OH*(3,1) rotational temperatures observed
from Wuppertal in the time interval 1988 - 2022. The long-term evolution
of the time series is characterised by two components. Firstly, we
derived a significant correlation of the temperatures and the F10.7 cm
solar radio flux. The sensitivity to the 11-year cycle of solar activity
is 4.8  0.7 K (100 SFU)&lt;SUP&gt;-1&lt;/SUP&gt;. Then we show that the second
major component in addition to this solar influence is a significant
long-period oscillation. The oscillation has a period of P = 22.2  1.5
years with an amplitude of A = 1.8  0.4 K. A significant linear trend
cannot be derived for the time series of OH*(3,1) rotational
temperatures. Due to the long-period oscillation the derivation of
linear trends heavily depends on the analysed time interval. This
explains the different linear trends that have been derived in past
studies for this time series. All of the previous results for this
quantity are in good agreement with the long-period oscillation
determined here, because different parts of the time series and,
therefore, different parts of the oscillation (e.g mainly downswing or a
complete cycle) have been analysed which led to largely different linear
trends.</description>
</item>
<item>
<title> Imaging spectroscopy of a spectral bump in a type II radio burst</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684L..22Z</link>
<description>Context. Observations of solar, type II radio bursts provide a unique
opportunity to analyze the nonthermal electrons accelerated by coronal
shocks and diagnose the plasma density distribution in the corona.
However, there are very few high-frequency resolution interferometric
observations of type II radio bursts that are capable of tracking these
electrons. &lt;BR&gt; Aims: Recently, more spatially resolved high-resolution
observations of type II radio bursts have been recorded with the Low-
Frequency Array (LOFAR). Using these observations, we aim to track the
location of a type II radio burst that experienced a sudden spectral
bump. &lt;BR&gt; Methods: We present the first radio imaging observations of a
type II burst with a spectral bump. We measured the variation in source
location and frequency drift of the burst and deducted the density
distribution along its propagation direction. &lt;BR&gt; Results: We have
identified a type II burst that experiences a sudden spectral bump in
its frequency-time profile. The overall frequency drift rate is 0.06 MHz
s&lt;SUP&gt;1&lt;/SUP&gt;, and this corresponds to an estimated speed of 295 km
s&lt;SUP&gt;1&lt;/SUP&gt;. The projected velocity of the radio source obtained from
imaging is 380 km s&lt;SUP&gt;1&lt;/SUP&gt; toward the east. At the spectral bump,
a deviation in the source locations of the type II split bands is
observed. The band separation increases significantly in the north-south
direction. &lt;BR&gt; Conclusions: The spectral bump shows an 8 MHz deviation
at 60 MHz, which corresponds to a 25% decrease in the plasma density.
The estimated crossing distance during the spectrum bump was 29 mm,
suggesting that this density variation occurs in a confined area. This
indicates that the shock most likely encountered the upper extent of a
coronal hole. &lt;P /&gt;Movie associated to Fig. 1 is available at &lt;A HREF="h
ttps://www.aanda.org/10.1051/0004-6361/202449365/olm"&gt;https://www.aanda.
org&lt;/A&gt;.</description>
</item>
<item>
<title> Tracking the motion of a shock along a channel in the low solar corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684L...7R</link>
<description>Context. Shock waves are excited by coronal mass ejections (CMEs) and
large-scale extreme-ultraviolet (EUV) wave fronts and can result in low-
frequency radio emission under certain coronal conditions. &lt;BR /&gt; Aims:
In this work, we investigate a moving source of low-frequency radio
emission as a CME and an associated EUV wave front move along a channel
of a lower density, magnetic field, and Alfvn speed in the solar
corona. &lt;BR /&gt; Methods: Observations from the Atmospheric Imaging
Assembly on board the Solar Dynamics Observatory, the Nanay Radio
Heliograph (NRH), and the Irish Low Frequency Array (I-LOFAR) were
analysed. Differential emission measure maps were generated to determine
densities and Alfvn maps, and the kinematics of the EUV wave front was
tracked using CorPITA. The radio sources' positions and velocity were
calculated from NRH images and I-LOFAR dynamic spectra. &lt;BR /&gt; Results:
The EUV wave expanded radially with a uniform velocity of 500 km
s&lt;SUP&gt;1&lt;/SUP&gt;. However, the radio source was observed to be deflected
and appeared to move along a channel of a lower Alfvn speed, abruptly
slowing from 1700 km s&lt;SUP&gt;1&lt;/SUP&gt; to 250 km s&lt;SUP&gt;1&lt;/SUP&gt; as it
entered a quiet-Sun region. A shock wave with an apparent radial
velocity of &gt; 420 km s&lt;SUP&gt;1&lt;/SUP&gt; was determined from the drift rate
of the associated Type II radio burst. &lt;BR /&gt; Conclusions: The apparent
motion of the radio source may have resulted from a wave front moving
along a coronal wave guide or by different points along the wave front
emitting at locations with favourable conditions for shock formation.</description>
</item>
<item>
<title> Localising pulsations in the hard X-ray and microwave emission of an X-class flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684A.215C</link>
<description>&lt;BR /&gt; Aims: The aim of this work is to identify the mechanism driving
pulsations in hard X-ray (HXR) and microwave emission during solar
flares. Using combined HXR and microwave observations from Solar
Orbiter/STIX and EOVSA, we investigate an X1.3 GOES class flare,
2022-03-30T17:21:00, which displays pulsations on timescales evolving
from 7 s in the impulsive phase to 35 s later in the flare. &lt;BR /&gt;
Methods: We analysed the temporal, spatial, and spectral evolution of
the HXR and microwave pulsations during the impulsive phase of the
flare. We reconstructed images for individual peaks in the impulsive
phase and performed spectral fitting at high cadence throughout the
first phase of pulsations. &lt;BR /&gt; Results: Our imaging analysis
demonstrates that the HXR and microwave emission originates from
multiple sites along the flare ribbons. The brightest sources and the
location of the emission change in time. Through HXR spectral analysis,
the electron spectral index is found to be anti-correlated with the HXR
flux, showing a "soft-hard-soft" spectral index evolution for each
pulsation. The timing of the associated filament eruption coincides with
the early impulsive phase. &lt;BR /&gt; Conclusions: Our results indicate that
periodic acceleration and/or injection of electrons from multiple sites
along the flare arcade is responsible for the pulsations observed in HXR
and microwave emission. The evolution of pulsation timescales is likely
a result of changes in the 3D magnetic field configuration over time
related to the associated filament eruption. &lt;P /&gt;Movie is available at
&lt;A href="https://www.aanda.org/10.1051/0004-6361/202348652/olm"&gt;https://
www.aanda.org&lt;/A&gt;.</description>
</item>
<item>
<title> Tracking solar radio bursts using Bayesian multilateration</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684A.182C</link>
<description>Context. Solar radio bursts (SRBs), such as Type IIs and IIIs, are
emitted by electrons propagating through the corona and interplanetary
space. Tracking such bursts is key to understanding the properties of
accelerated electrons and radio wave propagation as well as the local
plasma environment that they propagate through. &lt;BR&gt; Aims: In this work,
we present a novel multilateration algorithm called BayEsian
LocaLisation Algorithm (BELLA) and validate the algorithm using
simulated and observed SRBs. In addition, apparent SRB positions from
BELLA are compared with comparable localisation methods and the
predictions of solar wind models. &lt;BR&gt; Methods: BELLA uses Bayesian
inference to create probabilistic distributions of source positions and
their uncertainties. This facilitates the estimation of algorithmic,
instrumental, and physical uncertainties in a quantitative manner. &lt;BR&gt;
Results: We validated BELLA using simulations and a Type III SRB
observed by STEREO A and STEREO B at 116 from the Sun-Earth line and
by Wind at L1. BELLA tracked the Type III source from 10-150
R&lt;SUB&gt;&lt;/SUB&gt; (2-0.15 MHz) along a spiral trajectory. This allowed for
an estimate of an apparent solar wind speed of v&lt;SUB&gt;sw&lt;/SUB&gt;  400 km
s&lt;SUP&gt;1&lt;/SUP&gt; and a source longitude of &lt;SUB&gt;0&lt;/SUB&gt;  30. We
compared these results with well-established methods of positioning:
Goniopolarimetric (GP), analytical time-difference-of-arrival (TDOA),
and Solar radio burst Electron Motion Tracker (SEMP). We found them to
be in agreement with the results obtained by BELLA. Additionally, the
results aligned with solar wind properties assimilated by the
Heliospheric Upwind Extrapolation with time dependence (HUXt) model.
&lt;BR&gt; Conclusions: We have validated BELLA and used it to identify
apparent source positions as well as velocities and densities of the
solar wind. Furthermore, we identified higher than expected electron
densities, suggesting that the true emission sources were at lower
altitudes than those identified by BELLA, an effect that may be due to
appreciable scattering of electromagnetic waves by electrons in
interplanetary space.</description>
</item>
<item>
<title> Study of solar brightness profiles in the 18-26 GHz frequency range with INAF radio telescopes. II. Evidence of coronal emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684A.123M</link>
<description>Context. One of the most important objectives of solar physics is to
gain a physical understanding of the solar atmosphere, whose structure
can also be described in terms of the density (N) and temperature (T)
distributions of the atmospheric matter. Several multi-frequency
analyses have shown that the characteristics of these distributions are
still under debate, especially for outer coronal emission. &lt;BR /&gt; Aims:
We aim to constrain the T and N distributions of the solar atmosphere
through observations in the centimetric radio domain. We employed
single-dish observations from two of the INAF radio telescopes at the
K-band frequencies (18-26 GHz). We investigated the origin of the
significant brightness temperature (T&lt;SUB&gt;B&lt;/SUB&gt;) detected up to the
upper corona (at an altitude of 800 Mm with respect to the photospheric
solar surface). &lt;BR /&gt; Methods: To probe the physical origin of the
atmospheric emission and to constrain instrumental biases, we reproduced
the solar signal by convolving specific 2D antenna beam models. We
performed an analysis of the solar atmosphere by adopting a physical
model that assumes the thermal bremsstrahlung as the emission mechanism,
with specific T and N distributions. We compared the modelled
T&lt;SUB&gt;B&lt;/SUB&gt; profiles with those observed by averaging solar maps
obtained at 18.3 and 25.8 GHz during the minimum of solar activity
(2018-2020). &lt;BR /&gt; Results: We probed any possible discrepancies
between the T and N distributions assumed from the model and those
derived from our measurements. The T and N distributions are compatible
(within a 25% of uncertainty) with the model up to 60 Mm and 100 Mm in
altitude, respectively. &lt;BR /&gt; Conclusions: Our analysis of the role of
the antenna beam pattern on our solar maps proves the physical nature of
the atmospheric emission in our images up to the coronal tails seen in
our T&lt;SUB&gt;B&lt;/SUB&gt; profiles. Our results suggest that the modelled T and
N distributions are in good agreement (within 25% of uncertainty) with
our solar maps up to altitudes of 100 Mm. A subsequent, more
challenging analysis of the coronal radio emission at higher altitudes,
together with the data from satellite instruments, will require further
multi-frequency measurements.</description>
</item>
<item>
<title> Study of solar brightness profiles in the 18-26 GHz frequency range with INAF radio telescopes. I. Solar radius</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...684A.122M</link>
<description>Context. The Sun is an extraordinary workbench, on which several
fundamental astronomical parameters can be measured with high precision.
Among these parameters, the solar radius R&lt;SUB&gt;&lt;/SUB&gt; plays an
important role in several aspects, for instance, in evolutionary models.
Moreover, it conveys information about the structure of the different
layers that compose the solar interior and its atmosphere. Despite the
efforts to obtain accurate measurements of R&lt;SUB&gt;&lt;/SUB&gt;, the subject is
still debated, and measurements are puzzling and/or lacking in many
frequency ranges. &lt;BR /&gt; Aims: We determine the mean, equatorial, and
polar radii of the Sun (R&lt;SUB&gt;c&lt;/SUB&gt;, R&lt;SUB&gt;eq&lt;/SUB&gt;, and
R&lt;SUB&gt;pol&lt;/SUB&gt;) in the frequency range 18.1  26.1 GHz. We employed
single-dish observations from the newly appointed Medicina Gavril Grueff
Radio Telescope and the Sardinia Radio Telescope (SRT) in five years,
from 2018 to mid-2023, in the framework of the SunDish project for solar
monitoring. &lt;BR /&gt; Methods: Two methods for calculating the radius at
radio frequencies were employed and compared: the half-power, and the
inflection point. To assess the quality of our radius determinations, we
also analysed the possible degrading effects of the antenna beam pattern
on our solar maps using two 2D models (ECB and 2GECB). We carried out a
correlation analysis with the evolution of the solar cycle by
calculating Pearson's correlation coefficient  in the 13-month running
means. &lt;BR /&gt; Results: We obtained several values for the solar radius,
ranging between 959 and 994 arcsec, and , with typical errors of a few
arcseconds. These values constrain the correlation between the solar
radius and solar activity, and they allow us to estimate the level of
solar prolatness in the centimeter frequency range. &lt;BR /&gt; Conclusions:
Our R&lt;SUB&gt;&lt;/SUB&gt; measurements are consistent with the values reported
in the literature, and they provide refined estimates in the centimeter
range. The results suggest a weak prolateness of the solar limb
(R&lt;SUB&gt;eq&lt;/SUB&gt; &gt; R&lt;SUB&gt;pol&lt;/SUB&gt;), although R&lt;SUB&gt;eq&lt;/SUB&gt; and
R&lt;SUB&gt;pol&lt;/SUB&gt; are statistically compatible within 3 errors. The
correlation analysis using the solar images from the Grueff Radio
Telescope shows (1) a positive correlation between solar activity and
the temporal variation in R&lt;SUB&gt;c&lt;/SUB&gt; (and R&lt;SUB&gt;eq&lt;/SUB&gt;) at all
observing frequencies, and (2) a weak anti-correlation between the
temporal variation of R&lt;SUB&gt;pol&lt;/SUB&gt; and solar activity at 25.8 GHz.</description>
</item>
<item>
<title> Ionospheric TEC Prediction Based on Ensemble Learning Models</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SpWea..2203790Z</link>
<description>In this paper, we propose the usage of an ensemble learning approach for
predicting total electron content (TEC). The training data set spans
from 2007 to 2016, while the testing data set is set to the year 2017.
The model inputs in our study included Solar radio flux (F107), Solar
Wind plasma speed, By, Bz, Dst, Ap, AE, day of year, universal time,
30-day and 90-day TEC averages. Specifically, eXtreme Gradient Boosting
(XGBoost), Gradient Boosting Decision Tree, and Decision Tree were
utilized for 1-hr TEC prediction at high- (80W, 80N), mid- (80W,
40N), and low- latitudes (80W, 10N). Results indicate that all three
models performed well in predicting TEC, with a mean error of only
approximately 0.6 TECU at high- and mid- latitudes and 1.13 TECU at low
latitudes. At the same time, we compared the model with 1-day Beijing
University of Aeronautics and Astronautics model during the period of
magnetic storm from 25 August 2018 to 27 August 2018 and a quiet period
from 13 December 2018 to 15 December 2018. In the magnetic storm period,
Our model showed an average reduction of 1.83 TECU compared to BUAA
model. During the quiet period, XGBoost exhibit an average error that is
1.14 TECU lower than that of BUAA model. Moreover, TEC prediction over
the region between the 20N-45N and 70E120E during geomagnetic storm
has an error of 2.74 TECU, showing the stability and superiority of
XGBoost. Overall, the ensemble learning approach exhibits its advantage
in predicting TEC.</description>
</item>
<item>
<title> Multiwavelength Observations of Quasiperiodic Pulsations in the Impulsive Phase of an Eruptive Flare with the Hard X-Ray Imager On Board ASO-S and Other Instruments</title>
<link>https://ui.adsabs.harvard.edu/abs/2024SoPh..299...30S</link>
<description>We investigated the quasiperiodic pulsations (QPPs) of the X1.2 solar
flare (SOL2023-01-06T00:57) based on multi-instrument observations,
especially the Hard X-ray Imager (HXI) on board the Advanced Space-based
Solar Observatory (ASO-S). The quasiperiod of 27 s was identified in
hard X-rays (HXR) and microwaves using the Markov Chain Monte Carlo
method, while no corresponding oscillation was found in soft X-rays. The
HXI imaging demonstrates that HXR pulsations arise from the double-
footpoint HXR sources. Moreover, the fluctuation of 27 s period was
also present in the nonthermal electron power-law index derived from the
X-ray spectra, which is the signature of periodic electron
acceleration/precipitation during the impulsive phase. The electron
spectral indices not only exhibited the well-known "softhardsoft"
evolution, but also showed the negative correlation with the HXR
pulsations. These results suggest that QPPs directly originate from
quasiperiodic injections of accelerated electrons into flare-loop
footpoints. We also discuss the possible generation mechanisms for QPPs.</description>
</item>
<item>
<title> Circular-ribbon flares and the related activities</title>
<link>https://ui.adsabs.harvard.edu/abs/2024RvMPP...8....7Z</link>
<description>Solar flares are an impulsive increase of emissions as a result of
impetuous release of magnetic free energy. This paper will present the
recent progress on circular-ribbon flares (CRFs) and their related
activities, including coronal jets, filaments, coronal mass ejections
(CMEs), radio bursts, coronal dimmings, and coronal loop oscillations.
Owing to the prevalence of three-dimensional (3D) magnetic null points
and the corresponding fan-spine topology in the solar atmosphere, CRFs
are regularly observed in ultraviolet (UV), extreme-ultraviolet (EUV),
and H passbands. Spine reconnection and fan reconnection around the
null points are predominantly responsible for the energy release and
subsequent particle acceleration. Slipping reconnection at quasi-
separatrix layers (QSLs) may explain the sequential brightening or rapid
degradation of the circular ribbons. Periodic or quasi-periodic
acceleration and precipitation of non-thermal particles in the
chromosphere produce observed quasi-periodic pulsations (QPPs) of CRFs
in multiple altitudes as well as wavelengths. Like two-ribbon flares,
the injected high-energy particles result in explosive evaporation in
circular and inner ribbons, which is characterized by simultaneous
blueshifts in the coronal emission lines and redshifts in the
chromospheric emission lines. Homologous CRFs residing in the same
active region present similar morphology, evolution, and energy
partition. The peculiar topology of CRFs with closed outer spines
facilitates remote brightenings and EUV late phases, which are uncommon
in two-ribbon flares. Besides, CRFs are often accompanied by coronal
jets, type III radio bursts, CMEs, shock waves, coronal dimmings, and
kink oscillations in coronal loops and filaments. Magnetohydrodynamics
numerical simulations are very helpful to understand the key problems
that are still unclear up to now. Multiwavelength and multipoint
observations with state-of-the-art instruments are enormously desired to
make a breakthrough. The findings in CRFs are important for a
comprehensive understanding of solar flares and have implication for
stellar flares.</description>
</item>
<item>
<title> a first-principles precursor for astrophysical radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.529..169B</link>
<description>Electromagnetic fundamental and harmonic emission is ubiquitously
observed throughout the heliosphere, and in particular it is commonly
associated with the occurrence of type II and III solar radio bursts.
Classical analytic calculations for the plasma-emission process, though
useful, are limited to idealized situations; a conclusive numerical
verification of this theory is still lacking, with earlier studies often
providing contradicting results on e.g. the precise parameter space in
which fundamental and harmonic emission can be produced. To accurately
capture the chain of mechanisms underlying plasma emission - from
precursor plasma processes to the generation of electromagnetic waves
over long times - we perform large scale, first-principles simulations
of beam-plasma instabilities. By employing a very large number of
computational particles we achieve very low numerical noise, and explore
(with an array of simulations) a wide parameter space determined by the
beam-plasma density ratio and the ion-to-electron temperature ratio. In
particular, we observe direct evidence of both fundamental and harmonic
plasma emission when the beam-to-background density ratio 0.005 (with
beam-to-background energy ratio ~0.5), tightly constraining this
threshold. We observe that, asymptotically, in this regime $\sim 0.1~{{\
\rm per\ cent}}$ of the initial beam energy is converted into harmonic
emission, and $\sim 0.001~{{\ \rm per\ cent}}$ into fundamental
emission. In contrast with previous studies, we also find that this
emission is independent of the ion-to-electron temperature ratio. In
addition, we report the direct detection of third-harmonic emission in
all of our simulations, at power levels compatible with observations.
Our findings have important consequences for understanding the viable
conditions leading to plasma emission in space systems, and for the
interpretation of observed electromagnetic signals throughout the
heliosphere.</description>
</item>
<item>
<title> Absence of High Frequency Echoes From Ionosondes During the 23-25 April 2023 Geomagnetic Storm; What Happened?</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JGRA..12932277H</link>
<description>We report an unusual event on absence of high frequency (HF) echoes in
ionosonde observations from the ionospheric F2 region during the
geomagnetic storm of 23-25 April 2023. This event was observed in both
southern and northern hemispheres over two stations, Grahamstown
(33.3S, 26.5E), South Africa and Pruhonice (50.0N, 14.6E), Czech
Republic. Significant O/N&lt;SUB&gt;2&lt;/SUB&gt; depletion over the stations was
observed by TIMED/GUVI, indicating a strong negative ionospheric storm.
This is unique since absence of echoes in ionosonde measurements is
usually due to strong radio absorption in the ionosphere associated with
solar flares. However, there was no flare activity during the periods of
"absent" F2 HF echoes. On the other hand, the ionosonde detected echoes
from E-layer. TIEGCM simulation reproduced TIMED/GUVI O/N&lt;SUB&gt;2&lt;/SUB&gt;
depletion and showed that NmE was larger than NmF2 on dayside over
Pruhonice. TIMED/GUVI O/N&lt;SUB&gt;2&lt;/SUB&gt; also showed a clear spatial
gradient in the O/N&lt;SUB&gt;2&lt;/SUB&gt; depleted regions, suggesting F-region
ionosphere was tilted. By estimating the critical frequency of the F2
layer using GNSS observations, we have shown that it wasn't possible for
the ionospheric electron density to reach depletion levels prohibiting
reflection of HF echoes from ionosondes. We suggest that this phenomena
may have been caused by either (a) maximum electron density of E layer
exceeding that of F2 layer and/or (b) ionospheric tilting which made the
signals to be reflected far away from the ionosonde locations.</description>
</item>
<item>
<title> Element abundance and the physics of solar energetic particles</title>
<link>https://ui.adsabs.harvard.edu/abs/2024FrASS..1168043R</link>
<description>The acceleration and transport of solar energetic particles (SEPs) cause
their abundance, measured at a constant velocity, to be enhanced or
suppressed as a function of the magnetic rigidity of each ion, and
hence, of its atomic mass-to-charge ratio of A/Q. Ion charges, in turn,
depend upon the source electron temperature. In small "impulsive" SEP
events, arising from solar jets, acceleration during magnetic
reconnection causes steep power-law abundance enhancements. These
impulsive SEP events can have 1,000-fold enhancements of heavy elements
from sources at 2.5 MK and similar enhancements of 3He/4He and of
streaming electrons that drive type-III radio bursts. Gamma-ray lines
show that solar flares also accelerate 3He-rich ions, but their
electrons and ions remain trapped in magnetic loops, so they dissipate
their energy as X-rays, -rays, heat, and light. "Gradual" SEPs
accelerated at shock waves, driven by fast coronal mass ejections
(CMEs), can show power-law abundance enhancements or depressions, even
with seed ions from the ambient solar corona. In addition, shocks can
reaccelerate seed particles from residual impulsive SEPs with their pre-
existing signature heavy-ion enhancements. Different patterns of
abundance often show that heavy elements are dominated by a source
different from that of H and He. Nevertheless, the SEP abundance,
averaged over many large events, defines the abundance of the corona
itself, which differs from the solar photosphere as a function of the
first ionization potential (FIP) since ions, with FIP &lt;10 eV, are driven
upward by forces of electromagnetic waves, which neutral atoms, with FIP
&gt;10 eV, cannot feel. Thus, SEPs provide a measurement of element
abundance in the solar corona, distinct from solar wind, and may even
better define the photosphere for some elements.</description>
</item>
<item>
<title> Toward a General Empirical Model for the Study of Planetary Aeronomy</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJS..271...11X</link>
<description>Accurate estimation of the solar vacuum ultraviolet irradiance between
0.1 and 200 nm is critical for the study of planetary aeronomy. Previous
empirical models have relied on a limited number of reference spectra,
or on multiple data sets with various degrees of uncertainty, and on an
empirical selection of solar proxies. Here we propose a novel method for
the development of empirical models based on Fourier transform and
least-squares fitting of the long-term measurements from the Solar EUV
Experiment on the Thermosphere Ionosphere Mesosphere Energetics and
Dynamics mission. A Fourier transform analysis is performed to examine a
large number of solar proxies, which reveals that the solar radio flux
at 10.7 cm and the solar Ly flux at 121.6 nm are better proxies for
solar irradiance below and above 120 nm, respectively. Using these two
proxies, a nonlinear empirical model is developed through Fourier
transform and least-squares fitting of solar irradiance measurements,
which can reproduce the solar irradiance with uncertainties of only
1%2% above 120 nm, 2%4% within 45120 nm, and 4%8% below 45 nm.
Comparison with measurements from the Extreme Ultraviolet Monitor on the
Mars Atmosphere and Volatile Evolution mission indicates that the solar
irradiance at Mars can be predicted with uncertainties of less than 8%
by geometric extrapolation of the solar irradiance measured from Earth,
provided that the measurements from Earth can be calibrated accurately.
Our study provides a general method for the development of empirical
models using long-term observations in planetary aeronomy.</description>
</item>
<item>
<title> Second Harmonic Electromagnetic Wave Emissions from a Turbulent Plasma with Random Density Fluctuations</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...964...65K</link>
<description>In the solar wind, electromagnetic waves at the harmonic plasma
frequency 2 &lt;SUB&gt; p &lt;/SUB&gt; can be generated as a result of coalescence
between forward- and backward-propagating Langmuir waves. A new approach
to calculate their radiation efficiency in plasmas with external
background density fluctuations is developed. The evolution of Langmuir
wave turbulence is studied by solving numerically the Zakharov equations
in a two-dimensional randomly inhomogeneous plasma. Then, the dynamics
of the nonlinear electric currents modulated at frequencies close to 2
&lt;SUB&gt; p &lt;/SUB&gt; are calculated, as well as their radiation into harmonic
electromagnetic waves. In the frame of this non-self-consistent approach
where all transformations of Langmuir waves on density inhomogeneities
are taken into account, the electromagnetic wave radiation rate
(emissivity) is determined numerically as well as analytically,
providing in both cases similar results. Moreover, scaling laws of the
harmonic wave emissivity as a function of the ratio of the light
velocity to the electron plasma thermal velocity are found. It is also
shown how the emissivity depends on the average level of density
fluctuations and on the isotropic/anisotropic character of the Langmuir
waves' and density fluctuations' spectra.</description>
</item>
<item>
<title> Evidence for flare-accelerated particles in large scale loops in the behind-the-limb gamma-ray solar flare of September 29, 2022</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A.208P</link>
<description>We report on the detection of the gamma-ray emission above 100 MeV from
the solar flare of September 29, 2022, by Fermi LAT with simultaneous
coverage in HXR by Solar Orbiter STIX. The Solar Orbiter-Earth
separation was 178 at the time of the flare as seen from Earth, with
Solar Orbiter observing the east limb. Based on STIX imaging, the flare
was located 16 behind the eastern limb as seen from Earth. The STIX and
GBM non-thermal emission and the LAT emission above 100 MeV all show
similarly shaped time profiles, and the Fermi profiles peaked only 20 s
after the STIX signal from the main flare site, setting this flare apart
from all the other occulted flares observed by Fermi LAT. The radio
spectral imaging based on the Nanay Radioheliograph and ORFEES
spectrograph reveal geometries consistent with a magnetic structure that
connects the parent active region behind the limb to the visible disk.
We studied the basic characteristics of the gamma-ray time profile, in
particular, the rise and decay times and the time delay between the
gamma-ray and HXR peak fluxes. We compared the characteristics of this
event with those of four Fermi LAT behind-the-limb flares and with an
on-disk event and found that this event is strikingly similar to the
impulsive on-disk flare. Based on multiwavelength observations, we find
that the gamma-ray emission above 100 MeV originated from ions
accelerated in the parent active region behind the limb and was
transported to the visible disk via a large magnetic structure connected
to the parent active region behind the limb. Our results strongly
suggest that the source of the emission above 100 MeV from the September
29, 2022 flare cannot be the CME-driven shock. &lt;P /&gt;Movie is available
at &lt;A href="https://www.aanda.org/10.1051/0004-6361/202348088/olm"&gt;https
://www.aanda.org&lt;/A&gt;.</description>
</item>
<item>
<title> Spatially resolved radio signatures of electron beams in a coronal shock</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A.123Z</link>
<description>Context. Type II radio bursts are a type of solar radio bursts
associated with coronal shocks. Type II bursts usually exhibit fine
structures in dynamic spectra that represent signatures of accelerated
electron beams. So far, the sources of individual fine structures in
type II bursts have not been spatially resolved in high-resolution low-
frequency radio imaging. &lt;BR /&gt; Aims: The objective of this study is to
resolve the radio sources of the herringbone bursts found in type II
solar radio bursts and investigate the properties of the acceleration
regions in coronal shocks. &lt;BR /&gt; Methods: We used low-frequency
interferometric imaging observations from the Low Frequency Array to
provide a spatially resolved analysis for three herringbone groups (A,
B, and C) in a type II radio burst that occurred on 16 October 2015. &lt;BR
/&gt; Results: The herringbones in groups A and C have a typical frequency
drift direction and a propagation direction along the frequency. Their
frequency drift rates correspond to those of type III bursts and
previously studied herringbones. Group B has a more complex spatial
distribution, with two distinct sources separated by 50 arcsec and no
clear spatial propagation with frequency. One of the herringbones in
group B was found to have an exceptionally large frequency drift rate.
&lt;BR /&gt; Conclusions: The characteristics derived from imaging
spectroscopy suggest that the studied herringbones originate from
different processes. Herringbone groups A and C most likely originate
from single-direction beam electrons, while group B may be explained by
counterstreaming beam electrons.</description>
</item>
<item>
<title> Identification and extraction of type II and III radio bursts based on YOLOv7</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A..90Z</link>
<description>Solar radio bursts (SRBs) are extreme space weather events characterized
by intense solar radio emissions that are closely related to solar
flares. They represent signatures of the same underlying processes that
are responsible for well-documented solar phenomena such as sunspots,
solar flares, and coronal mass ejections (CMEs). The study of SRBs holds
significant importance as it provides a means to monitor and predict
solar flares and CMEs, enhancing our ability to forecast potential
impacts on Earth's communications and satellites. Typically, SRBs below
several hundred megahertz can be categorized into five types (I-V), with
type II and type III bursts being the most prevalent. This study
introduces a novel approach based on the YOLOv7 model for the detection
and classification of type II and type III SRBs. The proposed method
effectively identifies and classifies various SRB types, achieving a
mean average precision accuracy of 73.5%. A trained neural network was
deployed for SRB detection in the Chashan Broadband Solar radio
spectrograph at meter wavelength (CBSm) data, enabling the extraction of
valuable SRB information for subsequent research. This demonstrates that
even when we are dealing with extensive datasets, this method can
automatically recognize outbursts and extract pertinent physical
information. Although our experiments with the CBSm dataset currently
rely on the daily spectrum, further advancements in CBSm backend data
processing techniques are expected to enable near-real-time burst
detection, which is a powerful tool for accurately assessing and
analyzing SRBs, and significantly contribute to the field of space
weather forecasting and protective measures. Furthermore, the
applicability of this method to other stations within the Chinese
Meridian Project II (e.g., Mingantu Spectral Radioheliograph and
Daocheng Solar Radio Telescope) enhances the capability of space weather
data fusion and model development. Therefore, this research represents a
substantial contribution to the domain of space weather research,
offering a valuable tool for the detection and classification of SRBs
and thereby improving our ability to predict and mitigate the impacts of
extreme space weather events on Earth's technology and infrastructure.</description>
</item>
<item>
<title> Observation of solar radio burst events from Mars orbit with the Shallow Radar instrument</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A..56G</link>
<description>Context. Multispacecraft and multiwavelength observations of solar
eruptions, such as flares and coronal mass ejections, are essential to
understanding the complex processes behind these events. The study of
solar burst events in the radio frequency spectrum has relied almost
exclusively on data from ground-based observations and a few dedicated
heliophysics missions such as STEREO or Wind. &lt;BR /&gt; Aims: By
reanalysing existing data from the Mars Reconnaissance Orbiter (MRO)
Shallow Radar (SHARAD) instrument, a Martian planetary radar sounder, we
discovered the instrument was also capable of detecting solar radio
bursts and that it was able to do so with unprecedented resolution for a
space-based solar instrument. In this study, we aim to demonstrate the
reliability and value of SHARAD as a new solar radio observatory. &lt;BR /&gt;
Methods: We characterised the sensitivity of the instrument to type III
solar radio bursts through a statistical analysis of correlated
observations using STEREO and Wind as references. Using 38 correlated
detections, we established the conditions under which SHARAD can observe
solar bursts in terms of acquisition geometry. As an example of
scientific application, we also present the first analysis of type III
characteristic times at high resolution beyond 1 AU. &lt;BR /&gt; Results: A
simple logistic model based purely on geometrical acquisition parameters
can predict burst show versus no-show in SHARAD data with an accuracy of
79.2%, demonstrating the reliability of the instrument in detecting
solar bursts and laying the foundation for using SHARAD as a solar radio
observatory. The extremely high resolution of the instrument, both in
temporal and frequency directions; its bandwidth; and its position in
the Solar System enable SHARAD to make significant contributions to
heliophysics. Notably, it could provide data on plasma processes on the
site of the burst generation and along the propagation path of
associated fast electron beams.</description>
</item>
<item>
<title> Efficiency of solar microflares in accelerating electrons when rooted in a sunspot</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A..41S</link>
<description>Context. The spectral shape of the X-ray emission in solar flares varies
with the event size, with small flares generally exhibiting softer
spectra than large events, indicative of a relatively lower number of
accelerated electrons at higher energies. &lt;BR /&gt; Aims: We investigate
two microflares of GOES classes A9 and C1 (after background subtraction)
observed by STIX onboard Solar Orbiter with exceptionally strong
nonthermal emission. We complement the hard X-ray imaging and spectral
analysis by STIX with co-temporal observations in the (E)UV and visual
range by AIA and HMI to investigate what makes these microflares so
efficient in high-energy particle acceleration. &lt;BR /&gt; Methods: We made
a preselection of events in the STIX flare catalog based on the ratio of
the thermal to nonthermal quicklook X-ray emission. The STIX spectrogram
science data were used to perform spectral fitting to identify the non-
thermal and thermal components. The STIX X-ray images were reconstructed
to analyze the spatial distribution of the precipitating electrons and
the hard X-ray emission they produce. The EUV images from SDO/AIA and
SDO/HMI LOS magnetograms were analyzed to better understand the magnetic
environment and the chromospheric and coronal response. For the A9
event, EOVSA microwave observations were available, allowing for image
reconstruction in the radio domain. &lt;BR /&gt; Results: We performed case
studies of two microflares observed by STIX on October 11, 2021 and
November 10, 2022, which showed unusually hard microflare X-ray spectra
with power-law indices of the electron flux distributions of  = (2.98 
0.25) and  = (4.08  0.23), during their non-thermal peaks and photon
energies up to 76 keV and 50 keV, respectively. For both events under
study, we found that one footpoint is located within a sunspot covering
areas with mean magnetic flux densities in excess of 1500 G, suggesting
that the hard electron spectra are caused by the strong magnetic fields
the flare loops are rooted in. Additionally, we revisited a previously
published unusually hard RHESSI microflare and found that in this event,
there was also one flare kernel located within a sunspot, which
corroborates the result from the two hard STIX microflares under study
in this work. &lt;BR /&gt; Conclusions: The characteristics of the strong
photospheric magnetic fields inside the sunspot umbrae and penumbrae
where flare loops are rooted play an important role in the generation of
exceptionally hard X-ray spectra in these microflares. &lt;P /&gt;Movies
associated to Figs. 5 and 9 are available at &lt;A href="https://www.aanda.
org/10.1051/0004-6361/202348295/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> Connecting remote and in situ observations of shock-accelerated electrons associated with a coronal mass ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...683A..31M</link>
<description>Context. One of the most prominent sources for energetic particles in
our Solar System are huge eruptions of magnetised plasma from the Sun,
known as coronal mass ejections (CMEs), which usually drive shocks that
accelerate charged particles up to relativistic energies. In particular,
energetic electron beams can generate radio bursts through the plasma
emission mechanism, for example, type II and accompanying herringbone
bursts. &lt;BR /&gt; Aims: In this work, we investigate the acceleration
location, escape, and propagation directions of various electron beams
in the solar corona and compare them to the arrival of electrons at
spacecraft. &lt;BR /&gt; Methods: To track energetic electron beams, we used a
synthesis of remote and direct observations combined with coronal
modeling. Remote observations include ground-based radio observations
from the Nanay Radioheliograph (NRH) combined with space-based extreme-
ultraviolet and white-light observations from Solar Dynamics Observatory
(SDO), Solar Terrestrial Relations Observatory (STEREO), and Solar
Orbiter (SolO). We also used direct observations of energetic electrons
from the STEREO and Wind spacecraft. These observations were then
combined with a three-dimensional (3D) representation of the electron
acceleration locations, including the results of magneto-hydrodynamic
models of the solar corona. This representation was subsequently used to
investigate the origin of electrons observed remotely at the Sun and
their link to in situ electrons. &lt;BR /&gt; Results: We observed a type II
radio burst followed by herringbone bursts that show single-frequency
movement through time in NRH images. The movement of the type II burst
and herringbone radio sources seems to be influenced by regions in the
corona where the CME is more capable of driving a shock. We found two
clear distinct regions where electrons are accelerated in the low corona
and we found spectral differences between the radio emission generated
in these regions. We also found similar inferred injection times of
near-relativistic electrons at spacecraft to the emission time of the
type II and herringbone bursts. However, only the herringbone bursts
propagate in a direction where the shock encounters open magnetic field
lines that are likely to be magnetically connected to the same
spacecraft. &lt;BR /&gt; Conclusions: Our results indicate that if the in situ
electrons are indeed shock-accelerated, the most likely origin of the in
situ electrons arriving first is located near the acceleration site of
herringbone electrons. This is the only region during the early
evolution of the shock where there is clear evidence of electron
acceleration and an intersection of the shock with open field lines,
which can be directly connected to the observing spacecraft. &lt;P /&gt;Movies
are available at &lt;A href="https://www.aanda.org/10.1051/0004-6361/202347
873/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> The Non-Thermal Radio Emissions of the Solar Transition Region and the Proposal of an Observational Regime</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Univ...10...82T</link>
<description>The transition region is a very thin but most peculiar layer in the
solar atmosphere located between the solar chromosphere and the corona.
It is a key region for understanding coronal heating, solar eruption
triggers, and the origin of solar winds. Here, almost all physical
parameters (density, temperature, and magnetic fields) have the maximum
gradient. Therefore, this region should be highly dynamic, including
fast energy releasing and transporting, plasma heating, and particle
accelerating. The physical processes can be categorized into two
classes: thermal and non-thermal processes. Thermal processes can be
observed at ultraviolet (UV) and extreme ultraviolet (EUV) wavelengths
via multi-wavelength images. Non-thermal processes accelerate non-
thermal electrons and produce radio emissions via the gyrosynchrotron
mechanism resulting from the interaction between the non-thermal
electrons and magnetic fields. The frequency range spans from several
GHz to beyond 100 GHz, in great number of bursts with narrowband,
millisecond lifetime, rapid frequency drifting rates, and being referred
to as transition region small-scale microwave bursts (TR-SMBs). This
work proposes a new type of Solar Ultra-wide Broadband Millimeter-wave
Spectrometer (SUBMS) that can be used to observe TR-SMBs. From SUBMS
observations, we can derive rich dynamic information about the
transition region, such as information about non-thermal energy release
and propagation, the flows of plasma and energetic particles, the
magnetic fields and their variations, the generation and transportation
of various waves, and the formation and evolution of the source regions
of solar eruptions. Such an instrument can actually detect the non-
thermal signals in the transition region during no flare as well as the
eruptive high-energy processes during solar flares.</description>
</item>
<item>
<title> Quantifying chaos and randomness in magnetar bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2024MNRAS.528L.133Y</link>
<description>In this study, we explore the dynamical stability of magnetar bursts
within the context of the chaos-randomness phase space for the first
time, aiming to uncover unique behaviours compared to various
astrophysical transients, including fast radio bursts (FRBs). We analyse
burst energy time series data from active magnetar sources SGR
J1550-5418 and SGR J1935+2154, focusing on burst arrival time and energy
differences between consecutive events. We find a distinct separation in
the time domain, where magnetar bursts exhibit significantly lower
randomness compared to FRBs, solar flares, and earthquakes, with a
slightly higher degree of chaos. In the energy domain, magnetar bursts
exhibit a broad consistency with other phenomena, primarily due to the
wide distribution of chaos-randomness observed across different bursts
and sources. Intriguingly, contrary to expectations from the FRB-
magnetar connection, the arrival time patterns of magnetar bursts in our
analysis do not exhibit significant proximity to repeating FRBs in the
chaos-randomness plane. This finding may challenge the hypothesis that
FRBs are associated with typical magnetar bursts but indirectly supports
the evidence that FRBs may primarily be linked to special magnetar
bursts like peculiar X-ray bursts from SGR J1935+2154 observed
simultaneously with Galactic FRB 200428.</description>
</item>
<item>
<title> Experiments with a Three-Element Radio Interferometer in 12 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JKAS...57...25H</link>
<description>In order to attract students to the radio universe, we have constructed
a three-element radio interferometer in the National Youth Space Center,
Goheung, Korea. It consists of three 1.8 m off-axis parabola antennas
with driving systems, sideband separation receivers operating in 12 GHz,
a narrow band digitizer, and correlation software. We have used as many
commercial products as possible to reduce development costs. The maximum
separation of 20 m gives an angular resolution of ~4', and the shortest
baseline of 3.8 m prevents a serious missing flux. Fringes are detected
for several radio sources, including the sun and Cas A. After a rough
relative calibration, we have derived visibilities for the sun, whose
amplitudes are decreasing for longer baselines. We have made a solar
image using the visibility amplitudes and closure phases, referring to
the 17 GHz image by Nobeyama Radioheliograph. Developing a flexible
real-time correlator seems most crucial if this kind of the system is to
be used for more rigorous scientific studies.</description>
</item>
<item>
<title> Reconstruction of global ionospheric TEC maps from IRI-2020 model based on deep learning method</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JGeod..98...10G</link>
<description>The Total Electron Content (TEC) computed from ionospheric models is a
widely used parameter for characterizing the morphological structure of
the ionosphere. The global TEC maps from empirical models, like the
International Reference Ionosphere (IRI) model, have limited accuracy
compared to those calculated by dual-frequency measurements from the
global navigation satellite systems (GNSS). We have developed a
reconstructed IRI TEC model for generating high-precision global TEC
maps based on a deep learning method. For this, we have collected 48,204
pairs of global TEC maps from the IRI-2020 model and Global Ionosphere
Maps (GIM) model with 2-h time resolution from 2009 to 2019 covering the
whole solar cycle 24. The daily solar radio flux (F&lt;SUB&gt;10.7&lt;/SUB&gt;),
sunspot number (SSN), Dst, and Kp indices are also introduced as input
features to train the model. We have investigated the optimum
combination of the input parameters for the reconstructed TEC model and
compared the performance of the model during the years with high and low
solar activity levels. Results show that the reconstructed TEC model
with F&lt;SUB&gt;10.7&lt;/SUB&gt; and Kp features has a better performance compared
to that considering all solar and geomagnetic indices. The global TEC
maps predicted from our model are much more consistent with the
corresponding TEC maps from the GIM model than those from the IRI-2020
model. Especially, the large-scale equatorial ionospheric anomaly (EIA)
crests and the pronounced enhancement of TEC are well predicted by the
reconstructed TEC model. From statistical metrics, the accuracy of the
reconstructed TEC model increased by 40.8% during the high solar
activity year 2015 and 43.0% during the low solar activity year 2018
compared with the IRI-2020 model. The prediction performance of the
reconstructed TEC model also shows better accuracy during the storm
periods.</description>
</item>
<item>
<title> Dependence of Annual Asymmetry in NmF2 on Local Time</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ge&amp;Ae..64...77S</link>
<description>Based on the global empirical model of the median of the critical
frequency of the F2 layer (SDMF2), the properties of diurnal variations
in the annual asymmetry in the maximal concentration NmF2 of the F2
layer for different values of the solar activity index F are analyzed.
The AI index characterizing the relative difference in NmF2 averaged
over all latitudes and longitudes between January and July at a given
local time is used as a parameter of this asymmetry. It is found that a
semidiurnal mode prevails in the diurnal variations in the AI index with
maxima at the daytime and nighttime hours. The daytime maximum of the AI
index hardly depends at all on the solar activity level. The nighttime
AI maximum decreases with an increase in solar activity. The daytime and
nighttime maxima in AI almost coincide by the amplitude when AI = 1617%
for low solar activity. The difference in the solar radio emission flux
between January and July due to the ellipticity of Earth's orbit
relative to the Sun contributes substantially into the AI index at all
hours of the day. On average, it is 34% and could reach 5% for low
solar activity during the nighttime hours. The difference in the AI
index for low and high solar activity according to the International
Reference Ionosphere model IRI (with the URSI and even more with the
CCIR coefficients) is overestimated with respect to the SDMF2 model at
almost all hours of the day, apparently due to limited amount of the
experimental data used to obtain the CCIR and URSI coefficients,
especially over oceans.</description>
</item>
<item>
<title> Predicting the Arrival Time of an Interplanetary Shock Based on DSRT Spectrum Observations for the Corresponding Type II Radio Burst and a Blast Wave Theory</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...962..178L</link>
<description>Since fast head-on coronal mass ejections and their associated shocks
represent potential hazards to the space environment of the Earth and
even other planets, forecasting the arrival time of the corresponding
interplanetary shock is a priority in space weather research and
prediction. Based on the radio spectrum observations of the 16-element
array of the Daocheng Solar Radio Telescope (DSRT), the flagship
instrument of the Meridian Project of China, during its construction,
this study determines the initial shock speed of a type II solar radio
burst on 2022 April 17 from its drifting speed in the spectrum. Assuming
that the shock travels at a steady speed during the piston-driven phase
(determined from the X-ray flux of the associated flare) and then
propagates through interplanetary space as a blast wave, we estimate the
propagation and arrival time of the corresponding shock at the orbit of
the Solar Terrestrial Relations Observatory-A (STEREO-A). The prediction
shows that the shock will reach STEREO-A at 14:31:57 UT on 2022 April
19. The STEREO-A satellite detected an interplanetary shock at 13:52:12
UT on the same day. The discrepancy between the predicted and observed
arrival time of the shock is only 0.66 hr. The purpose of this paper is
to establish a general method for predicting the shock's propagation and
arrival time from this example, which will be utilized to predict more
events in the future based on the observations of ground-based solar
radio spectrometers or telescopes like DSRT.</description>
</item>
<item>
<title> Implications for an Independent Small-scale Dynamo</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...961L..46C</link>
<description>Clette recently showed that F &lt;SUB&gt;10.7&lt;/SUB&gt; systematically approaches
a quiet Sun daily value of 67 solar flux units (sfu) at solar minima as
the number of spotless days on the Sun increases. Previously, a floor of
2.8 nT had been proposed for the solar wind (SW) magnetic field
strength (B). F &lt;SUB&gt;10.7&lt;/SUB&gt;, which closely tracks the Sun's unsigned
photospheric magnetic flux, and SW B exhibit different relationships to
their floors at 11 yr solar minima during the last 50 yr. While F
&lt;SUB&gt;10.7&lt;/SUB&gt; approaches 67 sfu at each minimum, the corresponding SW
B is offset above 2.8 nT by an amount approximately proportional to the
solar polar field strengthwhich varied by a factor of 2.5 during this
interval. This difference is substantiated by 130 yr of reconstructed F
&lt;SUB&gt;10.7&lt;/SUB&gt; (via the range of the diurnal variation of the East-
component (rY) of the geomagnetic field) and SW B (based on the
interdiurnal variability geomagnetic activity index). For the last 60
yr, the contribution of the slow SW to SW B has exhibited a floor-like
behavior at 2 nT, in contrast to the contributions of coronal mass
ejections and high-speed streams that vary with the solar cycle. These
observations, as well as recent SW studies based on Parker Solar Probe
and Solar Dynamics Observatory data, suggest that (1) the Sun has a
small-scale turbulent dynamo that is independent of the 11 yr sunspot
cycle; and (2) the small-scale magnetic fields generated by this
nonvarying turbulent dynamo maintain a constant open flux carried to the
heliosphere by the Sun's floor-like slow SW.</description>
</item>
<item>
<title> Adiabatic Spectrum of Radio Emission of Plasma Clouds, Emitted by the Sun During Solar Flares, and Inhomogeneities of the Spectrum of Radio Emission of Clouds</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ARep...68..183D</link>
<description>It is known that so-called solar flares systematically occur in the area
of sunspots. They are accompanied by radiation in almost all frequency
ranges and sometimes by the emission of hot plasma. Observations on the
RATAN-600 radio telescope have shown that the radio emission spectrum of
plasma clouds heated to values of the order of 10&lt;SUP&gt;6&lt;/SUP&gt; K erupted
from the solar flare region turned out to be adiabatic. The high
correlation of the inhomogeneities of the radio emission spectra of
active formation over a group of sunspots indicates the stable presence
of recombination radio lines in the radiation of active formation.
However, the radio emission spectra of hot plasma clouds ejected from
the region of solar flares occurring in this group of spots do not show
any correlation.</description>
</item>
<item>
<title> Radio signatures and in-situ observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2024PhDT.........9T</link>
<description>Coronal Mass Ejections (CMEs) are large-scale releases of hot plasma, to
which the magnetic field is frozen-in. If the CMEs are faster than the
local magnetosonic velocity in the solar wind, they create shock waves
as they travel through the corona and Interplanetary (IP) space. Shock
waves driven by CMEs can accelerate Solar Energetic Particles (SEPs).
Both phenomena involve the acceleration of electrons, which can be
observed as electromagnetic radiation and plasma radiation. This
doctoral thesis presents analyses of the presence and propagation of
accelerated electrons in the IP medium. By utilizing the observations of
multiple science satellites, such as STEREO-A, STEREO-B, and Wind, we
get a comprehensive picture of the accelerated particles and solar radio
bursts, at various wavelengths. We can use this information to determine
the origin of the eruptions, their directivity, and connections to other
solar events. In particular, the role of shock waves in the acceleration
of relativistic electrons is the subject of this research. Earlier
studies have already confirmed the role of shock waves in the
acceleration of electrons to keV energies using radio bursts, but for
the higher energies, the research is still in progress. &lt;P /&gt;As a result
of observations by many space instruments we now have a 3D view of the
Sun, particularly in the analysis of type IV radio bursts in multi-
spacecraft radio dynamic spectra. The directivity of radio bursts, i.e.,
being seen only toward a certain direction, can be explained either by
absorption in the surrounding medium or by obstruction of dense plasma
region, even by the solar disk itself. The presence of dense plasma
regions like solar streamers, in directions where no radiation is
visible, strengthens this conclusion. Type II radio bursts can be
associated with the interaction of streamers and shock waves. Our
analysis of three separate type IV radio bursts revealed that their
radiation was not visible toward directions where type II radio bursts
were observed. The eruptions were generated by the same active region on
three different days, and the location of the eruption region on the Sun
changed from the disk center to the solar limb. The directivity of the
type IV radio bursts could therefore be explained as absorption in the
type II burst regions, as the shock fronts contain higher-density
plasma. &lt;P /&gt;In the study of isolated type II radio bursts, i.e., when
separated from other bursts in time and also in frequency, we found that
contrary to the previous studies, the majority of these radio bursts
were associated with shocks that were created near the CME leading
fronts. The analysis suggests the necessity of special coronal
conditions, to form this subgroup of low-frequency type II radio bursts.
&lt;P /&gt;The creation of relativistic electrons in IP shocks led to the
investigation of whether these shocks can continue to accelerate
electrons up to one Astronomical Unit (AU). Using in-situ observations
of the electron flux, SEP events, and associated Energetic Storm
Particle (ESP) occurrences, we identified nine cases observed by High
Energy Telescope (HET) onboard STEREO where MeV electrons showed a
significant increase associated with shocks driven by fast speed
Interplanetary CMEs (ICMEs). We also found that such events were rare at
a distance of 1 AU. The research suggests the necessity to make
observations with satellites orbiting closer to the Sun, such as the
Parker Solar Probe and Solar Orbiter, so that we can find out how
electrons are accelerated in IP shocks. Finally, in-situ observations
show clear signatures of local acceleration of electrons during the
passage of the shock wave or the sheath region of the ICME during the
ESP event.</description>
</item>
<item>
<title> Characterization and performance modeling of non-imaging solar X-ray spectrometers and their use in analyzing solar eruptions</title>
<link>https://ui.adsabs.harvard.edu/abs/2024PhDT.........7L</link>
<description>The Sun, besides being by far the most important source of energy for
all life on the Earth, also exhibits various forms of intense magnetic
activity. The most spectacular are the eruptive phenomena such as solar
flares and coronal mass ejections (CMEs). Solar flares are abrupt
localized explosions of energy, where increased radiation is unleashed
throughout the whole electromagnetic spectrum from radio to gamma-rays,
while CMEs are huge eruptions of plasma and magnetic field from the
solar corona. Flares and CMEs can occur independently, but they often
occur simultaneously and originate from the destabilization of the same
magnetic structure in the solar atmosphere. These phenomena are also the
primary drivers of space weather within the heliosphere. The increased
X-ray and EUV radiation during solar flares can cause ionization in the
upper atmosphere, which can disrupt long range radio communications and
the geomagnetic storms caused by interactions between CMEs and the
Earth's magnetic field can be very damaging to electrical grid systems
and pipeline networks on the ground. Solar flares and CMEs are also
often accompanied by solar energetic particle events, which can be
damaging to the satellite electronics and pose a radiation hazard in
space and on-board aircraft at cruising altitude. &lt;P /&gt;Solar eruptions
originate from the magnetic structures in the Sun's hot and tenuous
corona. The electromagnetic emission of the coronal plasma is mainly in
EUV and soft X-ray bands, which are very efficiently absorbed by the
Earth's atmosphere. Monitoring of solar eruptions must therefore be
performed in space using satellite based EUV and X-ray observatories. In
this thesis I present an overview about the missions and instrumentation
that are currently or have been previously used for studying and
monitoring the solar and stellar coronae. The emphasis is on non-imaging
X-ray spectrometers based on solid state detectors that utilize high-
purity silicon photodiodes. These instruments are capable of monitoring
the whole solar corona simultaneously in a wide dynamic range of X-ray
fluxes, from the levels of quiescent Sun to strong X-class solar flares
with high energy resolution of &lt;200 eV at 6 keV. &lt;P /&gt;Two non-imaging
solar X-ray spectrometers based on high-purity Si detectors are
described in detail. They are the X-ray detection system of the Solar
Intensity X-ray and particle Spectrometer (SIXS) on-board BepiColombo
mission to Mercury and the X-ray Flux Monitor for CubeSats (XFM-CS),
which has been used in the successful in-orbit demonstration of XFM
technology on-board the SUNSTORM-1 CubeSat at low Earth orbit. The
basics of operation of these instruments, their detectors and readout
electronics are described. I also present a performance model for
modeling the sensitivity, energy resolution and background of non-
imaging solid state X-ray spectrometers, which was used to optimize the
designs of SIXS and XFM-CS detectors. The characterization of SIXS and
XFM-CS instruments and evaluation of their scientific performance is
presented in detail. Included are procedures for both ground and in-
flight characterization as well as the descriptions of the science data
processing pipelines that are used to calibrate the raw solar X-ray
data. The results of cross calibration of SIXS and XFM-CS instruments
against the GOES X-ray sensors are also presented. &lt;P /&gt;The use of high-
resolution spectral data of solar X-rays in space weather forecasting is
discussed. Time resolved spectroscopic analysis was performed to a
sample of 16 M and X class solar flares observed with XFM-CS in an
effort to identify spectral features associated with CMEs accompanying
the flares. The results were compared against the simultaneous EUV
images from the Solar Dynamics Observatory and coronagraph images from
SOHO and STEREO-A. The results show that associated CMEs reduce the
plasma temperature and density inside the flaring magnetic structures,
which can be used for early detection of CMEs as well as for rough
estimation of their mass when combined with independent observations of
the flaring magnetic structures. It was also tentatively found that
flare associated CMEs delay the stabilization of the elemental
fractionation of the plasma to the normal levels in closed loop corona
during the decay phases of flares and that the strength of this effect
appears to correlate with the CME lift-off time. The additional
information about the CME properties complements the information that
can be derived from coronagraph imaging and can be useful in improving
our understanding of the processes responsible for flares and CMEs, and
can also improve the timeliness and accuracy of space weather forecasts.</description>
</item>
<item>
<title> Interaction of global electron content with the Sun and solar wind during intense geomagnetic storms</title>
<link>https://ui.adsabs.harvard.edu/abs/2024P&amp;SS..24005830G</link>
<description>Assessment of solar and solar wind parameters driving the ionosphere
model is essential for prediction of the ionospheric weather. In the
present paper impact of the different solar, interplanetary and
geomagnetic parameters on the global electron content (GEC) during
intense space weather storms is investigated. Hourly GEC values are
calculated from JPL global maps of total electron content GIM-TEC from
1995 to 2023. The sample comprises 90 intense storms from 1995 to 2023
associated with monthly peak of the weighted accumulation of the
geomagnetic Apo(, t) index exceeding 90 nT. The 27 day weighted
accumulation of the solar sunspot numbers SSN2(), solar radio flux
F10.7(), the solar hydrogen emission Lyman_() and the composite
magnesium MgII() indices are explored as precursors of GEC
enhancements. As distinct from the positive ionosphere storm, the solar
wind speed Vsw, the solar wind electric field Ey, merging electric field
Em and Apo(, t) indices proved to be effective as potential drivers of
the negative GEC depletion. The positive and negative dGEC deviations
from hourly GEC are produced by subtracting a quiet reference GECav
averaged during 24h prior the storm normalized by GECav. The hourly
storm profiles Vsw(t), Em(t), Ey(t), Apo(, t), Dst(t), GEC(t) and
dGEC(t) were reduced by method of superposed epochs. The zero epoch
t&lt;SUB&gt;0&lt;/SUB&gt; = 0 was taken at the peak Apo*(, t&lt;SUB&gt;0&lt;/SUB&gt;) and the
storm time lasted for 48h from -12h prior t&lt;SUB&gt;0&lt;/SUB&gt; and 35h
afterwards. The best correlation of the positive storm dGECp amplitude
is obtained with MgII() and the negative storm dGECn with
E&lt;SUB&gt;m&lt;/SUB&gt;* and Apo*(, t&lt;SUB&gt;0&lt;/SUB&gt;) which are used to derive
characteristics of five key points of storm-time dGEC(t) model: 1 -
onset of the storm profile t&lt;SUB&gt;1&lt;/SUB&gt; = t(dGECp); 2 - the amplitude
dGECp&lt;SUB&gt;max&lt;/SUB&gt; and its time t&lt;SUB&gt;2&lt;/SUB&gt;(dGECp&lt;SUB&gt;max&lt;/SUB&gt;); 3 -
the time of transition t&lt;SUB&gt;3&lt;/SUB&gt;(dGEC = 0) from the positive to
negative () GEC storm; 4 - minimum negative disturbance
dGECn&lt;SUB&gt;min&lt;/SUB&gt; and its time t&lt;SUB&gt;4&lt;/SUB&gt;(dGECn&lt;SUB&gt;min&lt;/SUB&gt;), 5 -
the end of the storm profile t&lt;SUB&gt;5&lt;/SUB&gt;(dGECn). Analytical model of
dGEC(t) is derived with Epstein step functions fitting 5 key points.
Deviations dGEC(t) are inverted to GEC(t) using quiet reference pre-
storm GECav. The model is validated for three intense storms on 26-28
February, 23-25 March and 23-25 April 2023. The results show improvement
of dGEC forecast with RMS error reduced from 45 to 80% compared to
results produced by the international reference ionosphere-plasmasphere
model IRI-Plas.</description>
</item>
<item>
<title> Evolution and Flare Activity of Carrington-Class Solar Active Region NOAA 13664 and its Impact on the Earth</title>
<link>https://ui.adsabs.harvard.edu/abs/2024OAP....37..112K</link>
<description>We have analyzed the temporal and spatial evolution and the flare
activity of the active region (AR) NOAA 13664 and its impact on the
Earth. The large group of sunspots that formed it definitely belonged to
the Carrington class. The region appeared in the southern hemisphere of
the solar disk on 2024 May 1. The number of sunspots was growing rapidly
and its area increased from 40 to 2400 millionths of the solar
hemisphere. The AR had a complex multipolar configuration of the
magnetic field beginning on May 7. On May 8, solar flares of intensity
X1.0, M8.7 and M9.9 took place in it, which caused coronal mass
ejections (CMEs). These CMEs reached the Earth on May 10, causing strong
and extreme geomagnetic storms with bright and very long-lasting
auroras. The event was classified as a G5 geomagnetic storm, making it
the most intense storm since 2003. On May 9-11, flares of intensity
X2.3, X1.5, X4, and X5.8 occurred, each of which caused a CME. The
radiation from the X5.8 flare caused a deep shortwave radio blackout
over the Pacific Ocean. On May 14, an X8.7-class flare occurred on the
western limb of the Sun, the most powerful in solar cycle 25 at that
time. The CME that formed caused a short-wave radio blackout over
America. &lt;P /&gt;On May 9 during observations at the Ernest Gurtovenko
solar horizontal telescope of the Main Astronomical Observatory of the
National Academy of Sciences of Ukraine the X2.3 flare spectrograms in
its main phase were obtained. &lt;P /&gt;The active region 13664 passed beyond
the solar disk and returned on May 29. It has been renumbered as NOAA
13697. On May 31 and June 1 AR produced three X-flares: X1.1, X1.4, and
X1.0. Each of them formed CMEs, which reduced the power of shortwave
transmissions at all frequencies below 30 MHz. Radiation from M9.8-class
flare on June 8 ionized the upper part of the Earth's atmosphere,
causing a deep shortwave radio blackout in the western Pacific Ocean. &lt;P
/&gt;On June 24 AR13664 returned again. This was its 3rd trip across the
solar disk. It was renamed as NOAA 13723. Although the sunspot region
was already fragmented to a fraction of its former size, its magnetic
component continued to produce powerful solar flares. On June 23,
M9.3-class flare occurred in AR, CME from which caused a moderate
shortwave radio blackout in Western Europe and Africa. &lt;P /&gt;In total,
AR13664 produced 198 C-class, 87 M-class, and 17 X-class flares during
its three passes across the Sun's disk. &lt;P /&gt;By studying in detail the
evolution of this hyperactive region NOAA 13664 and its impact on Earth,
we are improving our ability to predict solar activity and warn of the
extreme space weather events it causes.</description>
</item>
<item>
<title> Diagnostics of Solar Proton Events and Coronal Shock Waves by the Parameters of Solar Radio Bursts of Type II and IV</title>
<link>https://ui.adsabs.harvard.edu/abs/2024OAP....37..107I</link>
<description>This paper presents the results of a study of the relationship between
solar cosmic rays (SCR) and coronal shock waves (CSW) with the
parameters of solar microwave continuum radio bursts of type IV
(-bursts), as well as with the parameters of type II radio bursts. A
total of 349 solar proton events (SPE) were analyzed for the period from
03-02-1986 to 12-02-2018. For the analysis, we used original records of
solar radio emission at 8 fixed frequencies in the range of 245-15400
MHz based on data from the Radio Solar Telescope Network (RSTN),
original records of dynamic spectra from the SRS (Solar Radio
Spectrograph) in the range of 25-180 MHz, tabular data for the velocity
of coronal shock waves, as well as original records of the SCR proton
flux intensity with proton energies E&lt;SUB&gt;p&lt;/SUB&gt; in the range of &gt;1-100
MeV based on data from the GOES series devices. &lt;P /&gt;It has been
previously shown that for most proton events there is a strong
relationship between the SCR proton flux and the parameters of type IV
continuum microwave bursts, which indicates a dominant role of the SCR
acceleration process in the flare region. However, as a result of recent
detailed studies of the fine structure of type II radio bursts, a strong
relationship was found between the intensity of the mid-relativistic SCR
proton flux and certain parameters of type II radio bursts in the 25-180
MHz range. The presence of a strong relationship between the SCR proton
flux and the parameters of type II radio bursts indicates an important
role of SCR proton acceleration at the fronts of coronal shock waves. A
fairly strong relationship was also found between the velocity of
coronal shock waves and the parameters of type IV microwave bursts,
which definitely indicates that coronal shock waves are associated with
solar flares.</description>
</item>
<item>
<title> Detection of long-lasting aurora-like radio emission above a sunspot</title>
<link>https://ui.adsabs.harvard.edu/abs/2024NatAs...8...50Y</link>
<description>Auroral radio emissions in planetary magnetospheres typically feature
highly polarized, intense radio bursts, usually attributed to electron
cyclotron maser emission from energetic electrons in the planetary polar
region that features a converging magnetic field. Similar bursts have
been observed in magnetically active low-mass stars and brown dwarfs,
often prompting analogous interpretations. Here we report observations
of long-lasting solar radio bursts with high brightness temperature,
wide bandwidth and high circular polarization fraction akin to these
auroral and exo-auroral radio emissions, albeit two to three orders of
magnitude weaker than those on certain low-mass stars. Spatially,
spectrally and temporally resolved analysis suggests that the source is
located above a sunspot where a strong, converging magnetic field is
present. The source morphology and frequency dispersion are consistent
with electron cyclotron maser emission due to precipitating energetic
electrons produced by recurring nearby flares. Our findings offer new
insights into the origin of such intense solar radio bursts and may
provide an alternative explanation for aurora-like radio emissions on
other flare stars with large starspots.</description>
</item>
<item>
<title> Solar radio bursts impact on the International GNSS Service Network during Solar Cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JSWSC..14...32F</link>
<description>Solar radio bursts (SRB) are a known source of noise for Global
Navigation Satellite Systems (GNSS) such as GPS or Galileo. They can
degrade the carrier-to-noise ratio of satellite signals, thereby
diminishing system performance and, in severe cases, causing total
service outages. Although a small amount of particularly intense events
have already been studied in detail, the commonness and intensity of
SRBs that could potentially impair GNSS performance remain uncertain.
This study broadens the scope beyond merely extreme SRBs, studying the
impact of SRBs on GNSS throughout Solar Cycle 24. Solar 1.4 GHz
observations from the Radio Solar Telescope Network are used to find the
20 most intense SRBs at that frequency. The impact of each SRB is then
evaluated in terms of GNSS signal strength decrease, reduction in the
number of available satellites, and precision degradation. The results
show that at the GPS L1 frequency only one event presented extended
service degradation, while at the L2 frequency, minimum operational
requirements were not met by at least one station during seven of the
SRBs. Only a modest correlation between performance degradation and SRB
intensity is found. In particular, it is reported how some mild SRBs
affected satellite signals while others almost ten times more intense
went unnoticed. The fundamental role that the SRB circular polarization
plays in these discrepancies is shown with new 1.4 GHz circular
polarization observations from the SMOS satellite. The different
responses of GNSS receivers to SRBs depending on the receiver
manufacturer are also explored.</description>
</item>
<item>
<title> Ionospheric Response to Solar EUV Radiation Variations Using GOLD Observations and the CTIPe Model</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JGRA..12930887V</link>
<description>To understand the global response of thermospheric-ionospheric (TI)
parameters to variations in solar irradiance measurements from the
Global-Scale Observations of the Limb and Disk (GOLD) ultraviolet
imaging spectrograph, solar radio flux F10.7, predictions from the
Coupled Thermosphere Ionosphere Plasmasphere electrodynamics (CTIPe)
model, and International Global Navigation Satellite System Service
total electron content maps (TEC) have been used. Various parameters
such as GOLD O/N&lt;SUB&gt;2&lt;/SUB&gt;, O&lt;SUB&gt;2&lt;/SUB&gt;, and the nighttime peak
electron density (Nmax) have been compared with the CTIPe model
simulations. The GOLD observed Nmax shows a number of significant
features including a winter anomaly and an equatorial ionization
anomaly. The comparison with solar proxies showed that the GOLD
Q&lt;SUB&gt;EUV&lt;/SUB&gt; correlates very well with the EUV observations compared
to the F10.7 index. The study also examined the relationship between the
solar proxies and Nmax on different time scales and found that Nmax
responded significantly to Q&lt;SUB&gt;EUV&lt;/SUB&gt; at both medium- and long-term
timescales. Furthermore, a low correlation between Nmax in the
equatorial region and solar proxies was found. A delayed ionospheric TEC
response against solar flux variations within the 27-day solar rotation
was investigated. This ionospheric delay of TEC with respect to solar
flux was observed to be less than 1 day, which was reproduced in model
simulations. The current study has shown that the GOLD observations can
be used to investigate the delayed ionospheric response and to gain a
better understanding of the influence of solar activity on the TI
system.</description>
</item>
<item>
<title> Initial results from multi-beam observations of pulsars and solar transient with the digital beamformer for the Gauribidanur pulsar system</title>
<link>https://ui.adsabs.harvard.edu/abs/2024JATIS..10a4001B</link>
<description>Recently a prototype for pulsar observations at low radio frequencies
(RFs) (&lt;100 MHz) using log-periodic dipole antennas (LPDAs) in the
Gauribidanur Radio Observatory (77&lt;SUP&gt;&lt;/SUP&gt;E14&lt;SUP&gt;&lt;/SUP&gt;N) near
Bangalore, India, was commissioned. The aforementioned system is
currently being augmented (i) to directly digitize the RF signals from
the individual antennas and (ii) with a digital beamformer to
simultaneously observe different regions of the sky present within the
primary "beam" of the LPDA used in the array. Our initial results
indicate that co-temporal observations of a known pulsar along with the
Sun using two different beams could be used to calibrate the dynamic
spectrum of the solar radio transients. This is important because the
calibration of the latter in observations with the conventional solar
radio spectrographs is difficult.</description>
</item>
<item>
<title> Design and FPGA Implementation of an Adaptive Narrowband Interference Suppression Filter</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ITIM...7372219Z</link>
<description>The sensitivity and spectral performance of radio telescopes are
increasingly affected by deteriorating electromagnetic environments.
Therefore, developing a real-time interference elimination algorithm is
urgent for future radio observations. In this article, we developed an
improved interference suppression filter algorithm named the improved
least mean square (IMLMS). Unlike traditional algorithms, the IMLMS
algorithm uses an exponential function varying with error to adjust the
step size. The input signal is normalized according to its own average
energy so that it can not only satisfy the slow change in the step size
at an error near zero but also reduce the influence of the input signal
size on the algorithm. The improvement degree of the target interference
ratio and the interference suppression degree are used to evaluate the
performance of the IMLMS filter. Compared with traditional algorithms,
the IMLMS algorithm has a better target interference ratio and
interference suppression. The IMLMS filter is implemented in a Xilinx
UltraScale KU115 FPGA, and the design of the IMLMS filter is optimized
to meet the real-time observation requirements of a radio telescope with
a 6-m aperture antenna at the Chashan observatory. The timing
performance reaches 187.5 MHz. Compared to existing design and
implementation methods, the IMLMS adaptive filter has high timing
performance and solves the problem of interference suppression that
requires high timing performance in fields such as radar and solar
radio. Th e IMLMS filter is applied to the Chashan radio telescope for
real-time observation, which further verifies the practicability of the
IMLMS algorithm.</description>
</item>
<item>
<title> Triple Voltage Threshold Approximate Cache for Energy Harvesting Nonvolatile Processors</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ITCAD..43.4546H</link>
<description>Energy harvesting is considered to be a substitute for batteries in many
modern systems. Systems based on energy harvesting receive environmental
energies from sources, such as sun, radio frequency, wind, vibration,
etc, and convert them to electrical energy to be used by the capacitor
of the system or feed the cyber-physical system (CPS) system directly.
Despite its advantages, energy harvesting comes with some limitations,
such as the instability of the received energy, which means that the
energy may not be received for a moment due to environmental conditions
during energy harvesting. Therefore, due to not receiving enough energy,
the system function may face problems, which can lead to system shutdown
and data loss. To prevent program execution interruption caused by
frequent power interruptions in systems based on energy harvesting,
these systems use nonvolatile processor (NVP). Saving the state in the
NVP is done through nonvolatile registers and memories that can hold the
contents until the power is restored. However, systems based on energy
harvesting and NVPs also have challenges, such as frequent backups'
energy consumption, slow program forward progress, and loss of data. In
this article, we propose TVTAC, a framework for energy harvesting-based
NVP CPS systems. TVTAC modifies conventional NVP's cache architecture to
efficiently work with newly introduced operational mode to prevent
unnecessary backup operations. Furthermore, TVTAC is equipped with an
NVP's specific approximation unit that controls the approximation knobs
during the approximate data cache accesses in order to save more energy.
The simulation results show that TVTAC improves forward progress by 28%
in the best case and 12% on average, compared to similar methods. From
an energy consumption perspective, TVTAC reduces energy consumption by
43.5% in the best case and 28.5% on average.</description>
</item>
<item>
<title> Weak Solar Radio Bursts from the Solar Wind Acceleration Region Observed by the Parker Solar Probe and Its Probable Emission Mechanism</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...961..136C</link>
<description>The Parker Solar Probe (PSP) provides us with an unprecedentedly close
approach to the observation of the Sun and hence the possibility of
directly understanding the elementary process that occurs on the kinetic
scale of particles' collective interaction in solar coronal plasmas. We
report a type of weak solar radio burst (SRB) that was detected by PSP
when it passed a low-density magnetic channel during its second
encounter phase. These weak SRBs have a low starting frequency of ~20
MHz and a narrow frequency range from a few tens of MHz to a few hundred
kHz. Their dynamic spectra display a strongly evolving feature of the
intermediate relative drift rate decreasing rapidly from above 0.01
s&lt;SUP&gt;-1&lt;/SUP&gt; to below 0.01 s&lt;SUP&gt;-1&lt;/SUP&gt;. Analyses based on common
empirical models of solar coronal plasmas indicate that these weak SRBs
originate from a heliocentric distance of ~1.1-6.1 R &lt;SUB&gt;S&lt;/SUB&gt; (the
solar radius), a typical solar wind acceleration region with a low-
plasma, and that their sources have a typical motion velocity of ~v
&lt;SUB&gt;A&lt;/SUB&gt; (Alfvn velocity) obviously lower than that of the fast
electrons required to effectively excite SRBs. We propose that solitary
kinetic Alfvn waves with kinetic scales could be responsible for the
generation of these small-scale weak SRBs, called solitary wave
radiation.</description>
</item>
<item>
<title> Opening a New Frontier in Solar Physics</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...961...96K</link>
<description>Solar radio emissions provide several unique diagnostics to estimate
different physical parameters of the solar corona, which are otherwise
simply inaccessible. However, imaging the highly dynamic solar coronal
emissions spanning a large range of angular scales at radio wavelengths
is extremely challenging. At gigahertz frequencies, MeerKAT radio
telescope is possibly globally the best-suited instrument at present for
providing high-fidelity spectroscopic snapshot solar images. Here, we
present the first published spectroscopic images of the Sun made using
the observations with MeerKAT in the 880-1670 MHz band. This work
demonstrates the high fidelity of spectroscopic snapshot MeerKAT solar
images through a comparison with simulated radio images at MeerKAT
frequencies. The observed images show extremely good morphological
similarities with the simulated images. Our analysis shows that below
~900 MHz MeerKAT images can recover essentially the entire flux density
from the large angular-scale solar disk. Not surprisingly, at higher
frequencies, the missing flux density can be as large as ~50%. However,
it can potentially be estimated and corrected for. We believe once solar
observation with MeerKAT is commissioned, it will enable a host of novel
studies, open the door to a large unexplored phase space with
significant discovery potential, and also pave the way for solar science
with the upcoming Square Kilometre Array-Mid telescope, of which MeerKAT
is a precursor.</description>
</item>
<item>
<title> Spatial Localization and Correlation with Solar Flare Intensity</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...961...88K</link>
<description>We present a comprehensive study of type III radio bursts and their
association with solar flares of magnitude M1.0 and larger, as observed
by four widely separated spacecraft (Parker Solar Probe, Solar Orbiter,
STEREO-A, and Wind). Our main focus is the introduction and validation
of two methods for localizing radio bursts using the available
multispacecraft data. The first method utilizes intensity fitting with a
circular Gaussian distribution, while the second method is based on the
time arrival of radio bursts. We demonstrate the effectiveness of these
methods through the analysis of a single type III burst event and
compare their results with the traditional radio triangulation
technique. Furthermore, we conduct a statistical study of 17 type III
bursts associated with M- and X-class solar flares in years 2020-2022.
Our findings suggest a possible correlation between solar flare
intensities and longitudes, with east limb flares tending to be weaker
than west limb flares. We also observe a systematic drift of radio burst
longitudes toward the east, potentially explained by a poleward
component of the local density gradient. Our results suggest a strong
correlation between solar flare intensities and radio burst properties,
enhancing our understanding of the relationship between solar flares and
type III radio bursts.</description>
</item>
<item>
<title> High-harmonic Plasma Emission Induced by Electron Beams in Weakly Magnetized Plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...960..111L</link>
<description>Electromagnetic radiation at higher harmonics of the plasma frequency (
~ n  &lt;SUB&gt;pe&lt;/SUB&gt;, n &gt; 2) has been occasionally observed in type II
and type III solar radio bursts, yet the underlying mechanism remains
undetermined. Here we present two-dimensional fully kinetic
electromagnetic particle-in-cell simulations with high spectral
resolution to investigate the beam-driven plasma emission process in
weakly magnetized plasmas of typical coronal conditions. We focused on
the generation mechanisms of high-harmonic emission. We found that a
larger beam velocity (u &lt;SUB&gt; d &lt;/SUB&gt;) favors the generation of the
higher-harmonic emission. The emissions grow later for higher harmonics
and decrease in intensity by ~2 orders of magnitude for each jump of the
harmonic number. The second and third harmonic (H&lt;SUB&gt;2&lt;/SUB&gt; and
H&lt;SUB&gt;3&lt;/SUB&gt;) emissions get closer in intensity with larger u &lt;SUB&gt; d
&lt;/SUB&gt;. We also show that (1) the H&lt;SUB&gt;3&lt;/SUB&gt; emission is mainly
generated via the coalescence of the H&lt;SUB&gt;2&lt;/SUB&gt; emission with the
Langmuir waves, i.e., H&lt;SUB&gt;2&lt;/SUB&gt; + L  H&lt;SUB&gt;3&lt;/SUB&gt;, wherein the
coalescence with the forward-propagating beam-Langmuir wave leads to the
forward-propagating H&lt;SUB&gt;3&lt;/SUB&gt;, and coalescence with the backward-
propagating Langmuir wave leads to the backward-propagating
H&lt;SUB&gt;3&lt;/SUB&gt;; and (2) the H&lt;SUB&gt;4&lt;/SUB&gt; emission mainly arises from the
coalescence of the H&lt;SUB&gt;3&lt;/SUB&gt; emission with the forward-
(backward-)propagating Langmuir wave, in terms of H&lt;SUB&gt;3&lt;/SUB&gt; + L 
H&lt;SUB&gt;4&lt;/SUB&gt;.</description>
</item>
<item>
<title> Enhancing Triangulation of Interplanetary Type III Bursts through Wavevector Correction</title>
<link>https://ui.adsabs.harvard.edu/abs/2024ApJ...960..101K</link>
<description>Interplanetary Type III bursts, generated by relativistic electron beams
at solar flare reconnection sites, are explored through an investigation
of 152 instances observed by the Solar Terrestrial Relations Observatory
mission. This study reveals that the absolute values of the wavevector
deviations from the Sun-spacecraft line are statistically 3.72 and 2.10
larger than predicted by the density model, assuming fundamental and
harmonic emission, respectively. Through Monte Carlo simulations, we
examine the impact of scattering by density inhomogeneities on the
apparent locations of radio emissions in the interplanetary medium. The
findings indicate that relative density fluctuations of 0.40 can account
for the observed angular shift, a conclusion supported by the multiple
flux-tube solar wind model, which confirms the presence of such
magnitude of relative perpendicular density fluctuations in the solar
wind. We propose a wavevector correction that incorporates this effect
to enhance the triangulation of interplanetary Type III bursts,
demonstrating that radio triangulation, with this correction, can
reliably track electron beams in the interplanetary medium.</description>
</item>
<item>
<title> Periodic-chaotic alternating regimes during a fast solar metric-radio pulsation event</title>
<link>https://ui.adsabs.harvard.edu/abs/2024Ap&amp;SS.369....9M</link>
<description>In the magnetically dominated corona, loop-like structures are expected
to undergo pulsating events which are highly structured in time and
classified into different types from strictly periodic to irregular. In
the case of periodic pulsations, they differ in their characteristic
period: from tens of minutes (associated with global large-scale
structure oscillations) to milliseconds (fast oscillations associated
with a small local scale). These pulsations are strongly related to the
basic physical properties of the solar corona and the evolution of
magnetic loop-like structures that make up the entire solar atmosphere.
This contribution describes a real-world scenario where a route to chaos
and reverse processes take place. We examine the dynamic characteristics
of a group of a train of pulsations at metric waveband solar radio
emission as it evolves in time. The associated time series was recorded
with the radio polarimeter of the INAF Trieste Astronomical Observatory,
Basovizza Station on April 17, 2002, with a resolution time of 10 ms.
Possible scenarios and mechanisms for the observed deterministic-chaos
alternating regimes are discussed.</description>
</item>
<item>
<title> A correlation, artificial neural network, and spectral analysis</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..73.1092M</link>
<description>The objective of this study was to examine the relationship between
cosmic rays (CR) and various solar activity parameters, including the
interplanetary magnetic field (B), solar radio emission flux at 10.7 cm
(F10.7), solar wind speed (V), solar wind density (N), solar wind
pressure (P), and the variance of the interplanetary magnetic field
vector (F). The CR data collected from 2007 to 2013 were obtained using
a muon detector situated at King Abdulaziz University (KAAU) in Jeddah,
Saudi Arabia, with a rigidity cutoff of 14.8 GV. To explore the
correlation between the CR data and the selected parameters, three
distinct methods were employed: regression analysis, artificial neural
network (ANN), and power spectral analysis. &lt;P /&gt;Regression analysis
revealed significant positive correlations between CR muons and plasma
pressure (R = 0.1, p &lt; 0.05), as well as solar wind speed (R = 0.1, p &lt;
0.05). On the other hand, negative correlations were observed between
CRs and radio flux (R = 0.75, p &lt; 0.05), as well as interplanetary
magnetic field (R = 0.1, p &lt; 0.05). However, no significant correlations
were found between CRs and plasma density or the variance of the
interplanetary magnetic field vector (p &gt; 0.05). Furthermore,
multivariable correlation analyses were conducted to explore the
relationship between CR muons and the considered parameters, resulting
in only marginal improvement. &lt;P /&gt;For comparison purposes, data from
the King Abdulaziz City for Science and Technology (KACST) muon detector
in Riyadh, Saudi Arabia (with a rigidity cutoff of 14.4 GV), as well as
CR data from Oulu NM (with a rigidity cutoff of 0.3 GV), were utilized
for the same period as the KAAU data. The correlation results indicated
that the relationships between the CR data from the three detectors and
some of the considered parameters were consistent. However, the strength
of the correlations and the magnitudes of the slopes exhibited
variations. &lt;P /&gt;ANN procedures were also employed to compare the
efficiency of neural network analysis in forecasting CR muons based on
solar activity parameters. The Multilayer Perceptron (MLP) Module
trained using the backpropagation learning algorithm was utilized to
build a neural network model and assess its accuracy. The results
indicated that the ANN method provided slightly more accurate
predictions compared to regression analysis. &lt;P /&gt;Finally, Fast Fourier
Transform (FFT) analyses were conducted to examine the presence of
periodicities between the CRs and the variables under consideration. The
analysis revealed several shared periodicities, including cycles
spanning 270-277 days, 146-158 days, 89-95 days, 66-73 days, and 21-31
days.</description>
</item>
<item>
<title> Empirical forecasting models for peak intensities of energetic storm particles at 1 AU</title>
<link>https://ui.adsabs.harvard.edu/abs/2024AdSpR..73.1050A</link>
<description>We have investigated the dependence of the peak intensities of energetic
storm particles (ESPs) on various parameters characterising the coronal
mass ejections (CMEs) and associated phenomena. The aim of this study is
to suggest empirical models for forecasting the peak intensities of ESP
events at 1 AU based on solar and interplanetary (IP) space
observations. &lt;P /&gt;For this study we searched for the associations of
front-side full and partial halo CMEs with linear speeds &gt; 400 km
s&lt;SUP&gt;-1&lt;/SUP&gt;during the years 1996-2015 with IP shocks at 1 AU and ESP
events observed near the time when the shock passes the observer. We
found 88 CME-driven IP shocks associated with ESP events at proton
energy range 5.0-7.2 MeV (nominal energy 6.0 MeV) and 59 shocks at the
energy range 15.1-21.9 MeV (nominal energy 18.2 MeV). At these two
energies 71 % and 68 % of the ESP events were associated with solar
energetic particle (SEP) events, 85 % and 84 % were associated with
decametric-hectometric (DH) type II radio bursts while 67 % and 66 %
were associated with both. &lt;P /&gt;For each CME - shock pair we calculated
the predicted shock transit speed (V&lt;SUB&gt;TR&lt;/SUB&gt;) by using the method
of Belov et al. (2022) and used this as the primary parameter in the
investigation. We performed correlation analyses between the logarithm
of the peak intensities of the ESP events (log&lt;SUB&gt;10&lt;/SUB&gt;
[I&lt;SUB&gt;ESP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt; ]) and the solar parameters related to
the CMEs, solar flares, IP shocks, SEP events, and type II radio bursts.
When using a single explanatory variable, we found best correlation
coefficients for V&lt;SUB&gt;TR&lt;/SUB&gt; (0.68  0.05 and 0.71  0.06), the CME
space speed (V&lt;SUB&gt;CME&lt;/SUB&gt;&lt;SUP&gt;space&lt;/SUP&gt;) (0.59  0.05 and 0.68 
0.07), and the logarithm of SEP peak intensity (log&lt;SUB&gt;10&lt;/SUB&gt;
[I&lt;SUB&gt;SEP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt; ]) (0.55  0.08 and 0.70  0.08) at 6.0
and 18.2 MeV, respectively. Weak to moderate correlations were found for
the logarithm of the soft X-ray flux (log&lt;SUB&gt;10&lt;/SUB&gt; [SXRF]) and the
logarithm of the duration of DH type II radio burst (log&lt;SUB&gt;10&lt;/SUB&gt;
[D&lt;SUB&gt;TII&lt;/SUB&gt; ]). &lt;P /&gt;Using linear combinations of two or more
variables improved the correlations. The best two-variable combination
explaining log&lt;SUB&gt;10&lt;/SUB&gt; [I&lt;SUB&gt;ESP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt; ] was
V&lt;SUB&gt;TR&lt;/SUB&gt; combined with log&lt;SUB&gt;10&lt;/SUB&gt;
[I&lt;SUB&gt;SEP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt; ] and the best three- and four-variable
combinations also included these two parameters. We found two methods
for forecasting ESP peak intensities, one of which can be used for long
lead time and the other for medium lead time forecasting. For long lead
time forecasting V&lt;SUB&gt;TR&lt;/SUB&gt; , V&lt;SUB&gt;CME&lt;/SUB&gt;&lt;SUP&gt;space&lt;/SUP&gt; and
log&lt;SUB&gt;10&lt;/SUB&gt; [SXRF] are used. The correlation coefficients between
the calculated and observed log&lt;SUB&gt;10&lt;/SUB&gt;
[I&lt;SUB&gt;ESP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt; ] were 0.71  0.05 at 6.0 MeV and 0.74 
0.06 at 18.2 MeV. This method only depends on the coronagraph and X-ray
observations at the Sun. For medium lead time forecasting the four
parameters used are V&lt;SUB&gt;TR&lt;/SUB&gt; , log&lt;SUB&gt;10&lt;/SUB&gt;
[I&lt;SUB&gt;SEP&lt;/SUB&gt;&lt;SUP&gt;peak&lt;/SUP&gt;], V&lt;SUB&gt;CME&lt;/SUB&gt;&lt;SUP&gt;space&lt;/SUP&gt; (or
log&lt;SUB&gt;10&lt;/SUB&gt; [SXRF]), and log&lt;SUB&gt;10&lt;/SUB&gt; [D&lt;SUB&gt;TII&lt;/SUB&gt; ]. The
correlation coefficients were 0.80  0.04 at 6.0 MeV and 0.84  0.05 at
18.2 MeV. Coronagraph observations at the Sun and solar energetic
particle and DH type II burst measurements in IP space are required for
this method. The medium lead time forecasting provides an average
warning time of 30  16 h.</description>
</item>
<item>
<title> Deep Learning LSTM-based approaches for 10.7 cm solar radio flux forecasting up to 45-days</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;C....4600786J</link>
<description>Accurate forecasting of F10.7 index is important on short, medium and
long-term timescales since F10.7 is an excellent proxy of solar activity
and it plays an important role within the Space Weather framework. The
analysis of the signatures of transient solar radio emission and its
prediction are a challenging task as the underpinning physical processes
are typically nonlinear, non-stationary and chaotic. In this paper we
want to present three Deep Learning approaches for the daily forecasting
of the adjusted F10.7 solar radio flux up to 45 days, using a family of
Long Short Term Memory (LSTM) based models. We investigated two novel
hybrid architectures: the LSTM model used in combination with Fast
Iterative Filtering as decomposition algorithm (FIF-LSTM) and a method
based on Multi-Head-Attention architecture (FIF-LSTM-MHA). FIF is a
robust decomposition signal method very suitable for analyzing non-
linear and non-stationary time series and it is used to separate the
original time series into different oscillation components according to
frequency, derived without leaving the time domain before to be fed into
the neural network. The Attention mechanism is able to keep track of
long-term dependencies in data sequences and improve the computational
efficiency of the prediction model by reducing the effect of irrelevant
information, mimicking human attention and selecting the most critical
input. Our comparative analysis evaluated the models' performance for
different time lags and solar activity levels. The results indicated
that the hybrid models achieve better performance than the LSTM model
for mid-range F10.7 predictions while the LSTM achieves better
performance within the first few time lags. FIF-LSTM-MHA gives more
promising output for longer forecasts since it tends to smooth the
prediction curve due to the peculiarity of the Attention module to
discard less relevant features of the time series and highlight the
global trend.</description>
</item>
<item>
<title> Particle-in-cell simulations of electron-positron cyclotron maser forming pulsar radio zebras</title>
<link>https://ui.adsabs.harvard.edu/abs/2024A&amp;A...681A.113L</link>
<description>Context. The microwave radio dynamic spectra of the Crab pulsar
interpulse contain fine structures represented via narrowband
quasiharmonic stripes. The pattern significantly constrains any
potential emission mechanism. Similar to the zebra patterns observed,
for example, in type IV solar radio bursts or decameter and kilometer
Jupiter radio emission, the double plasma resonance (DPR) effect of the
cyclotron maser instability may allow for interpretion of observations
of pulsar radio zebras. &lt;BR /&gt; Aims: We provide insight at kinetic
microscales of the zebra structures in pulsar radio emissions
originating close to or beyond the light cylinder. &lt;BR /&gt; Methods: We
present electromagnetic relativistic particle-in-cell (PIC) simulations
of the electron-positron cyclotron maser for cyclotron frequency smaller
than the plasma frequency. In four distinct simulation cycles, we
focused on the effects of varying the plasma parameters on the
instability growth rate and saturation energy. The physical parameters
were the ratio between the plasma and cyclotron frequency, the density
ratio of the "hot" loss-cone to the "cold" background plasma, the loss-
cone characteristic velocity, and comparison with electron-proton
plasma. &lt;BR /&gt; Results: In contrast to the results obtained from
electron-proton plasma simulations (for example, in solar system
plasmas), we find that the pulsar electron-positron maser instability
does not generate distinguishable X and Z modes. On the contrary, a
singular electromagnetic XZ mode was generated in all studied
configurations close to or above the plasma frequency. The highest
instability growth rates were obtained for the simulations with integer
plasma-to-cyclotron frequency ratios. The instability is most efficient
for plasma with characteristic loss-cone velocity in the range
v&lt;SUB&gt;th&lt;/SUB&gt; = 0.2  0.3c. For low density ratios, the highest peak of
the XZ mode is at double the frequency of the highest peak of the
Bernstein modes, indicating that the radio emission is produced by a
coalescence of two Bernstein modes with the same frequency and opposite
wave numbers. Our estimate of the radiative flux generated from the
simulation is up to 30 mJy from an area of 100 km&lt;SUP&gt;2&lt;/SUP&gt; for an
observer at 1 kpc distance without the inclusion of relativistic beaming
effects, which may account for multiple orders of magnitude.</description>
</item>
<item>
<title> Magnetic Properties of Source Regions of CMEs and DH Type II Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298..144V</link>
<description>The Sun is a dynamic star that exhibits various phenomena, including
solar flares, coronal mass ejections (CMEs), and Type II radio bursts.
CMEs are large-scale eruptions of plasma and magnetic field from the Sun
that can disrupt the interplanetary medium and the Earth's magnetic
field. Type II radio bursts are radio emissions associated with shocks
generated by the CMEs. Only a few CMEs are associated with Type II radio
bursts and the reasons for the absence of these bursts are still under
debate. The magnetic properties of source active regions (ARs) from
where CMEs with and without decameter-hectometer (DH) Type II radio
bursts originate are investigated. Relations between the speed of CMEs
and the source region properties are also obtained for these two groups
of events (with and without radio bursts). The data from the Solar
Dynamics Observatory (SDO) and the Radio and Plasma Wave (WAVES)
Experiment on board the Wind spacecraft and the CMEs observed by the
Solar and Heliospheric Observatory (SOHO) mission for the period of 2010
- 2014 in Solar Cycle 24 are utilized for this study. The statistical
properties (like range, mean, median, and standard deviation) of source
AR magnetic properties and the speed of the CMEs associated with DH Type
II radio bursts (first group called radio loud) are found to be higher
than those of CMEs without DH Type II radio bursts (second group called
radio quiet). In addition, we found a positive correlation between the
magnetic properties of the source AR and the speed of the CMEs with DH
Type II radio bursts, but it is absent for events without DH Type II
bursts. We also found that the probability of CME-streamer interaction
is higher for the first group than for the second group, which shows a
strong relation between the CME-streamer interaction and Type II bursts.
These results reveal distinct magnetic characteristics in the source
region for radio loud and radio quiet CMEs.</description>
</item>
<item>
<title> Analysis of Two Selected Solar Events in 2011 and 2015 With Mars Express Radio Occultation Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RaSc...5807784K</link>
<description>The temporal behavior of the Martian ionosphere is highly variable due
to various dynamic processes including space weather events. Here, we
study the effect of solar flares and coronal mass ejections (CMEs) on
the Martian ionosphere for two selected solar events in 2011 and 2015,
using the publicly available Mars EXpress (MEX) radio occultation (RO)
data (MaRS). We developed a data processing software that converts the
calibrated Radio Occultation (RO) Doppler data to scientifically
valuable atmospheric profiles. Using this software and previously
unexplored MaRS observations, the variations in ionospheric parameters
(electron density profiles and total electron content (TEC)) are
calculated in order to evaluate the ionospheric changes due to solar
flares and CMEs. The RO measurements mostly available 1-4 days apart
from the peak events, showed no evident change in the TEC nor in the
shape of electron density profiles except for a possible gradual
decrease in altitude of M2 (main layer) peak density following the
arrival of CMEs. To better quantify the effect of solar events on
electron density profiles, RO observations near the time of arrival of
solar flares and CMEs are crucial. This can be achieved by frequent RO
measurements by various Mars orbiters including spacecraft-to-spacecraft
measurements assisted by multi-instrument monitoring of the ionosphere.</description>
</item>
<item>
<title> A Novel Low-frequency Radio Astronomical Observation Array (1   90 MHz) and its First Light</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RAA....23l5007Y</link>
<description>The extremely low frequency (f &lt; 40 MHz) is a very important frequency
band for modern radio astronomy observations. It is also a key frequency
band for solar radio bursts, planetary radio bursts, fast radio bursts
detected in the lunar space electromagnetic environment, and the Earth's
middle and upper atmosphere with low dispersion values. In this
frequency band, the solar stellar activity, the early state of the
universe, and the radiation characteristics of the planetary
magnetosphere and plasma layer can be explored. Since there are few
observations with effective spatial resolution in the extremely low
frequency, it is highly possible to discover unknown astronomical
phenomena on such a band in the future. In conjunction with low
frequency radio observation on the far side of the Moon, we initially
set up a novel low-frequency radio array in the Qitai station of
Xinjiang Astronomical Observatory deep in Tianshan Mountains, Xinjiang,
China on 2021 August 23. The array covers an operating frequency range
of 1 ~ 90 MHz with a sensitivity of -78 dBm/125kHz, a dynamic range of
72 dB, and a typical gain value of 6 dBi, which can realize unattended
all-weather observations. The two antennas due south of the Qitai Low-
Frequency Radio Array were put into trial observations on 2021 May 28,
and the very quiet electromagnetic environment of the station has been
confirmed. So far, many solar radio bursts and other foreign signals
have been detected. The results show that this novel low frequency radio
array has the advantages of good performance, strong direction, and high
antenna efficiency. It can play a unique role in Solar Cycle 25, and has
a potential value in prospective collaborative observation between the
Earth and space for extremely low frequency radio astronomy.</description>
</item>
<item>
<title> Application to early great solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2023PASJ...75.1095M</link>
<description>Large solar flares occasionally trigger significant space-weather
disturbances that affect the technological infrastructures of modern
civilization, and therefore require further investigation. Although
these solar flares have been monitored by satellite observations since
the 1970s, large solar flares occur only infrequently and restrict
systematic statistical research owing to data limitations. However,
Toyokawa Observatory has operated solar radio observations at low
frequencies (at 3.75 and 9.4 GHz) since 1951 and captured the early
great flares as solar radio bursts. To estimate the magnitudes of flares
that occurred before the start of solar X-ray (SXR) observations with
the Geostationary Operational Environmental Satellite (GOES) satellites,
we show the relationship between microwave fluxes at 3.75 and 9.4 GHz
and X-ray fluxes of flares that occurred after 1988. In total, we
explored 341 solar flares observed with the Nobeyama Radio Polarimeters
and Toyokawa Observatory from 1988-2014 and compared them with the SXR
observations recorded by the GOES satellites. The correlation
coefficient was approximately 0.7. Therefore, the GOES X-ray class can
be estimated from the peak flux at 3.75 and 9.4 GHz with a large
variance and an error of factor of 3 (1). Thus, for the first time, we
quantitatively estimated the light curves of two early solar flares
observed in 1956 February by the Toyokawa solar radio observations using
the relationship between SXR thermal radiation and microwave nonthermal
radiation (Neupert, 1968, ApJ, 153, 59).</description>
</item>
<item>
<title> Fast radio bursts trigger aftershocks resembling earthquakes, but not solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.526.2795T</link>
<description>The production mechanism of repeating fast radio bursts (FRBs) is still
a mystery, and correlations between burst occurrence times and energies
may provide important clues to elucidate it. While time correlation
studies of FRBs have been mainly performed using wait time
distributions, here we report the results of a correlation function
analysis of repeating FRBs in the 2D space of time and energy. We
analyse nearly 7,000 bursts reported in the literature for the three
most active sources of FRB 20121102A, 20201124A, and 20220912A, and find
the following characteristics that are universal in the three sources. A
clear power-law signal of the correlation function is seen, extending to
the typical burst duration (~ 10 msec) towards shorter time intervals
(t). The correlation function indicates that every single burst has
about a 10-60 per cent chance of producing an aftershock at a rate
decaying by a power law as  (t)&lt;SUP&gt;-p&lt;/SUP&gt; with p = 1.5-2.5, like
the Omori-Utsu law of earthquakes. The correlated aftershock rate is
stable regardless of source activity changes, and there is no
correlation between emitted energy and t. We demonstrate that all these
properties are quantitatively common to earthquakes, but different from
solar flares in many aspects, by applying the same analysis method for
the data on these phenomena. These results suggest that repeater FRBs
are a phenomenon in which energy stored in rigid neutron star crusts is
released by seismic activity. This may provide a new opportunity for
future studies to explore the physical properties of the neutron star
crust.</description>
</item>
<item>
<title> Using Partial Solar Eclipse for the 14-Metre Radio Telescope Calibration</title>
<link>https://ui.adsabs.harvard.edu/abs/2023LatJP..60f..54K</link>
<description>A partial solar eclipse occurred on 25 October 2022, in the central and
northern parts of Europe. The partial solar eclipse was observed at
Aalto University Metshovi Radio Observatory, Finland at the radio
wavelength of 8 mm (37 GHz). In Finland, the magnitude of the partial
solar eclipse was 62.7 %. Solar radio maps at the time cadence of about
9 minutes were observed over the whole eclipse. The solar eclipse
observations could be used for instrument calibration purposes. This
paper investigates the solar brightness temperature, the limb
brightening effect, the height of the chromosphere and the location of
radio brightening using the aforementioned partial solar eclipse
observations. &lt;P /&gt;We got the confirmation that our earlier results are
consistent, e.g., the solar brightness temperature matches with 8100 K 
300 K. It was also possible to detect limb brightening effect. However,
the prevailing solar activity might have distorted the final
conclusions. The Moon should operate as a focusing element and the
location of radio brightenings could be defined more carefully than in
the normal conditions. We investigated this feature. Our results are in
some parts unexpected and need further investigations.</description>
</item>
<item>
<title> Pre-impulsive and Impulsive Phases of the Sub-Terahertz Flare of March 28, 2022</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63.1218M</link>
<description>Properties of the solar radio spectrum, as well as the temporal profiles
of flare emission, indicate the thermal nature of the sub-terahertz
(sub-THz) component observed as the growth of radio emission in the
frequency range of 1001000 GHz. The sub-THz flare onset can be ahead of
the impulsive phase for several minutes. However, the origin of the pre-
impulsive and impulsive sub-THz emission remains unclear. The present
work is devoted to a detailed analysis of the M4.0 X-class solar flare
observed on March 28, 2022 with the Bauman Moscow State Technical
University Radio Telescope RT-7.5 at 93 GHz. We supply these data with
multiwavelength solar observations in the X-ray (GOES, GBM/Fermi),
extreme ultraviolet (AIA/SDO), and microwave ranges. The differential
emission measure (DEM) responsible for EUV emission is determined by
solving the inverse problem based on the AIA/SDO data. Using the DEM and
assuming a thermal free-free emission mechanism in pre-impulsive and
impulsive phases, we calculated the millimeter emission flux of coronal
plasma of the flare source, which turned out to be much smaller than the
observed values. We concluded that electrons accelerated in the corona
and heat fluxes from the coronal loop top cannot be responsible for
heating the sub-THz emission source located in the transition region and
upper chromosphere. A possible origin of chromospheric heating in the
pre-impulsive phase of the solar flare is discussed.</description>
</item>
<item>
<title> A Statistical Model of CME Acceleration</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63.1197O</link>
<description>An algorithm for automatic approximation of the time dependence x(t) is
built for the observed coordinate of the coronal mass ejection (CME)
front from the admissible starting point to the first appearance in the
field of view of the LASCO coronagraph and further, up to a heliocentric
distance of ~25 solar radii (R&lt;SUB&gt;S&lt;/SUB&gt;). In the region from the
starting point to the first appearance of the CME, two sections are
assumed, with uniform (impulsive) acceleration and with uniform motion;
then, the motion is approximated by observations. At the beginning of
the approximation, either the CME start time is found through the
appearance of certain frequencies of radio emissions (RSTN data) and
type II and IV radio emissions (sequence characteristics are determined
by machine learning), or the start time is determined by averaging over
the allowable takeoff area; then the polynomial-ballistic model is
optimized. The first and second derivatives x(t) determine the speed and
acceleration of the CME at any point of its trajectory. Such an
algorithm is necessary to obtain the most accurate kinematic
characteristics of CMEs, which can allow one to study the physical,
spatial, and temporal relationships between flares and CMEs in all their
diversity. Widely used approximation techniques simplify the real CME
trajectories x(t), thereby possibly discarding important features of the
CME kinematics and flare development in the posteruptive phase. The
algorithm was trained and tested on 17 solar flares and associated CMEs,
which are known for their powerful proton events with proton energies
greater than 300 MeV. The rate of the first occurrence of CMEs turned
out to be different from the average rate given in the LASCO catalog,
which is important for estimating the energy of flares and CMEs. In 7
out of 17 events, there was acceleration only in the impulsive phase
(and then deceleration), while acceleration in the impulsive and
posteruptive phases occurred in 10 events. In 4 out of 17 events, CME
velocities greater than 2000 km/s were reached at a distance of
20R&lt;SUB&gt;S&lt;/SUB&gt;. The accuracy of determining the kinematic
characteristics of CMEs can be improved by using additional
observations, for example, SDO AIA in the September 10, 2017 event.</description>
</item>
<item>
<title> On the Relationship of Solar Energetic Particles with Metric Type II Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63.1086T</link>
<description>According to the data from the GOES satellites and the SRS solar radio
spectrograph, 112 proton events were analyzed for the time interval from
November 24, 2000 to December 20, 2014, accompanied by an increase in
the intensity of solar energetic particles (protons) I&lt;SUB&gt;p&lt;/SUB&gt; with
energies E&lt;SUB&gt;p&lt;/SUB&gt; &gt; 1850 MeV and type II radio bursts in the range
of 25180 MHz. A correlation was found for the proton intensity
I&lt;SUB&gt;p&lt;/SUB&gt; with the intensity of type II radio bursts I&lt;SUB&gt;i&lt;/SUB&gt;
and the frequency drift rate V. The correlation coefficients between
I&lt;SUB&gt;p&lt;/SUB&gt; and I&lt;SUB&gt;i&lt;/SUB&gt;, as well as between I&lt;SUB&gt;p&lt;/SUB&gt; and V,
reach approximately 0.82 and 0.67, respectively. The correlation
decreases quite sharply at E&lt;SUB&gt;p&lt;/SUB&gt; &gt; 100 MeV. Nonthermal electrons
responsible for type II radio bursts and energetic protons are generated
at the fronts of the same shock waves, while the acceleration of
relativistic particles with E&lt;SUB&gt;p&lt;/SUB&gt; &gt; 100 MeV is determined by
nonthermal processes in the region of flare energy release.</description>
</item>
<item>
<title> Quick Event During the Decay Phase of the Microwave Emission of a Flare on May 22, 2021</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63.1062M</link>
<description>This paper presents the results of a study of a short event that
occurred during the decay phase of a C6.0 circular flare (GOES). The
event was simultaneously observed by the Irkutsk Incoherent Scatter
Radar at 161 MHz and by the Siberian Radioheliograph (SRH) at 5.6 GHz.
The SRH data were obtained at a single frequency, but with a high time
resolution (0.2 s). This made it possible to localize the microwave
source and carry out its temporal profile using imaging photometry. The
similarity of the time profiles at both frequencies and the close values
of the periods of the quasi-periodic oscillations seen on both profiles
indicate a close relationship between the emeission in the meter and
microwave ranges. According to the images at 5.6 GHz, the burst source
was located near the circular ribbon of the flare, but was not a part of
it. The event was folowed by an eruption that manifested itself in the
meter range as the Type II radio burst at frequencies above 200 MHz,
while a burst at 161 MHz demonstrated the emission of the Type III radio
burst. An analysis of the three-dimensional structure of the magnetic
field, reconstructed on the basis of vector magnetograms, showed that
the event source was located on relatively open field lines, which were
above the dome structure of the circular flare. The active region
topology near the microwave source of the event suggests the following
scenario based on the expansion of the dome structure of the circular
flare due to gas dynamic processes. This caused an impact on relatively
open field lines, which resulted to eruption, acceleration of electrons,
and their propagation along open field lines. It is shown that the event
was triggered by a flare, despite the absence of a direct spatial
connection between the burst and flare ribbons.</description>
</item>
<item>
<title> Sub-Terahertz Radiation Features from the Flare of Proxima Cen</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..937T</link>
<description>A comparative analysis of stellar and solar flares at millimeter
wavelength range has been carried out using the red dwarf Proxima
Centauri as an example. The main attention is paid to the results of
ALMA observations, which show that the flux of sub-THz radiation from
stellar flares is an order of magnitude greater than that for solar
flares, decreases with radiation frequency, and has a degree of linear
polarization reaching tens of percent. We showed that the synchrotron
mechanism is responsible for the sub-THz radiation, which assumes the
acceleration of electrons to ultrarelativistic energies. The observed
relationship between sub-THz, radio, and X-ray emission from stellar
flares is discussed. The hypothesis about the important role of flare
energy release in the dense layers of the stellar atmosphere is
substantiated.</description>
</item>
<item>
<title> Ground-Based Observations of the Sun for Space Weather Forecasting</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..863T</link>
<description>The possibilities for organizing a solar activity observation service
for space weather forecasting are considered. At this stage, the most
promising approach is the establishment of a ground-based observation
network. This network should include solar magnetographs for observing
large-scale magnetic fields of the Sun and patrol optical telescopes for
detecting coronal mass ejections and solar flares. Magnetographic
observations provide data for assessing recurrent solar wind streams.
Patrol telescopes operating in continuous mode make it possible to
detect eruptive moments and determine parameters of coronal mass
ejections at the initial stage. The network can be complemented by other
types of observations in radio and optical bands. The article discusses
the composition of observation tools as well as methods and models of
forecasting.</description>
</item>
<item>
<title> numerical modeling</title>
<link>https://ui.adsabs.harvard.edu/abs/2023CoSka..53c.176K</link>
<description>Solar flares, as strong explosions on the Sun's surface, are well known
driving agents that severely affect the near-Earth environment,
producing additional ionization within the sunlit Earth's atmospheric
layers. X-ray solar flares can be classified regarding their effects on
the lower ionosphere and its electron density profile. The focus of this
research is on the study of disturbances induced by X-ray solar flares
in order to predict the impact of possible weak solar events. In this
paper we examined solar activity of lower intensity by conducting
numerical modeling using several models and based on data obtained by
very low frequency radio signals and from the Geostationary Operational
Environmental Satellite (GOES) database on solar X-ray radiation.</description>
</item>
<item>
<title> data and modeling</title>
<link>https://ui.adsabs.harvard.edu/abs/2023CoSka..53c.138K</link>
<description>Solar flares are among main extraterrestrial events that are well known
to severely affect both space weather and near-Earth surrounding
conditions. Under incident X-ray solar flare radiation, ionospheric
plasma undergoes perturbations clearly and distinctly observable on
ground-based monitoring systems' recordings. Mid-latitude lower
ionosphere under influence of energetic solar flare events was examined
by employing different numerical modeling procedures, including Machine
Learning, relying on ground-based Very Low Frequency (VLF) radio signal
recordings from Belgrade VLF database and solar soft X-ray irradiance
satellite measurements taken from Geostationary Operational
Environmental Satellite (GOES) database.</description>
</item>
<item>
<title> Expansion of the Soft X-ray Source and ``Magnetic Detonation'' in Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AstL...49..731S</link>
<description>The detection of radio emission from solar flares at frequencies below
${}2$ GHz allows the upper limits for the characteristic size of the
soft X-ray (SXR) source $L(t)$ to be estimated under the assumption that
the density $n(t)$ is determined by the plasma frequency
$&lt;SUB&gt;p&lt;/SUB&gt;$. If the SXR source with a higher density is inside the
radio source, then the size of the SXR source will be
$L(t)&lt;(EM(t)/2n(t)&lt;SUP&gt;2&lt;/SUP&gt;)^{1/3}$, where $EM(t)$ is the emission
measure. For three flares (C7.2 on December 22, 2009, M2.9 on July 6,
2012, and X1.1 on July 6, 2012) we calculate the expansion speeds of the
SXR source $V(t) dL(t)/dt$, which are compared with the estimates of
the sound speed and the Alfvn speed. By ``magnetic detonation'' we mean
the process of the propagation of magnetic reconnection with a
supersonic speed in eruptive flares. Magnetic detonation and the
succeeding coronal mass ejection (CME) were realized in the December 22,
2009 C7.2 and July 6, 2012 X1.1 flares, in which supersonic and super-
Alfvn speeds were reached if the density of the SXR source was lower
than $2.1 10&lt;SUP&gt;9&lt;/SUP&gt;$ and $7.4 10&lt;SUP&gt;8&lt;/SUP&gt;$ cm${}^{-3}$
($&lt;SUB&gt;p&lt;/SUB&gt;&lt;410$ and ${&lt;}245$ MHz), respectively. There were no
magnetic detonation and CME in the July 6, 2012 M2.9 flare, whose radio
emission frequencies were only above 1415 MHz ($n&gt;2.5 10^{10}$
cm${}^{-3}$). For magnetic detonation in the July 6, 2012 X1.1 flare we
have estimated the magnetic field strength, the reconnection electric
field strength, the plasma flow, and the CME mass.</description>
</item>
<item>
<title> Solar Radio Burst Detection Based on the MobileViT-SSDLite Lightweight Model</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJS..269...51H</link>
<description>Real-time detection of solar radio bursts is crucial in solar physics
research and space weather forecasting. However, current research on the
automatic detection of solar radio bursts is limited to identifying the
presence or absence of solar radio bursts or recognizing only a single
type of burst, such as type II or III. Furthermore, existing methods
cannot learn spectral and temporal features and often suffer from the
drawbacks of large network models, resulting in slow speeds. This paper
proposes an automatic recognition and localization method based on a
lightweight object detection model for solar radio burst events. We
collected observation data from e-CALLISTO and established a data set
containing type II, III, IV, and V solar radio bursts. To address the
real-time requirements of practical applications and consider the
temporal and frequency domain information of spectrogram images, we
improved a vision transformer with a self-attention mechanism and
adopted a lightweight model for detection. The experimental results
demonstrate that our proposed method achieves an average precision at a
50% intersection-over-union threshold of 78.2% and a recall rate of 92%
on the established solar radio burst data set. Additionally, the model
operates at a detection speed of 54.8 frames s&lt;SUP&gt;-1&lt;/SUP&gt;, where a
frame refers to a spectral image with a duration of 15 minutes, enabling
efficient automated detection and localization of type II, III, IV, and
V solar radio bursts.</description>
</item>
<item>
<title> The Effect of the Parametric Decay Instability on the Morphology of Coronal Type III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...959L..33S</link>
<description>The nonlinear evolution of Alfvn waves in the solar corona leads to the
generation of Alfvnic turbulence. This description of the Alfvn waves
involves parametric instabilities where the parent wave decays into slow
mode waves giving rise to density fluctuations. These density
fluctuations, in turn, play a crucial role in the modulation of the
dynamic spectrum of type III radio bursts, which are observed at the
fundamental of local plasma frequency and are sensitive to the local
density. During observations of such radio bursts, fine structures are
detected across different temporal ranges. In this study, we examine
density fluctuations generated through the parametric decay instability
(PDI) of Alfvn waves as a mechanism to generate striations in the
dynamic spectrum of type III radio bursts using magnetohydrodynamic
simulations of the solar corona. An Alfvn wave is injected into the
quiet solar wind by perturbing the transverse magnetic field and
velocity components, which subsequently undergo the PDI instability. The
type III burst is modeled as a fast-moving radiation source that samples
the background solar wind as it propagates to emit radio waves. We find
the simulated dynamic spectrum to contain striations directly affected
by the multiscale density fluctuations in the wind.</description>
</item>
<item>
<title> Solar Orbiter Observations of a Match Made in the Heliosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...959..128L</link>
<description>Solar Orbiter's four in situ instruments have recorded numerous
energetic electron events at heliocentric distances between 0.5 and 1
au. We analyze energetic electron fluxes, spectra, pitch-angle
distributions, associated Langmuir waves, and type III solar radio
bursts for three events to understand what causes modifications in the
electron flux and identify the origin and characteristics of features
observed in the electron spectrum. We investigate what electron beam
properties and solar wind conditions are associated with Langmuir wave
growth and spectral breaks in the electron peak flux as a function of
energy. We observe velocity dispersion and quasilinear relaxation in the
electron flux caused by the resonant wave-particle interactions in the
deca-keV range, at the energies at which we observe breaks in the
electron spectrum, cotemporal with the local generation of Langmuir
waves. We show, via the evolution of the electron flux at the time of
the event, that these interactions are responsible for the spectral
signatures observed around 10 and 50 keV, confirming the results of
simulations by Kontar and Reid. These signatures are independent of
pitch-angle scattering. Our findings highlight the importance of using
overlapping FOVs when working with data from different sensors. In this
work, we exploit observations from all in situ instruments to address,
for the first time, how the energetic electron flux is modified by the
beam-plasma interactions and results in specific feature appearing in
the local spectrum. Our results, corroborated with numerical
simulations, can be extended to a wider range of heliocentric distances.</description>
</item>
<item>
<title> Scale Invariance in Gamma-Ray Flares of the Sun and 3C 454.3</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...959..109P</link>
<description>Using the gamma-ray flare samples of the Sun and 3C 454.3 observed by
the Fermi telescope, we investigate the statistical properties of sizes
including fluence (energy), peak flux (luminosity), duration time, and
waiting time in this work. We find that the cumulative distribution of
the fluctuations of these sizes follow well the Tsallis q-Gaussian
function. The obtained q values from q-Gaussian distribution remain
stable around 2 without any significant change, implying that there is a
scale invariance structure in gamma-ray flares of the Sun and 3C 454.3.
This scale invariance characteristics of the Sun and 3C 454.3 indicated
by q values are also comparable to those of earthquakes, soft gamma
repeaters, fast radio burst (FRB 20121102), and X-ray flares of gamma-
ray bursts. On top of that, we verify the relationship between q values
and the power-law indices  from the size frequency distributions, which
is expressed as q = ( + 2)/. These statistical findings could be well
explained within the physical framework of a self-organizing criticality
system.</description>
</item>
<item>
<title> Solar Radio Spectro-polarimeter (50-500 MHz). I. Design, Development, and Characterization of a Cross-polarized, Log-periodic Dipole Antenna</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...958..181K</link>
<description>The Zeeman effect has been routinely used to image and quantify the
solar photospheric magnetic field (B). Such a direct measuring technique
is not yet available for the corona (Lin et al. 2004). Since almost all
transient nonthermal radio emissions from the corona are either
partially or fully circularly polarized, observing their polarization
signatures over broad frequency ranges would be of help to estimate B as
a function of heliocentric height. This article aims to describe the
design and development of a Cross-polarized Log-Periodic Dipole Antenna
(CLPDA), an integral part of a radio spectro-polarimeter, which works in
the 50-500 MHz frequency-range and to explain the tests that were
carried out to characterize it. The above frequency range corresponds to
a heliocentric height range 1.03 &lt; r &lt; 2.5 R &lt;SUB&gt;&lt;/SUB&gt; (R
&lt;SUB&gt;&lt;/SUB&gt; = photospheric radius), wherein the numerous coronal
nonthermal transients associated with space-weather effects are observed
to originate. The CLPDA is used to determine the strength and sense of
polarization of the received radio signal. The uncertainty involved in
the determination depends on the polarization-isolation (PI) between the
two orthogonal components of a CLPDA. Some of the recent advancements
made in the antenna design concepts at high frequencies (~GHz) were
adopted to reduce the PI at low frequencies (~MHz). Throughout the above
frequency range, the CLPDA has a gain, return loss, and PI of 6.6 dBi,
-10 dB, and -27 dB, respectively. The average PI of the CLPDA varies
from -30 to -24 dB over an azimuthal angle range 0 to 45 within which
the observations are performed regularly.</description>
</item>
<item>
<title> A Comparative Study of Ground-level Enhancement Events of Solar Energetic Particles</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...958..122K</link>
<description>Major solar eruptions can accelerate protons up to relativistic
energies. Solar relativistic ions arriving at 1 au may cause a solar
particle event detectable by the worldwide network of neutron monitors
(NMs), a ground-level enhancement (GLE) event. Using the newly computed
NM yield function, we have fitted the 15 historic GLEs. Moments of the
fitted proton distributions are used for the analysis. Profiles of the
proton net flux are very diverse, while some profiles are similar. For
this study, we select two events with similar time profiles, GLE 60
(2001 April 15) and GLE 65 (2003 October 28), and ask what makes these
GLEs similar. We compare the GLEs with their progenitor solar flares and
coronal mass ejections (CMEs). We find a close relationship between the
rise and peak of the GLE, on the one hand, and the solar flare and the
metric radio emissions from extended coronal sources at the base of the
CME, on the other hand. The GLE decay time, the rate of the proton
spectrum evolution, and the CME speed are proportional to the duration
of the soft X-ray flare. We compare the two GLEs with GLE 59 (2000 July
14) analyzed by Klein et al. and with the deka-MeV nucleon&lt;SUP&gt;-1&lt;/SUP&gt;
proton and helium data from the ERNE instrument on the Solar and
Heliospheric Observatory spacecraft. The comparison indicates that a
single solar eruption can produce more than one component of solar
energetic particles, differently contributing at different energies and
locations.</description>
</item>
<item>
<title> The physics of solar spectral imaging observations in dm-cm wavelengths and the application on space weather</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72.5563T</link>
<description>Recently, several new solar radio telescopes have been put into
operation and provided spectral-imaging observations with much higher
resolutions in decimeter (dm) and centimeter (cm) wavelengths. These
telescopes include the Mingantu Spectral Radioheliograph (MUSER, at
frequencies of 0.415 GHz), the Expanded Owens Valley Solar Array
(EOVSA, at frequencies of 118 GHz), and the Siberian Radio Heliograph
(SRH, at frequencies of 324 GHz). These observations offer
unprecedented opportunities to study solar physics and space weather,
especially to diagnose the coronal magnetic fields, reveal the basic
nature of solar eruptions and the related non-thermal energy release,
particle accelerations and propagation, and the related emission
mechanisms. These results might be the important input to the space
weather modeling for predicting the occurrence of disastrous powerful
space weather events. In order to provide meaningful reference for other
solar physicists and space weather researchers, this paper mainly focus
on discussing the potential scientific problems of solar radio spectral-
imaging observations in dm-cm wavelengths and its possible applications
in the field of space weather. These results will provide a helpful
reference for colleagues to make full use of the latest and future
observation data obtained from the above solar radio telescopes.</description>
</item>
<item>
<title> Modelling of foF2 using artificial neural network over Equatorial Ionization Anomaly (EIA) region stations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72.5539A</link>
<description>An ANN based model has been suggested for foF2 values over EIA region
stations during 19582008. The developed model predicts foF2 with a root
mean square error of less than 1 MHz for the unseen testing data. The
model may be used for practical purposes over Asian longitude sector,
particularly for Pakistan.</description>
</item>
<item>
<title> Performance of a locally adapted NeQuick-2 model during high solar activity over the Brazilian equatorial and low-latitude region</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72.5520O</link>
<description>The Brazilian equatorial and low-latitude regions are subject to various
dynamic and electrodynamics processes. As a result, ionospheric modeling
over this region remains a challenge. In this article, we present the
results of first observation of data ingestion into the climatological
model, NeQuick during both quiet and disturbed conditions over Brazil.
The variation of the daily F10.7 solar radio flux, the main driver of
the NeQuick model, strongly influences its performance in both space and
time, especially during high solar activity. With data ingestion, using
the local level of ionization, NeQuick's performance can be improved. We
developed an algorithm to obtain the local effective ionization
parameters (Az1 and Az2) using a single station, in the equatorial
trough and low-latitude regions, which are subsequently used in the
NeQuick to reproduce vTEC at co-located stations. The model's input
(effective ionization level) was obtained when the modeled vTEC best
fits the measured vTEC at the reference stations Maraba (5.35 S, 49.11
S, dip lat.: 3.06 S; MABA) and Ourinhos (22.93 S, 49.88 S, dip lat.:
17.42 S; OURI). Statistical results show that the model's performance
greatly improves after data ingestion, reproducing vTEC at all latitudes
close to the reference stations in 2014. We found that NeQuick improved
by 71 %, 74 %, 83 %, and 69 % after ingestion during the storm periods
of 1721 February, 1014 April, 610 June, and 2327, December in the
low-latitude region at SJSP. Using the Az1 values obtained at MABA and
Az3 at SALU during July 2014, NeQuick reproduces the critical frequency
of the F2 layer with a percentage improvement of approximately 20 % and
37 % respectively.</description>
</item>
<item>
<title> Coronal diagnostics of solar type III radio bursts using LOFAR and PSP observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...680A.106N</link>
<description>Context. Solar type III radio bursts are common phenomena, recognized as
the result of accelerated electron beams propagating through the solar
corona. These bursts are of particular interest as they provide valuable
information about the magnetic field and plasma conditions in the
corona, which are difficult to measure directly. &lt;BR /&gt; Aims: This study
aims to investigate the ambiguous source and the underlying physical
processes of the type III radio bursts that occurred on April 3, 2019,
through the utilization of multi-wavelength observations from the Low-
Frequency Array (LOFAR) radio telescope and the Parker Solar Probe (PSP)
space mission, as well as incorporating results from a Potential Field
Source Surface (PFSS) and magnetohydrodynamic (MHD) models. The primary
goal is to identify the spatial and temporal characteristics of the
radio sources, as well as the plasma conditions along their
trajectories. &lt;BR /&gt; Methods: We applied data preprocessing techniques
to combine high- and low-frequency observations from LOFAR and PSP
between 2.6 kHz and 80 MHz. We then extracted information on the
frequency drift and speed of the accelerated electron beams from the
dynamic spectra. Additionally, we used LOFAR interferometric
observations to image the sources of the radio emission at multiple
frequencies and determine their locations and kinematics in the corona.
Lastly, we analyzed the plasma parameters and magnetic field along the
trajectories of the radio sources using PFSS and MHD model results. &lt;BR
/&gt; Results: We present several notable findings related to type III
radio bursts. Firstly, through our automated implementation, we were
able to effectively identify and characterize 9 type III radio bursts in
the LOFAR-PSP combined dynamic spectrum and 16 type III bursts in the
LOFAR dynamic spectrum. We found that the frequency drift for the
detected type III bursts in the combined spectrum ranges between 0.24
and 4 MHz s&lt;SUP&gt;1&lt;/SUP&gt;, while the speeds of the electron beams range
between 0.013 and 0.12 C. Secondly, our imaging observations show that
the electrons responsible for these bursts originate from the same
source and within a short time frame of fewer than 30 min. Finally, our
analysis provides informative insights into the physical conditions
along the path of the electron beams. For instance, we found that the
plasma density obtained from the magnetohydrodynamic algorithm outside a
sphere (MAS) model is significantly lower than the expected theoretical
density.</description>
</item>
<item>
<title> Source positions of an interplanetary type III radio burst and anisotropic radio-wave scattering</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...680A...1C</link>
<description>Interplanetary solar radio type III bursts provide the means to remotely
study and track energetic electrons propagating in the interplanetary
medium. Due to the lack of direct radio source imaging, several methods
have been developed to determine the source positions from space-based
observations. Moreover, none of the methods consider the propagation
effects of anisotropic radio-wave scattering, which would strongly
distort the trajectory of radio waves, delay their arrival times, and
affect their apparent characteristics. We investigate the source
positions and directivity of an interplanetary type III burst
simultaneously observed by Parker Solar Probe, Solar Orbiter, STEREO,
and Wind and we compare the results of applying the intensity fit and
timing methods with ray-tracing simulations of radio-wave propagation
with anisotropic density fluctuations. The simulation calculates the
trajectories of the rays, their time profiles at different viewing
sites, and the apparent characteristics for various density fluctuation
parameters. The results indicate that the observed source positions are
displaced away from the locations where emission is produced, and their
deduced radial distances are larger than expected from density models.
This suggests that the apparent position is affected by anisotropic
radio-wave scattering, which leads to an apparent position at a larger
heliocentric distance from the Sun. The methods to determine the source
positions may underestimate the apparent positions if they do not
consider the path of radio-wave propagation and incomplete scattering at
a viewing site close to the intrinsic source position.</description>
</item>
<item>
<title> Solar Flare Prediction and Feature Selection Using a Light-Gradient-Boosting Machine Algorithm</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298..137V</link>
<description>Solar flares are among the most severe space-weather phenomena, and they
have the capacity to generate radiation storms and radio disruptions on
Earth. The accurate prediction of solar-flare events remains a
significant challenge, requiring continuous monitoring and
identification of specific features that can aid in forecasting this
phenomenon, particularly for different classes of solar flares. In this
study, we aim to forecast C- and M-Class solar flares utilising a
machine-learning algorithm, namely the Light Gradient Boosting Machine.
We have utilised a dataset spanning nine years, obtained from the Space-
weather Helioseismic and Magnetic Imager Active Region Patches (SHARP),
with a temporal resolution of 1 h. A total of 37 flare features were
considered in our analysis, comprising of 25 active-region parameters
and 12 flare-history features. To address the issue of class imbalance
in solar-flare data, we employed the Synthetic Minority Over-sampling
Technique (SMOTE). We used two labelling approaches in our study: a
fixed 24-h window label and a varying window that considers the changing
nature of solar activity. Then, the developed machine-learning algorithm
was trained and tested using forecast-verification metrics, with an
emphasis on evaluating the true skill statistic (TSS). Furthermore, we
implemented a feature-selection algorithm to determine the most
significant features from the pool of 37 features that could distinguish
between flaring and non-flaring active regions. We found that utilising
a limited set of useful features resulted in improved prediction
performance. For the 24-h prediction window, we achieved a TSS of 0.63
(0.69) and an accuracy of 0.90 (0.97) for C- (M)-Class solar flares.</description>
</item>
<item>
<title> The Brightness Temperature and Magnetic Field of Active Regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298..124M</link>
<description>Solar radio observations provide a powerful diagnostic of the physical
conditions of the solar atmosphere over a wide range of heights. In this
paper, we report regular solar mapping made at the X-band (8.1 - 9.2
GHz) with the Arecibo 12-m radio telescope, covering a period between 13
December 2021 and 9 April 2023. This has demonstrated its potential for
identifying active regions and tracking their brightness-temperature
changes. The X-band results are discussed along with the near-
simultaneous datasets available from space- and ground-based
observations. A comparison of magnetic properties of active regions with
their emission characteristics indicates that the X-band brightness
temperature provides better information of the magnetic-field strength
associated with the emission and a brightness temperature in excess of
13 000 K allows us to infer the possibility of intense flares (i.e., 
M1 class) and coronal mass ejections. The `latitude-time' distribution
of the brightness temperature reveals the three-dimensional evolution of
quiet regions on the Sun, coronal holes, and eruptive sites, over many
solar rotations in the ascending phase of the current Solar Cycle 25.</description>
</item>
<item>
<title> The Correlation between Ionospheric Electron Density Variations Derived from Swarm Satellite Observations and Seismic Activity at the Australian-Pacific Tectonic Plate Boundary</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RemS...15.5557J</link>
<description>Swarm electron density (Ne) observations from the Langmuir probe (LP)
can detect ionospheric disturbances at the altitude of a satellite.
Along-track satellite observations provide a large number of very short
observations of different places in the ionosphere, where Ne is
disturbed. Moreover, different perturbations occupy various Ne signal
frequencies. Therefore, such short signals are more recognizable in two
dimensions, where aside from their change in time, we can observe their
diversity in the frequency domain. Spectral analysis is an essential
tool applied here, as it enables signal decomposition and the
recognition of composite patterns of Ne disturbances that occupy
different frequencies. This study shows a high-resolution application of
short-term Fourier transform (STFT) to Swarm Ne observations in the
Papua New Guinea region in the vicinity of earthquakes, tsunamis, and
related general seismic activity. The system of tectonic plate
junctions, including the Pacific-Australian boundary, is located
orthogonally to Swarm track footprints. The selected wavelengths of
seismically induced ionospheric disturbances detected via Swarm are
compared with the three sets of three-month records of seismic activity:
in the winter solstice of 2016/2017, when seismic activity was highest,
and in the summer solstice and vernal equinox of 2016, which were
calmer. Moreover, more Swarm data records are analyzed at the same
latitudes for validation purposes, in a place where there are no
tectonic plate boundaries that are orthogonal to the Swarm orbital
footprint. Additional validation is supplied through Swarm Ne
observations from completely different latitudes, where the Swarm
orbital footprint orthogonally crosses a different subducting plate
boundary. Aside from the seismic energy, the solar radio flux (F10.7),
equatorial plasma bubbles (EPBs), and geomagnetic ap and Dst indices are
also reviewed here. Their influence on the ionospheric Ne is also found
in Swarm observations. Finally, the Pearson correlation coefficient
(PCC), applied to the pairs of 3-month time series created from Swarm Ne
variations, seismic energy, ap, Dst, and F10.7, summarizes the graphical
inspection of mutual correlations. It points to the predominant
correlation of Swarm Ne disturbances with seismicity, especially during
nighttime. We show that most of the Ne disturbances at a selected
wavelength of 300 km correlate more with seismicity than with
geomagnetic and solar indices. Therefore, Swarm LP can be assessed as
being capable of observing the lithosphere-atmosphere-ionosphere
coupling (LAIC) from the orbit.</description>
</item>
<item>
<title> Unifying VLF Transmitter and Sferic Modeling Efforts Via Tomography</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JGRA..12831989R</link>
<description>We demonstrate a methodology for utilizing measurements from very low
frequency (VLF, 330 kHz) transmitters and lightning emissions to
produce 3D lower electron density maps, and apply it to multiple
geophysical disturbances. The D-region lower ionosphere (6090 km) forms
the upper boundary of the Earth-ionosphere waveguide which allows VLF
radio waves to propagate to global distances. Measurements of these
signals have, in many prior studies, been used to infer path-average
electron density profiles within the D region. Historically, researchers
have focused on either measurements of VLF transmitters or radio
atmospherics (sferics) from lightning. In this work, we build on
recently published methods for each and present a method to unify the
two approaches via tomography. The output of the tomographic inversion
produces maps of electron density over a large portion of the United
States and Gulf of Mexico. To illustrate the benefits of this unified
approach, daytime and nighttime maps are compared between a sferic-only
model and the new approach suggested here. We apply the model to
characterize two geophysical disturbances: solar flares and lower
ionospheric changes associated with thunderstorms.</description>
</item>
<item>
<title> A New Index to Describe the Relationship between Solar Extreme Ultraviolet Variation and Solar Activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...958...69C</link>
<description>In this paper, a new solar activity index based on a novel disturbance
extraction method, the spectral whitening method (SWM), is introduced to
process the solar EUV data on the Atmospheric Imaging Assembly (AIA) on
board the Solar Dynamics Observatory. Our research suggests that the
spatial information derived by SWM can well reflect the location of
disturbance extraction, which is consistent with the location of the
solar active region. It indicates that the disturbance extraction is
effective. From AIA 094  to AIA 335 , SWM results are strongly
correlated with solar radio flux F107 and the sunspot number (SSN),
especially at AIA 211 , where the correlation coefficient reaches the
maximum, while at AIA 1600  and AIA 1700  there are no detectable
correlations. The proposed new solar activity index,
${J}_{P}\left(\mathrm{AIA}\right)$ , has the following characteristics:
(1) the new index can reflect the main variations of F107 and SSN,
indicating that the index is valid; (2) the new index has higher
temporal resolution, which is more conducive to the more detailed study
of solar activities on short timescales; (3) the new index reveals that
the solar atmosphere still has significant variability during solar
minimum characterized by low F107 and SSN; (4) the new index can be used
in conjunction with the new magnetospheric and ionospheric indices,
which are also derived by SWM to deepen the understanding of the causal
chain of space weather and promote the improvement of forecasting
capabilities.</description>
</item>
<item>
<title> Improved Electron Density Model for Solar Wind</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...957...13K</link>
<description>We present a comprehensive analysis of electron density measurements in
the solar wind using quasi-thermal noise (QTN) spectroscopy applied to
data from the first 15 encounters of the Parker Solar Probe mission
(2018 November-2023 March). Our methodology involves the identification
of the plasma line frequency and the calculation of plasma density based
on in situ measurements. By analyzing over 2.1 million data points, we
derive a power-law model for electron density as a function of radial
distance from the Sun in the range of 13 to 50 R &lt;SUB&gt;&lt;/SUB&gt;: n
&lt;SUB&gt;e&lt;/SUB&gt;(r) = (343,466  19921)  r &lt;SUP&gt;(-1.870.11)&lt;/SUP&gt;. This
model provides improved estimates for localizing interplanetary solar
radio bursts. Moreover, obtained electron densities can be used for
calibrating particle instruments on board the Parker Solar Probe. We
discuss its limitations and potential for further refinement with
additional Parker Solar Probe encounters.</description>
</item>
<item>
<title> Separating the effects of earthside and far side solar events. A case study</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72.4074P</link>
<description>On 8 November 2013 a halo-type coronal mass ejection (CME) was observed,
together with flares and type II radio bursts, but the association
between the flares, radio bursts, and the CME was not clear. Our aim is
to identify the origin of the CME and its direction of propagation, and
to exclude features that were not connected to it. On the Earth-facing
side, a GOES C5.7 class flare occurred close to the estimated CME launch
time, followed by an X1.1 class flare. The latter flare was associated
with an EUV wave and metric type II bursts. On the far side of the Sun,
a filament eruption, EUV dimmings, and ejected CME loops were observed
by imaging instruments onboard the Solar TErrestrial RElations
Observatory (STEREO) spacecraft that were viewing the backside of the
Sun. The STEREO radio instruments observed an interplanetary (IP) type
II radio burst at decameter-hectometric wavelengths, which was not
observed by the radio instrument onboard the Wind spacecraft located at
L1 near Earth. We show that the halo CME originated from the eruption on
the far side of the Sun, and that the IP type II burst was created by a
shock wave ahead of the halo CME. The radio burst remained unobserved
from the earthside, even at heliocentric source heights larger than 9
solar radii. During the CME propagation, the X-class flare eruption
caused a small plasmoid ejection earthward, the material of which was
superposed on the earlier CME structures observed in projection. The
estimated heights of the metric type II burst match well with the EUV
wave launched by the X-class flare. As this radio emission did not
continue to lower frequencies, we conclude that the shock wave did not
propagate any further. Either the shock driver died out, as a blast
wave, or the driver speed no longer exceeded the local Alfven speed.</description>
</item>
<item>
<title> Low latitude ionospheric TEC response to the solar flares during the peak of solar cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72.3890S</link>
<description>We describe the newly discovered response of differential vertical total
electron content (DVTEC) in the low-equatorial latitude ionosphere to
the solar flares during the peak of solar cycle 24 i.e., the year 2014.
GPS TEC data for the existing investigation has been acquired from the
international GNSS services network station in Bangalore, India
(geomagnetic latitude 4.58&lt;SUP&gt;&lt;/SUP&gt;N). For the year 2014, we
inspected five X-class solar flares, forty-nine M-class solar flares,
and three hundred ninety-six C-class solar flares in the current study.
To ascertain the relationship between DVTEC and the X-ray and EUV
fluxes, the two main ionizing radiation fluxes during flare events are
used. Additionally, to identify electron density change in the
ionosphere due to solar flares, we used two well-known methodologies,
the baseline method and the mean method. The baseline method provides a
better correlation between DVTEC and X-ray for X-, M-, and C-class
flares. For M- and C- class flares, both methods do not show any
meaningful correlation. The Solar disc location effect shows an enhanced
(0.573) correlation between DVTEC and X-ray*cos (CMD) for the X-class
flares, whereas for M- and C-class flares, no significant change was
observed, which indicates feeble or no CMD effect for lower class solar
flares while it is opposite for X-class flares. Here we suggest that the
high solar activity, and location of the observation station to the EIA
trough region might be the possible reason for the observed results.</description>
</item>
<item>
<title> Uncertainties of the 30-408 MHz Galactic emission as a calibration source for radio detectors in astroparticle physics</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...679A..50B</link>
<description>Context. Arrays of radio antennas have proven to be successful in
astroparticle physics with the observation of extensive air showers
initiated by high-energy cosmic rays in the Earth's atmosphere. Accurate
determination of the energy scale of the primary particles' energies
requires an absolute calibration of the radio antennas for which, in
recent years, the utilization of the Galactic emission as a reference
source has emerged as a potential standard. &lt;BR /&gt; Aims: To apply the
"Galactic calibration" a proper estimation of the systematic
uncertainties on the prediction of the Galactic emission from sky models
is necessary, which we aim to quantify on a global level and for the
specific cases of selected radio arrays. We further aim to determine the
influence of additional natural radio sources on the Galactic
calibration. &lt;BR /&gt; Methods: We compared seven different sky models that
predict the full-sky Galactic emission in the frequency range from 30 to
408 MHz. We made an inventory of the reference maps on which they rely
and used the output of the models to determine their global level of
agreement. We subsequently took typical sky exposures and the frequency
bands of selected radio arrays into account and repeated the comparison
for each of them. Finally, we studied and discuss the relative influence
of the quiet Sun, the ionosphere, and Jupiter. &lt;BR /&gt; Results: We find a
systematic uncertainty of 14.3% on the predicted power from the Galactic
emission, which scales to approximately half of that value as the
uncertainty on the determination of the energy of cosmic particles. When
looking at the selected radio arrays, the uncertainty on the predicted
power varies between 11.7% and 21.5%. The influence of the quiet Sun
turns out to be insignificant at the lowest frequencies but increases to
a relative contribution of ~30% around 400 MHz.</description>
</item>
<item>
<title> Element Abundances in Impulsive Solar Energetic-Particle Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..466R</link>
<description>Impulsive solar energetic-particle (SEP) events were first distinguished
as the streaming electrons that produce type III radio bursts as
distinct from shock-induced type II bursts. They were then observed as
the surprisingly enhanced 3He-rich SEP events, which were also found to
have element enhancements rising smoothly with the mass-to-charge ratio
A/Q through the elements, even up to Pb. These impulsive SEPs have been
found to originate during magnetic reconnection in solar jets where open
magnetic field lines allow energetic particles to escape. In contrast,
impulsive solar flares are produced when similar reconnection involves
closed field lines where energetic ions are trapped on closed loops and
dissipate their energy as X-rays, -rays, and heat. Abundance
enhancements that are power laws in A/Q can be used to determine Q
values and hence the coronal source temperature in the events. Results
show no evidence of heating, implying reconnection and ion acceleration
occur early, rapidly, and at low density. Proton and He excesses that
contribute their own power law may identify events with reacceleration
of SEPs by shock waves driven by accompanying fast, narrow coronal mass
ejections (CMEs) in many of the stronger jets.</description>
</item>
<item>
<title> Relativistic coronal mass ejections from magnetars</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.524.6024S</link>
<description>We study dynamics of relativistic coronal mass ejections (CMEs), from
launching by shearing of foot-points (either slowly - the 'Solar flare'
paradigm, or suddenly - the 'star quake' paradigm), to propagation in
the preceding magnetar wind. For slow shear, most of the energy injected
into the CME is first spent on the work done on breaking through the
overlaying magnetic field. At later stages, sufficiently powerful CMEs
may lead to the 'detonation' of a CME and opening of the magnetosphere
beyond some equipartition radius r&lt;SUB&gt;eq&lt;/SUB&gt;, where the decreasing
energy of the CME becomes larger than the decreasing external
magnetospheric energy. Post-CME magnetosphere relaxes via the formation
of a plasmoid-mediated current sheet, initially at ~r&lt;SUB&gt;eq&lt;/SUB&gt;, and
slowly reaching the light cylinder. Both the location of the foot-point
shear and the global magnetospheric configuration affect the
frequent/weak versus rare/powerful CME dichotomy - to produce powerful
flares, the slow shear should be limited to field lines that close in
near the star. After the creation of a topologically disconnected flux
tube, the tube quickly (at ~ the light cylinder) comes into force-
balance with the preceding wind and is passively advected/frozen in the
wind afterward. For fast shear (a local rotational glitch), the
resulting large amplitude Alfvn waves lead to the opening of the
magnetosphere (which later recovers similarly to the slow shear case).
At distances much larger than the light cylinder, the resulting shear
Alfvn waves propagate through the wind non-dissipatively.</description>
</item>
<item>
<title> On the detection of a solar radio burst event that occurred on 28 August 2022 and its effect on GNSS signals as observed by ionospheric scintillation monitors distributed over the American sector</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JSWSC..13...28W</link>
<description>As part of an effort to observe and study ionospheric disturbances and
their effects on radio signals used by Global Navigation Satellite
Systems (GNSS), alternative low-cost GNSS-based ionospheric
scintillation and total electron content (TEC) monitors have been
deployed over the American sector. During an inspection of the
observations made on 28 August 2022, we found increases in the amplitude
scintillation index (S&lt;SUB&gt;4&lt;/SUB&gt;) reported by the monitors for the
period between approximately 17:45 UT and 18:20 UT. The distributed,
dual-frequency observations made by the sensors allowed us to determine
that the increases in S&lt;SUB&gt;4&lt;/SUB&gt; were not caused by ionospheric
irregularities. Instead, they resulted from Carrier-to-Noise (C/No)
variations caused by a solar radio burst (SRB) event that followed the
occurrence of two M-class X-ray solar flares and a Halo coronal mass
ejection. The measurements also allowed us to quantify the impact of the
SRB on GNSS signals. The observations show that the SRB caused maximum
C/No fadings of about 8 dB-Hz (12 dB-Hz) on L1 ~ 1.6 GHz (L2 ~ 1.2 GHz)
for signals observed by the monitor in Dallas for which the solar zenith
angle was minimum (~24.4) during the SRB. Calculations using
observations made by the distributed monitors also show excellent
agreement for estimates of the maximum (vertical equivalent) C/No
fadings in both L1 and L2. The calculations show maximum fadings of 9
dB-Hz for L1 and of 13 dB-Hz for L2. Finally, the results exemplify the
usefulness of low-cost monitors for studies beyond those associated with
ionospheric irregularities and scintillation.</description>
</item>
<item>
<title> Automatic Detection of Type II Solar Radio Burst by Using 1-D Convolution Neutral Network</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JKAS...56..213C</link>
<description>Type II solar radio bursts show frequency drifts from high to low over
time. They have been known as a signature of coronal shock associated
with Coronal Mass Ejections (CMEs) and/or flares, which cause an abrupt
change in the space environment near the Earth (space weather).
Therefore, early detection of type II bursts is important for
forecasting of space weather. In this study, we develop a deep-learning
(DL) model for the automatic detection of type II bursts. For this
purpose, we adopted a 1-D Convolution Neutral Network (CNN) as it is
well-suited for processing spatiotemporal information within the applied
data set. We utilized a total of 286 radio burst spectrum images
obtained by Hiraiso Radio Spectrograph (HiRAS) from 1991 and 2012, along
with 231 spectrum images without the bursts from 2009 to 2015, to
recognizes type II bursts. The burst types were labeled manually
according to their spectra features in an answer table. Subsequently, we
applied the 1-D CNN technique to the spectrum images using two filter
windows with different size along time axis. To develop the DL model, we
randomly selected 412 spectrum images (80%) for training and validation.
The train history shows that both train and validation losses drop
rapidly, while train and validation accuracies increased within
approximately 100 epoches. For evaluation of the model's performance, we
used 105 test images (20%) and employed a contingence table. It is found
that false alarm ratio (FAR) and critical success index (CSI) were 0.14
and 0.83, respectively. Furthermore, we confirmed above result by
adopting five-fold cross-validation method, in which we re-sampled five
groups randomly. The estimated mean FAR and CSI of the five groups were
0.05 and 0.87, respectively. For experimental purposes, we applied our
proposed model to 85 HiRAS type II radio bursts listed in the NGDC
catalogue from 2009 to 2016 and 184 quiet (no bursts) spectrum images
before and after the type I bursts. As a result, our model successfully
detected 79 events (93%) of type II events. This results demonstrates,
for the first time, that the 1-D CNN algorithm is useful for detecting
type II bursts.</description>
</item>
<item>
<title> Investigation of the nature and parameters of wave processes in the flare region of the solar atmosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2023INASR...8...97H</link>
<description>The paper presents the results of simultaneous observations of
fluctuations of the integral radio emission flux in the solar flare
region generated in the transition layer ( = 10.7 cm) and the lower
corona ( = 27.8 cm). The observations were carried out with the RT-12
radio telescope of the Institute of the Ionosphere of the Republic of
Kazakhstan on June 7, 2011, October 25, 2013, and February 20, 2014. By
measuring the time profiles between quasi-periodic radio emission
intensity fluctuations, it was found that for periods of 20350 seconds,
propagation of perturbations from the chromosphere to the corona is
always observed with a time delay of 20100 seconds. Using a number of
models for the active Sun, estimates were made of the propagation
velocities of disturbances of 2002500 km/s and the ranges of the
detected periods. It is shown that they correspond to the speed of
Alfven and fast magnetoacoustic waves. Thus, we conclude that in our
study, the quasi-periodicity in the flare region of the Sun is
associated with MHD oscillations.</description>
</item>
<item>
<title> Electron Cyclotron Maser Emission in Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChA&amp;A..47..722T</link>
<description>Radio bursts are ubiquitous in the cosmic plasma. Solar radio emission
mainly comes from the outer atmosphere of the sun. It is an induced
radiation phenomenon generated by the interaction between energetic
electrons and solar atmospheric plasma. Different dynamic spectra of
solar radio bursts (SRBs) contain physical information of the plasma
structure and state in the radiation source region. Therefore, the
radiative mechanism of radio bursts has always been the object of
research. There are two kinds of coherent radiation mechanisms related
to solar radio bursts: one is the plasma radiation mechanism based on
electron Langmuir frequency; the other is the electron cyclotron maser
(ECM) radiation mechanism based on the electron cyclotron frequency.
Although these two radiation mechanisms were proposed almost at the same
time, based on the understanding of the coronal environment and the ECM
mechanism at that time, the ECM radiation mechanism did encounter some
difficulties in explaining SRBs. Until 1979, Wu &amp; Lee introduced the
relativistic effect and used the ECM radiation to explain the earth's
Auroral Kilometric Radiation (AKR). Since then, the ECM emission has
attracted wide attention. Considering some difficulties in applying the
ECM emission mechanism to SRBs, we proposed a series of modified models
in recent years. Firstly, the cutoff in the energy spectrum of the
power-law electrons can effectively drive the ECM instability without
relying on the anisotropic distribution of electron velocity. Secondly,
considering the influence of Alfvn wave perturbations which are
prevalent in space and celestial plasmas, a self-consistent ECM emission
mechanism excited by energetic electron beams is developed. On this
basis, this paper summarizes the application of the ECM emission
mechanism in traditional SRB phenomena from type I to V and microwave
SRBs in recent years.</description>
</item>
<item>
<title> The Calibration of the 35-40 GHz Solar Radio Spectrometer with the New Moon and a Noise Source</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJS..268...45S</link>
<description>Calibrating solar radio flux has always been a concern in the solar
community. Previously, fluxes were calibrated by matching load or the
new Moon for relative calibration, and at times with the assistance of
other stations' data. Moreover, the frequency coverage seldom exceeded
26 GHz. This paper reports the upgraded and calibrated Chashan Broadband
Solar millimeter spectrometer (CBS) working from 35 to 40 GHz at the
Chashan Solar Observatory (CSO). Initially, the calibration of the solar
radiation brightness temperature is accomplished using the new Moon as
the definitive source. Subsequently, the 35-40 GHz standard flux is
achieved by establishing the correlation between the solar radio flux,
brightness temperature, and frequency. Finally, the calibration of the
solar radio flux is implemented by utilizing a constant temperature-
controlled noise source as a reference. The calibration in 2023 February
and March reveals that the solar brightness temperature is 11,636 K at
37.25 GHz with a standard deviation (STD) of 652 K. The solar radio
flux's intensity is ~3000-4000 solar flux units (SFU) in the range of
35-40 GHz with a consistency bias of 5.3%. The system sensitivity is
about ~5-8 SFU by a rough evaluation, a noise factor of about 200 K, and
the coefficient of variation of the system transmission slope of 6.5% @
12 hr at 37.25 GHz. It is expected that the upgraded CBS will capture
more activity during the upcoming solar cycle.</description>
</item>
<item>
<title> An Anisotropic Density Turbulence Model from the Sun to 1 au Derived from Radio Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...956..112K</link>
<description>Solar radio bursts are strongly affected by radio-wave scattering on
density inhomogeneities, changing their observed time characteristics,
sizes, and positions. The same turbulence causes angular broadening and
scintillation of galactic and extragalactic compact radio sources
observed through the solar atmosphere. Using large-scale simulations of
radio-wave transport, the characteristics of anisotropic density
turbulence from 0.1 R &lt;SUB&gt;&lt;/SUB&gt; to 1 au are explored. For the first
time, a profile of heliospheric density fluctuations is deduced that
accounts for the properties of extrasolar radio sources, solar radio
bursts, and in situ density fluctuation measurements in the solar wind
at 1 au. The radial profile of the spectrum-weighted mean wavenumber of
density fluctuations (a quantity proportional to the scattering rate of
radio waves) is found to have a broad maximum at around (4-7) R
&lt;SUB&gt;&lt;/SUB&gt;, where the slow solar wind becomes supersonic. The level of
density fluctuations at the inner scale (which is consistent with the
proton resonance scale) decreases with heliocentric distance as $\langle
\delta {{n}_{i}}^{2}\rangle (r)\simeq 2\times
{10}^{7}\,{\left(r/{R}_{\odot }-1\right)}^{-3.7}$ cm&lt;SUP&gt;-6&lt;/SUP&gt;. Due
to scattering, the apparent positions of solar burst sources observed at
frequencies between 0.1 and 300 MHz are computed to be essentially
cospatial and to have comparable sizes, for both fundamental and
harmonic emission. Anisotropic scattering is found to account for the
shortest solar radio burst decay times observed, and the required
wavenumber anisotropy is q &lt;SUB&gt;&lt;/SUB&gt;/q &lt;SUB&gt;&lt;/SUB&gt; = 0.25-0.4,
depending on whether fundamental or harmonic emission is involved. The
deduced radio-wave scattering rate paves the way to quantify intrinsic
solar radio burst characteristics.</description>
</item>
<item>
<title> X-Ray Flares to Energetic (E &gt; 10 MeV) Particle Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...956...24K</link>
<description>Energetic particle environments are an important factor for the
viability of life on exoplanets surrounding flare stars. In the
heliosphere, large gradual solar energetic (E &gt; 10 MeV) particle (SEP)
events are produced by shocks from fast coronal mass ejections (CMEs).
Extensive observations of solar X-ray flares, CMEs, and SEP events can
provide guidance for flare star models of stellar energetic particle
(StEP) events, for which stellar flares, but only rarely the associated
CMEs, are observed. Comparing an extensive list of peak fluxes,
timescales, and peak temperatures of 585  M3.0 solar X-ray flares with
the occurrence of associated SEP events of peak flux Ip &gt; 1.4 proton
flux units, enhanced with proxy decametric-hectometric type II radio
bursts, we determine guidelines for StEP event outcomes, given only
stellar X-ray flare inputs. Longer timescales and lower peak
temperatures of X-ray flares with a given peak X-ray flux Fp are more
favorable for occurrence of associated SEP/StEP events, which, however,
are only a minority of all solar flare outcomes. Most solar flares do
not result in SEP events, invalidating scaling laws between stellar
flares, CMEs, and StEP events. We discuss recent observations and models
of the flare-CME relationship and suggest that StEP intensities Ip may
often be overestimated.</description>
</item>
<item>
<title> Characteristics of the Accelerated Electrons Moving along the Loop Derived from Cyclical Microwave Brightenings at the Footpoints</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...955L..39M</link>
<description>Many particles are accelerated during solar flares. To understand the
acceleration and propagation processes of electrons, we require the
pitch-angle distributions of the particles. The pitch angle of
accelerated electrons has been estimated from the propagation velocity
of a nonthermal microwave source archived in Nobeyama Radioheliograph
data. We analyzed a flare event (an M-class flare on 2014 October 22)
showing cyclical microwave brightenings at the two footpoint regions.
Assuming that the brightenings were caused by the accelerated electrons,
we approximated the velocity parallel to the magnetic field of the
accelerated electrons as ~7.7  10&lt;SUP&gt;4&lt;/SUP&gt; and 9.0  10&lt;SUP&gt;4&lt;/SUP&gt;
km s &lt;SUP&gt;-1&lt;/SUP&gt;. The estimated pitch angle of the accelerated
electrons is 69-80 and the size of the loss cone at the footpoint
(estimated from the magnetic field strength in the nonlinear force-free
field model) is approximately 43. Most of the accelerated electrons
could be reflected at the footpoint region. This feature can be
interpreted as brightenings produced by bouncing motion of the
accelerated electrons.</description>
</item>
<item>
<title> A novel short-term radio flux trend prediction model based on deep learning</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ap&amp;SS.368...87Z</link>
<description>Solar radio flux is an important indicator of solar activity and solar
UV burst. Accurate prediction of solar radio flux plays a crucial role
in preventing and mitigating the impact of solar activity on human
productivity. We propose a novel approach for the first time to predict
short-term radio flux trends using a bidirectional long short-term
memory (BLSTM) network. This approach aims to address the unique
characteristics of temporality and nonlinearity observed in solar radio
flux data. Our model takes into account various frequency
characteristics that impact radio flux. This allows it to learn temporal
patterns within the data, ultimately enabling accurate predictions of
radio flux for the next 30 minutes. The proposed method is
experimentally applied to the radio flux dataset of the US Radio Solar
Telescope Network (RSTN). The results show that, in most frequency
bands, the BLSTM model exhibits superior prediction accuracy and greater
sensitivity to peak responses compared to the LSTM model, LSTM-Attention
(LSTM-A) model, BLSTM-Attention (BLSTM-A) model, and persistence model
(PM). Consequently, the BLSTM model is better equipped to accurately
forecast changes in radio flux for the next 30 minutes.</description>
</item>
<item>
<title> Solar source longitudinal dependence of SEPs and their association with solar flares and radio-loud CMEs</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ap&amp;SS.368...83P</link>
<description>In this article we examine the occurrence probability of 104 major (Ip,
at energies &gt; 10 MeV) solar energetic particle events (SEPs) and their
peak intensity dependence on source longitude and on the characteristics
of solar flares/radio-loud (RL) coronal mass ejections (CMEs) during the
period November 1997December 2014. We classified them into three sets
of events based on the source longitude (L) of the associated solar
flares: i) eastern side events (30E &lt; L  90E), ii) disk center (30E
 L  30W), and iii) western side events (30W &lt; L  90W). On average,
the mean rise time and duration of SEPs are significantly larger for
eastern side events (2168 min and 4.16 days, respectively) than the disk
center (1338 min and 2.65 days, respectively) and western side events
(662 min and 2.42 days, respectively). The mean peak intensity of SEPs
from the disk center (10&lt;SUP&gt;3.56&lt;/SUP&gt; pfu) is found to be greater than
that of SEPs from the western (10&lt;SUP&gt;2.88&lt;/SUP&gt; pfu) and eastern
(10&lt;SUP&gt;2.53&lt;/SUP&gt; pfu) sides, respectively. The western side events
(54%) have significantly higher occurrence probability than the disk
center (34%) and eastern side (12%). While there is no significant
difference in most of the properties of solar flares and RL CMEs, the
eastern side associated RL CMEs are highly decelerated (29.37 m
s&lt;SUP&gt;2&lt;/SUP&gt;) than the disk center (17.44 m s&lt;SUP&gt;2&lt;/SUP&gt;) and
western side (9.09 m s&lt;SUP&gt;2&lt;/SUP&gt;) events. The relationship between
peak intensity of SEPs and peak flux of solar flares shows that the
correlation coefficients (cc) decrease from the eastern side to the
western side: 0.65 (eastern), 0.51 (disk), and 0.35 (western).
Interestingly, we found that there is a good correlation between the
peak intensity of major SEPs and the speed of the CMEs (cc=0.75) for
disk center. From this study, we have concluded that gradualness depends
on source longitude and increases from western to eastern side. It is
also inferred that the relationship of peak intensity of SEP events with
solar flare flux/CME speed is strongly dependent on source longitude.</description>
</item>
<item>
<title> Understanding the radio emission from  Eridani</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...678A.185R</link>
<description>Some solar-type stars are known to present faint, time-variable radio
continuum emission whose nature is not clearly established. We report on
Jansky Very Large Array observations of the nearby star  Eridani at
10.0 and 33.0 GHz. We find that this star has flux density variations on
scales down to days, hours, and minutes. On 2020 April 15 it exhibited a
radio pulse at 10.0 GHz with a total duration of about 20 min and a peak
four times larger than the plateau of 40 Jy present in that epoch. We
were able to model the time behavior of this radio pulse in terms of the
radiation from shocks ramming into the stellar wind. Such shocks can be
produced by the wind interaction of violently expanding gas heated
suddenly by energetic electrons from a stellar flare, similar to the
observed solar flares. Because of the large temperature needed in the
working surface to produce the observed emission, this has to be
nonthermal. It could be gyrosynchrotron or synchrotron emission.
Unfortunately, the spectral index or polarization measurements from the
radio pulse do not have a high enough signal-to-noise ratio to allow us
to determine its nature.</description>
</item>
<item>
<title> ARTEMIS-IV/JLS and NRH Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..442A</link>
<description>Radio bursts provide important diagnostics of energetic phenomena of the
Sun. In particular, bursts in decimetric and metric wavelengths probe
the physical conditions and the energy release processes in the low
corona as well as their association with heliospheric phenomena. The
advent of spectral radio data with high time and high frequency
resolution has provided a wealth of information on phenomena of short
duration and narrow bandwidth. Of particular value are spectral data
combined with imaging observations at specific frequencies. In this work
we briefly review the results of a series of observations comprised from
high-sensitivity, low-noise dynamic spectra obtained with the acousto-
optic analyzer (SAO) of the ARTEMIS-IV/JLS solar radiospectrograph, in
conjunction with high time-resolution images from the Nanay
Radioheliograph (NRH). Our studies include fine structures embedded in
type-IV burst continua (mostly narrow-band "spikes" and intermediate
drift "fiber" bursts) and spike-like structures detected near the front
of type-II bursts. The implications of the observational results to
theoretical models are discussed.</description>
</item>
<item>
<title> Release Episodes of Electrons and Protons in Solar Energetic Particle Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..432K</link>
<description>We analyzed a sample of 21 solar energetic particle (SEP) events with
clear signatures in both near-relativistic electrons and high-energy
protons spanning over 2.5 solar cycles from 1997 to 2016. We employed
velocity dispersion analysis (VDA) for protons and fractional VDA (FVDA)
for electrons, as well as time shifting analysis (TSA) in order to
identify the solar release times (SRTs) of the electrons. We found that,
for the majority of the events (62%), a simultaneous release was
observed, while, for 14% of the events, electrons were released later
than protons (i.e., delayed electrons); for 24% of the events, the
opposite result was found (i.e., delayed protons). We found that the
path length (L) traveled by the protons and electrons was not related to
the aforementioned categorization. Moreover, we show that, in the case
of simultaneous SEP events, protons and electrons are being released in
close connection to type III and type II bursts, while the opposite is
the case for delayed events. In addition, we demonstrate that, for the
simultaneous events, both the proton and the electron release are
established in heights &lt; 5RS and that, especially for the well-connected
simultaneous events, there is a co-occurrence of the type II burst with
the release time of the particles.</description>
</item>
<item>
<title> Statistical analysis of microflares as observed by the 48 GHz spectropolarimeter</title>
<link>https://ui.adsabs.harvard.edu/abs/2023STP.....9c.102Z</link>
<description>Radio observations of weak events are one of the promising methods for
studying energy release and non-thermal processes in the solar corona.
The development of instrumental capabilities allows for radio
observations of weak transient coronal events, such as quasi-stationary
brightenings and weak flares of X-ray class B and below, which were
previously inaccessible for analysis. We have measured the spectral
parameters of microwave radiation for thirty weak solar flares with
X-ray classes ranging from A to C1.5, using observations from the Badary
Broadband Microwave Spectropolarimeter (BBMS). The spectra indicate that
plasma heating is caused by the appearance of non-thermal electron
fluxes, which can be detected by bursts of microwave radiation,
predominantly with an amplitude ~56 solar flux units (SFU) at 45 GHz
frequencies. One solar flux unit (SFU) of radio emission is equal to
1022 W/(mHz). The range of low-frequency spectrum growth indices f
varies widely from =0.3 to 15. The distribution of high-frequency decay
indices is similar to the distributions of regular flares. One of the
explanations for the appearance of large f values is the Razin effect,
which can influence the shape of the gyrosynchrotron spectrum during the
generation of bursts in dense plasma under relatively weak magnetic
fields. We have detected two events in which the appearance of non-
thermal electrons led to the generation of narrowband bursts at
frequencies near the double plasma frequency. SRH test trials have shown
the potential for measuring the structure of flare sources with fluxes
of the order of 1 SFU, indicating the high diagnostic potential of the
radioheliograph for detecting acceleration processes in weak flare
events and their localization in active regions.</description>
</item>
<item>
<title> applications and comparison</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RLSFN..34..663P</link>
<description>Solar activity affects the heliosphere in different ways. Variations in
particles and radiation that impact the Earth's atmosphere, climate, and
human activities often in disruptive ways. Consequently, the ability to
forecast solar activity across different temporal scales is gaining
increasing significance. In this study, we present predictions for solar
cycle 25 of three solar activity indicators: the core-to-wing ratio of
Mg II at 280 nm, the solar radio flux at 10.7 cmwidely recognized
proxies for solar UV emissionand the total solar irradiance, a natural
driver of Earth's climate. Our predictions show a very good agreement
with measurements of these activity indicators acquired during the
ascending phase of solar cycle 25, representing the most recent data
available at the time of writing.</description>
</item>
<item>
<title> Solar radio observations in Trieste contributed to avert a nuclear war in 1967</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MmSAI..94b..40M</link>
<description>Solar Radio Astronomy was started in Trieste by Margherita Hack in the
second half of the Sixties as an innovative and young field of research.
After the declassification in 2016, the science community could learn
that the solar radio astronomical observations at 239 MHz carried out in
May 1967 at the Trieste Astronomical Observatory helped to avert a
nuclear war. This was an ante litteram SpaceWeather application relevant
to the importance of Solar Radio Weather monitoring to detect potential
radio frequency interferences with radio communications. In this work,
we describe the solar radio event that was about to start a nuclear war
by emphasising the role played by the Trieste radio observations in
contributing to the correct scientific interpretation of the strong
radio interferences su ered by the US Ballistic Missile EarlyWarning
System radars in 1967, i.e., that they were of natural origin and not
due to a malicious action of an adversary. This event marked the
beginning of Solar Radio Weather operations in Trieste thanks to the
open mind of Margherita Hack, and made it possible for the solar radio
emission monitoring in Trieste to gain the scientific and applied role
recognised worldwide.</description>
</item>
<item>
<title> The Effect of Solar Flares on HF Radio Communications over Turkey</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..642Y</link>
<description>This study investigates the effect of solar flares on absorption of high
frequency (HF) radio signals over Turkey. For this purpose, the highest
affected frequency (HAF) values by 1 dB absorption due to solar Xray
flux over Turkey were analyzed for different phases of solar flare,
different local times (LT), different solar flare classes and different
days. The HAF and HAF values were calculated from an empirical model
using X-ray flux data with 1-min resolution measured by the
Geostationary Operational Environmental Satellite-15 (GOES-15) and solar
zenith angle data. The increase in X-ray flux density during the
ascending phase of the solar flare causes a sudden and large increase in
HAF values. During this phase of flare, the HAF has a logarithmic
relationship with X-ray flux values. The HAF reaches its maximum values
at the solar flare peak. During the descending phase of solar flare, the
HAF values gradually decrease as X-ray flux density decrease. The local
time has a significant effect on HF absorption. The greatest increase in
HAF values occurs around noon. Comparisons between solar flare classes
show that the HAF values increases significantly as the solar flare
density increases. For different days of year, the value of HAF
increases with decreasing solar zenith angles and the mean HAF has a
linear relationship with the values of mean solar zenith angle. The
results of this study are important because it is the first attempt to
examine the effect of solar flares on HF absorption over Turkey.</description>
</item>
<item>
<title> The Flare Emission of the May 4, 2022 Event and Its Millimeter Component</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..527S</link>
<description>Based on observations at the RT-7.5 radio telescope of the Bauman Moscow
State Technical University at a wavelength of 3.2 mm (93 GHz), along
with other ground-based and space instruments (Siberian Radioheliograph,
Solar Dynamics Observatory (SDO), Metshovi Radio Observatory), the
origin of millimeter radiation from X-ray class M 5.7
SOL2022-05-04T08:45 solar flare was investigated. An analysis of the
time profiles of radiation in the X-ray and radio ranges showed that the
millimeter emission source is not associated with hot (5 
10&lt;SUP&gt;5&lt;/SUP&gt;10&lt;SUP&gt;7&lt;/SUP&gt; K) coronal plasma. This is also evidenced
by the estimate of the sub-THz flux from radiating hot plasma according
to the AIA/SDO data, which turned out to be much less than the observed
values. Indications of the development of thermal instability in flare
ultraviolet loops were obtained. The relationship between the millimeter
emission of the flare and the heat source in the solar chromosphere has
been substantiated.</description>
</item>
<item>
<title> A New 6-15 GHz Solar Radio Observation System</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJS..268...27Z</link>
<description>In this study, we have developed a centimeter-band solar radio telescope
covering the 6-15 GHz frequency band. The radio telescope has the
outstanding advantages of a large instantaneous sampling bandwidth and
wide frequency coverage. As a new solar radio telescope, its time
resolution reaches a very high level of 0.26 ms at a frequency
resolution of 3 MHz, which is very conducive to observing the fine
structure of radio burst signals. In terms of the structure design, the
system employs a 3 m diameter parabolic antenna to receive solar radio
signals. The antenna has high gain and good directivity, and the
pointing accuracy reaches 0.02, which ensures the ability to accurately
track the Sun in real time. In the analog signal processing module, the
combination of radio frequency direct acquisition and down conversion is
used to reduce the interference caused by multiple spectrum shifts.
Regarding the digital receiver, a digital receiving module with high
sampling rate and acquisition resolution is used for data acquisition
and processing, which ensures that the observation system can obtain
observation data with high time and frequency resolutions and real-time
data processing. During the trial operation of the system, solar radio
bursts have been observed many times, and these observations have been
supported by similar international observation equipment. According to a
data comparison, the data obtained by our observation system are more
precise. At present, equipment calibration methods are being improved
and constructed to obtain more accurate observation data.</description>
</item>
<item>
<title> Fundamental-Harmonic Pairs of Interplanetary Type III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...955L..20J</link>
<description>Type III radio bursts are not only the most intense but also the most
frequently observed solar radio bursts. However, a number of their
defining features remain poorly understood. Observational limitations,
such as a lack of sufficient spectral and temporal resolution, have
hindered a full comprehension of the emission process, especially in the
hectokilometric wavelengths. Of particular difficulty is the ability to
detect the harmonics of type III radio bursts. Here we report the first
detailed observations of type III fundamental-harmonic pairs in the
hectokilometric wavelengths, observed by the Parker Solar Probe. We
present a statistical analysis of the spectral characteristics and
polarization measurements of the fundamental-harmonic pairs.
Additionally, we quantify various characteristics of the fundamental-
harmonic pairs, such as the time delay and time profile asymmetry. Our
report concludes that fundamental-harmonic pairs constitute a majority
of all type III radio bursts observed during close encounters when the
probe is in close proximity to the source region and propagation effects
are less pronounced.</description>
</item>
<item>
<title> Cold Solar Flares. I. Microwave Domain</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...954..122L</link>
<description>We identify a set of ~100 "cold" solar flares and perform a statistical
analysis of them in the microwave range. Cold flares are characterized
by a weak thermal response relative to nonthermal emission. This work is
a follow-up of a previous statistical study of cold flares, which
focused on hard X-ray emission to quantify the flare nonthermal
component. Here, we focus on the microwave emission. The thermal
response is evaluated by the soft X-ray emission measured by the GOES
X-ray sensors. We obtain spectral parameters of the flare
gyrosynchrotron emission and reveal patterns of their temporal
evolution. The main results of the previous statistical study are
confirmed: as compared to a "mean" flare, the cold flares have shorter
durations, higher spectral peak frequencies, and harder spectral indices
above the spectral peak. Nonetheless, there are some cold flares with
moderate and low peak frequencies. In the majority of cold flares, we
find evidence of the Razin effect in the microwave spectra, indicative
of rather dense flaring loops. We discuss the results in the context of
the electron acceleration efficiency.</description>
</item>
<item>
<title> Suprathermal Electron Transport and Electron Beam Formation in the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...954...43T</link>
<description>Electron beams that are commonly observed in the corona were discovered
to be associated with solar flares. These "coronal" electron beams are
found 300 Mm above the acceleration region and have velocities ranging
from 0.1c up to 0.6c. However, the mechanism for producing these beams
remains unclear. In this paper, we use kinetic transport theory to
investigate how isotropic suprathermal energetic electrons escaping from
the acceleration region of flares are transported upwardly along the
magnetic field lines of flares to develop coronal electron beams. We
find that magnetic focusing can suppress the diffusion of Coulomb
collisions and background turbulence and sharply collimate the
suprathermal electron distribution into beams with the observed velocity
within the observed distance. A higher bulk velocity is produced if
energetic electrons have harder energy spectra or travel along a more
rapidly expanding coronal magnetic field. By modeling the observed
velocity and location distributions of coronal electron beams, we
predict that the temperature of acceleration regions ranges from 5 
10&lt;SUP&gt;6&lt;/SUP&gt; to 2  10&lt;SUP&gt;7&lt;/SUP&gt; K. Our model also indicates that
the acceleration region may have a boundary where the temperature
abruptly decreases so that the electron beam velocity can become more
than triple (even up to 10 times) the background thermal velocity and
produce the coronal type III radio bursts.</description>
</item>
<item>
<title> An Unsupervised Machine Learning-based Algorithm for Detecting Weak Impulsive Narrowband Quiet Sun Emissions and Characterizing Their Morphology</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...954...39B</link>
<description>The solar corona is extremely dynamic. Every leap in observational
capabilities has been accompanied by unexpected revelations of complex
dynamic processes. The ever more sensitive instruments now allow us to
probe events with increasingly weaker energetics. A recent leap in the
low-frequency radio solar imaging ability has led to the discovery of a
new class of emissions, namely weak impulsive narrowband quiet Sun
emissions (WINQSEs). They are hypothesized to be the radio signatures of
coronal nanoflares and could potentially have a bearing on the long
standing coronal heating problem. In view of the significance of this
discovery, this work has been followed up by multiple independent
studies. These include detecting WINQSEs in multiple data sets, using
independent detection techniques and software pipelines, and looking for
their counterparts at other wavelengths. This work focuses on
investigating morphological properties of WINQSEs and also improves upon
the methodology used for detecting WINQSEs in earlier works. We present
a machine learning-based algorithm to detect WINQSEs, classify them
based on their morphology, and model the isolated ones using 2D
Gaussians. We subject multiple data sets to this algorithm to test its
veracity. Interestingly, despite the expectations of their arising from
intrinsically compact sources, WINQSEs tend to be resolved in our
observations. We propose that this angular broadening arises due to
coronal scattering. Hence, WINQSEs can provide ubiquitous and ever-
present diagnostic of coronal scattering (and, in turn, coronal
turbulence) in the quiet Sun regions, which has not been possible until
date.</description>
</item>
<item>
<title> The Solar Origin of an In Situ Type III Radio Burst Event</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...954...32W</link>
<description>Solar type III radio bursts are generated by beams of energetic
electrons that travel along open magnetic field lines through the corona
and into interplanetary space. However, understanding the source of
these electrons and how they escape into interplanetary space remains an
outstanding topic. Here we report multi-instrument, multiperspective
observations of an interplanetary type III radio burst event shortly
after the second perihelion of the Parker Solar Probe (PSP). This event
was associated with a solar jet that produced an impulsive microwave
burst event recorded by the Expanded Owens Valley Solar Array. The type
III burst event also coincided with the detection of enhanced in situ
energetic electrons recorded by both PSP at 0.37 au and WIND at 1 au,
which were located very closely on the Parker spiral longitudinally. The
close timing association and magnetic connectivity suggest that the in
situ energetic electrons originated from the jet's magnetic reconnection
region. Intriguingly, microwave imaging spectroscopy results suggest
that the escaping energetic electrons were injected into a large opening
angle of about 90, which is at least nine times broader than the
apparent width of the jet spire. Our findings provide an interpretation
for the previously reported, longitudinally broad spatial distribution
of flare locations associated with prompt energetic electron events and
have important implications for understanding the origin and
distribution of energetic electrons in interplanetary space.</description>
</item>
<item>
<title> Turbulence in Sources of Decimetric Flare Continua</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298...95K</link>
<description>Decimetric continua are commonly observed during long-lasting solar
flares. Their frequency boundaries vary with time. We studied frequency
boundary variations using the power spectrum analysis. Analyzing five
decimetric continua, we found that their power spectra have a power-law
form with the power-law index close to the Kolmogorov turbulence index
-5/3. The same power index was also found in the power spectra of radio
flux variations at frequencies in the range of the frequency boundary
variations. Moreover, these frequency boundary variations were highly
correlated with the radio flux ones. We interpret these results to be
due to turbulent density variations in the reconnection plasma outflow
to the termination shock formed above flare loops. In three cases of
decimetric continua, we estimated the level of the plasma density
turbulence to be 7.6 - 11.2% of the mean plasma density. We think that
the analysis of variations of decimetric continua can be used in studies
of the plasma turbulence in solar flares.</description>
</item>
<item>
<title> Decametric Solar Radio Spectrometer Based on 4-element Beamforming Array and Initial Observational Results</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RAA....23h5003G</link>
<description>The dynamic spectral observation at decametric wavelength is important
to study solar radio physics and space weather. However, the observing
system is difficult to observe with high sensitivity at this band due to
the fact that the system temperature is dominated by the sky background
noise and the antenna is difficult to design with high gain. An
effective solution to improve the sensitivity is constructing an antenna
array based on the beamforming method. Accordingly, we develop a
decametric solar radio spectrometer system based on a 4-element
beamforming array. The system consists of four antennas, an 8-channel
analog receiver and a digital receiver. We use the true time delay to
implement the beamformer and the classical FFT method to perform
spectrum analysis in the digital receiver. Operating at a frequency
range of 25-65 MHz with dual-circular polarizations, the system provides
high resolution dynamic spectrum with spectral resolution of ~12 kHz and
temporal resolution of ~5.3 ms (typical). Tens of solar radio bursts
have been observed successfully during the period of the trial
observation, demonstrating the system's ability to detect fine
structures with high spectral and temporal resolution. In this article,
we present the design, implementation, and initial observational results
of the decametric solar radio spectrometer system in detail.</description>
</item>
<item>
<title> Kappa-distributed electrons</title>
<link>https://ui.adsabs.harvard.edu/abs/2023PhPl...30h2106L</link>
<description>In space plasmas, electron populations exhibit non-equilibrium velocity
distributions with high-energy tails that are reproduced by the Kappa
power-laws and contrast with the Maxwellian distributions often used in
theoretical and numerical analyses. In this work, we investigate typical
electron beam-plasma systems and show the influence of Kappa tails on
the linear dispersion and stability spectra of Langmuir-beam waves. The
most common scenarios invoke instabilities of Langmuir waves at the
origin of radio emissions in solar flares and interplanetary shocks.
However, the parametric domain of these instabilities is narrow (i.e.,
energetic beams but with very low density, n b / n e  10 - 3), making
their analytical and numerical characterization not straightforward,
while the approximations used may lead to inconclusive results. Here, we
provide exact numerical solutions of the Langmuir-beam mode, which
distinguish from the classical ones (unaffected by the beam), and also
from electron beam modes destabilized by more energetic and/or denser
beams. Langmuir-beam solutions are only slightly modified by the Kappa
distribution of the beam component, due to its very low density.
However, if the main (core) population is Kappa distributed, the
instability of the Langmuir-beam mode is strongly inhibited, if not
suppressed. New analytical solutions are derived taking into account the
more or less resonant involvement of the electron core and beam
populations. As a result, the analytical solutions show an improved
match with the exact solutions, making them applicable in advanced
modeling of weak (weakly nonlinear) turbulence.</description>
</item>
<item>
<title> Operational prediction of solar flares using a transformer-based framework</title>
<link>https://ui.adsabs.harvard.edu/abs/2023NatSR..1313665A</link>
<description>Solar flares are explosions on the Sun. They happen when energy stored
in magnetic fields around solar active regions (ARs) is suddenly
released. Solar flares and accompanied coronal mass ejections are
sources of space weather, which negatively affects a variety of
technologies at or near Earth, ranging from blocking high-frequency
radio waves used for radio communication to degrading power grid
operations. Monitoring and providing early and accurate prediction of
solar flares is therefore crucial for preparedness and disaster risk
management. In this article, we present a transformer-based framework,
named SolarFlareNet, for predicting whether an AR would produce a 
-class flare within the next 24 to 72 h. We consider three  classes,
namely the M5.0 class, the M class and the C class, and build three
transformers separately, each corresponding to a  class. Each
transformer is used to make predictions of its corresponding  -class
flares. The crux of our approach is to model data samples in an AR as
time series and to use transformers to capture the temporal dynamics of
the data samples. Each data sample consists of magnetic parameters taken
from Space-weather HMI Active Region Patches (SHARP) and related data
products. We survey flare events that occurred from May 2010 to December
2022 using the Geostationary Operational Environmental Satellite X-ray
flare catalogs provided by the National Centers for Environmental
Information (NCEI), and build a database of flares with identified ARs
in the NCEI flare catalogs. This flare database is used to construct
labels of the data samples suitable for machine learning. We further
extend the deterministic approach to a calibration-based probabilistic
forecasting method. The SolarFlareNet system is fully operational and is
capable of making near real-time predictions of solar flares on the Web.</description>
</item>
<item>
<title> Dependence of the Annual Asymmetry Local Index for the NmF2 Median on Solar Activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..421D</link>
<description>Based on the medians of the F 2-layer maximum electron concentration NmF
2 for two ionospheric stations, Boulder and Hobart, in 19632013, an
analysis of the dependence of the annual asymmetry local index R at noon
on solar activity has been performed, where the R index is the
January/July ratio of the summary NmF2 concentration for this pair of
stations. Solar activity indices averaged over 81 days are used:
F&lt;SUB&gt;obs&lt;/SUB&gt; is the solar radio emission flux at a wavelength of 10.7
cm measured by ground-based radio telescopes and F&lt;SUB&gt;adj&lt;/SUB&gt; is the
value of F&lt;SUB&gt;obs&lt;/SUB&gt; reduced to a fixed distance from the Sun of one
astronomical unit. It is found that the regression equations that
manifest the NmF2 medians dependence on F&lt;SUB&gt;obs&lt;/SUB&gt; make it possible
to obtain the annual asymmetry index R for a fixed value of
F&lt;SUB&gt;obs&lt;/SUB&gt; with allowance for a substitution of F&lt;SUB&gt;obs&lt;/SUB&gt; by
cF&lt;SUB&gt;obs&lt;/SUB&gt; in these regression equations, the c coefficient is
equal to 1.03 and 0.97 for January and July, respectively. The c = 1
case corresponds to neglecting the annual asymmetry in the
F&lt;SUB&gt;obs&lt;/SUB&gt; index due to the ellipticity of the Earth's orbit. For
the c = 1 version, the R index increases with a solar activity increase
from 1.2 under low activity up to almost 1.4 under high activity. An
additional allowance for the annual asymmetry in F&lt;SUB&gt;obs&lt;/SUB&gt; leads
to an increase in the R index by approximately 0.1 almost independently
of the solar activity level. Apparently, this conclusion is being drawn
for the first time. The F&lt;SUB&gt;adj&lt;/SUB&gt; index also makes it possible to
obtain a correct estimate of the R index, because the annual asymmetry
in the solar radiation flux is indirectly taken into account via the
experimental values of NmF 2.</description>
</item>
<item>
<title> Evidences for Two-Stage Magnetic Reconnection during the Impulsive Phase</title>
<link>https://ui.adsabs.harvard.edu/abs/2023CosRe..61..265S</link>
<description>We present an analysis of the pre-limb eruptive X4.9 solar flare on
February 25, 2014, by means of which we confirm a hypothesis of the two-
stage energy release corresponding to two magnetic reconnection regimes
in the flare impulsive phase. This flare is selected, firstly, because
of its morphological peculiarities suggesting the presence of the two
energy release stages. Secondly, the flare was very suitably located
near the solar limb and it was well-observed by many instruments. We
performed an analysis of multiwavelength observational data of this
flare region to find a connection between changes of the photospheric
magnetic field, morphology of hard and soft X-ray sources, dynamics of
the photospheric optical emission sources, metric radio bursts, and
kinematics of an eruptive structure. The simultaneous usage of the line-
of-sight and vector Helioseismic Magnetic Imager (HMI) magnetograms
allowed us to trace magnetic field changes during the flare impulsive
phase with high temporal resolution. HMI filtergrams allowed to trace
displacement of the photospheric emission sources, associated with the
magnetic reconnection, with very high temporal resolution up to 2 s.
Using all observational results, we argue that the found flare stages
are characterized by the following magnetic reconnection regimes. The
first stage is predominantly characterized by the three-dimensional
zipping reconnection in the strong sheared magnetic field assuming the
tether-cutting geometry. The second stage corresponds to the so-called
"standard" model of eruptive flares with the quasi-two-dimensional
reconnection below the eruptive flux-rope. All observational
peculiarities of these two stages are discussed in details.</description>
</item>
<item>
<title> Observando la cromosfera solar en el infrarrojo</title>
<link>https://ui.adsabs.harvard.edu/abs/2023BAAA...64....1G</link>
<description>The solar chromosphere has historically been studied from spectral lines
in the visible and UV, notably H, CaII, MgII and Ly. Observations at
long UV wavelengths (304, 1600 and 1700 ) from space have been recently
added. However, the chromosphere can also be studied in the infrared
(IR), both in the continuum as in the lines. Studies in this spectral
band, which by definition extends from 1 m to 1 mm, are scarce and
recent, and its advantages having been little explored. In this work we
present a review of what has been done and detail how much can be done
with ground-based instruments. Argentina has a set of unique telescopes
for the observation of the chromosphere, some with more than 20 years of
operation and in process of renovation, others recently installed and
still some in development. The panorama is very encouraging and allows
to anticipate a strong international cooperation with other ground and
space facilities.</description>
</item>
<item>
<title> Acceleration, Transport, Heating, and Energy Budget</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...953..174F</link>
<description>Solar flares are driven by the release of free magnetic energy and its
conversion to other forms of energy-kinetic, thermal, and nonthermal.
Quantification of partitions between these energy components and their
evolution is needed to understand the solar flare phenomenon including
nonthermal particle acceleration, transport, and escape as well as the
thermal plasma heating and cooling. The challenge of remote-sensing
diagnostics is that the data are taken with finite spatial resolution
and suffer from line-of-sight (LOS) ambiguity including cases when
different flaring loops overlap and project one over the other. Here, we
address this challenge by devising a data-constrained evolving 3D model
of a multiloop SOL2014-02-16T064620 solar flare of GOES class C1.5.
Specifically, we employed a 3D magnetic model validated earlier for a
single time frame and extended it to cover the entire flare evolution.
For each time frame we adjusted the distributions of the thermal plasma
and nonthermal electrons in the model so that the observables
synthesized from the model matched the observations. Once the evolving
model had been validated in this way, we computed and investigated the
evolving energy components and other relevant parameters by integrating
over the model volume. This approach removes the LOS ambiguity and
permits us to disentangle contributions from the overlapping loops. It
reveals new facets of electron acceleration and transport as well as of
the heating and cooling of the flare plasma in 3D. We find signatures of
substantial direct heating of the flare plasma not associated with the
energy loss of nonthermal electrons.</description>
</item>
<item>
<title> Fine Structures of Radio Bursts from Flare Star AD Leo with FAST Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...953...65Z</link>
<description>Radio bursts from nearby active M-dwarfs have been frequently reported
and extensively studied in solar or planetary paradigms. Whereas, their
substructures or fine structures remain rarely explored despite their
potential significance in diagnosing the plasma and magnetic field
properties of the star. Such studies in the past have been limited by
the sensitivity of radio telescopes. Here we report the inspiring
results from the high time-resolution observations of a known flare star
AD Leo with the Five-hundred-meter Aperture Spherical radio Telescope.
We detected many radio bursts in the 2 days of observations with fine
structures in the form of numerous millisecond-scale sub-bursts. Sub-
bursts on the first day display stripe-like shapes with nearly uniform
frequency drift rates, which are possibly stellar analogs to Jovian
S-bursts. Sub-bursts on the second day, however, reveal a different
blob-like shape with random occurrence patterns and are akin to solar
radio spikes. The new observational results suggest that the intense
emission from AD Leo is driven by electron cyclotron maser instability,
which may be related to stellar flares or interactions with a planetary
companion.</description>
</item>
<item>
<title> Characterizing the Spectral Structure of Weak Impulsive Narrowband Quiet Sun Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...953....4M</link>
<description>Weak Impulsive Narrowband Quiet Sun Emissions (WINQSEs) are a newly
discovered class of radio emission from the solar corona. These
emissions are characterized by their extremely impulsive, narrowband,
and ubiquitous nature. We have systematically been working on their
detailed characterization, including their strengths, morphologies,
temporal characteristics, energies, etc. This work is the next step in
this series and focuses on the spectral nature of WINQSEs. Given that
their strength is only a few percent of the background solar emission,
we have adopted an extremely conservative approach to reliably identify
WINQSES. Only a handful of WINQSEs meet all of our stringent criteria.
Their flux densities lie in the 20-50 Jy range and they have compact
morphologies. For the first time, we estimate their bandwidths and find
them to be less than 700 kHz, consistent with expectations based on
earlier observations. Interestingly, we also find similarities between
the spectral nature of WINQSEs and the solar radio spikes. This is
consistent with our hypothesis that the WINQSEs are the weaker cousins
of the type III radio bursts and are likely to be the low-frequency
radio counterparts of the nanoflares, originally hypothesized as a
possible explanation for coronal heating.</description>
</item>
<item>
<title> First results</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..72..844M</link>
<description>The newly installed CALLISTO spectrometer, hosted by the Department of
Space Environment, Institute of Basic and Applied Sciences- EJUST,
commenced operation on August 14, 2021. The system contains a cross
dipole long-wavelength array antenna with high sensitivity to monitor
solar radio transients. Its antenna was strategically positioned and
appeared to be in the center of the CALLISTO network of spectrometers.
Moreover, in the northern section of Africa, the Egypt-Alexandria
CALLISTO and ALGERIA-CRAAG stations are the only ones operating. There
are no stations in the West African region, while stations in the
eastern part of Africa are not working. Thus, Egypt- Alexandria station
serves as a reference for other stations within the e-CALLISTO network.
Despite the low solar activity, the instrument detected several solar
radio bursts not limited to type II, type III, and type V. A vigorous
case study was conducted on two selected radio burst events to validate
the authenticity of the recorded events. Other solar radio stations at
different geographical locations recorded all the radio bursts detected
by the spectrometer. The case study included brief analyses that
indicated a type II radio burst observed on October 09, 2021, between
06:30 and 07:00 UT, was associated with an M1.6 solar flare located at
N18E08 within NOAA-AR 2882 and a CME with a shock front speed of  978
km/s. However, the type III radio burst is neither CME nor solar flare
associated. These analyses examine the instrument's capacity to provide
real-time solar radio transient data 24 h a day to mitigate the
challenges of data gaps faced in the African continent. Hence, the
instrument has become an integral part of space weather monitoring and
forecasting over the region and other parts of the globe.</description>
</item>
<item>
<title> New Insights from Imaging Spectroscopy of Solar Radio Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ARA&amp;A..61..427G</link>
<description>Newly available high-resolution imaging of solar radio emission at many
closely spaced frequencies and times provides new physical insight into
the processes, structure, and dynamics of the solar atmosphere. The
observational advances have spurred renewed interest in topics dating
from the early days of solar radio astronomy and have led to
considerable advances in our knowledge. Highlights of recent advances
include the following: Quantitatively measuring the dynamic magnetic
field strength, particle acceleration, and hot thermal plasma at the
heart of solar flares and hinting at the processes that relate them;
Resolving in space and time the energization and transport of electrons
in a wide range of contexts; Mapping the magnetized thermal plasma
structure of the solar chromosphere and corona over a substantial range
of heights in active and quiet regions of the Sun.This review explains
why solar radio imaging spectroscopy is so powerful, describes the body
of recent results, and outlines the future work needed to fully realize
its potential. The application of radio imaging spectroscopy to stars
and planets is also briefly reviewed.</description>
</item>
<item>
<title> Modulation depth of the gyrosynchrotron emission as an identifier of fundamental sausage modes</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...676A...8C</link>
<description>&lt;BR /&gt; Aims: We aim to study the intensity, the modulation depth, and
the mean modulation depth of the gyrosynchrotron (GS) radiation as a
function of the frequency and the line of sight (LOS) in fast sausage
modes. &lt;BR /&gt; Methods: By solving the 2.5D magnetohydrodynamics (MHD)
ideal equations of a straight coronal loop considering the chromosphere
and with typical flaring plasma parameters we analyse the wavelet
transform of the density and the GS emission for different radio
frequencies and different spatial resolutions, given impulsive and
general perturbations with energies in the microflare range. &lt;BR /&gt;
Results: A wavelet analysis performed over the GS radiation emission
showed that a fast fundamental sausage mode of 7 s with a first
harmonic mode of 3 s developed, for all the initial energy perturbations
used. For both the high spatial resolution (central pixel integration)
and the low spatial resolution (entire loop integration), the larger the
radio frequency, the larger the modulation depth. However, high- and
low-resolution integrations differ in that the larger the LOS angle with
respect to the loop axis, the larger and smaller the modulation depth,
respectively. &lt;BR /&gt; Conclusions: Fast MHD modes triggered by
instantaneous energy depositions of the order of a microflare energy are
able to reproduce deep intensity modulation depths in radio emission as
observed in solar events. As the trends of the GS emission previously
obtained for a linear and forced oscillation remain present when
analysing a more general context, considering the chromosphere and where
the sausage mode is triggered by an impulsive, non-linear perturbation,
it seems that the behaviour found can be used as observational
identifiers of the presence of sausage modes with respect to other
quasi-periodic pulsation features. It can be inferred from this that
finite-amplitude sausage modes have the potential to generate the
observed deep modulation depths.</description>
</item>
<item>
<title> A Case Study over Haikou Station</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RemS...15.3394W</link>
<description>This paper introduces a novel technique that uses observation data from
GNSS to estimate the ionospheric vertical total electron content (VTEC)
using the Kriging-Kalman method. The technique provides a method to
validate the accuracy of the Ionospheric VTEC analysis within the
Equatorial Ionization anomaly region. The technique developed uses GNSS
VTEC alongside solar parameters, such as solar radio flux (F10.7 cm),
Disturbance Storm Time (Dst) and other data, and Long Short Term Memory
(LSTM) Networks to predict the occurrence time of the ionospheric
equatorial anomaly and ionospheric VTEC changes. The LSTM method was
applied to GNSS data from Haikou Station. A comparison of this technique
with the neural network (NN) model and International Reference
Ionosphere model shows that the LSTM outperforms all of them at VTEC
estimation and prediction. The results, which are based on the root mean
square error (RMSE) between GNSS VTEC and GIM VTEC outside the
equatorial anomaly region, was 1.42 TECU, and the results of GNSS VTEC
and VTEC from Beidou geostationary orbit satellite, which lies inside
the equatorial ionization anomaly region, was 1.92 TECU. The method
developed can be used in VTEC prediction and estimation in real time
space operations.</description>
</item>
<item>
<title> The investigation of a portable solar telescope with a high gain metamaterial antenna for F10.7 radio flux measurement</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RScI...94g4708Z</link>
<description>A high gain and high aperture efficiency metamaterial (MTM) antenna is
applied to a solar telescope in this paper. First, a portable solar
telescope including the MTM antenna and a receiving system is presented.
Next, the theory of the MTM antenna is proposed and analyzed based on
the ray-tracing model. The designed MTM antenna is composed of a dual
circularly polarized Fabry-Prot resonant antenna (FPRA) and four phase
correction metasurfaces (PCMs). The proposed PCMs act as the reflection
surface and the phase correction surface at the same time. Every PCM
consists of 2  18 optimized artificial magnetic conductor (AMC) units.
To solve the parallel incidence and narrow bandwidth problems of AMC
units, a nonuniform partially reflective surface is designed. Compared
with traditional FPRA, the proposed MTM antenna has an increase in peak
gain of 37.5% and an aperture efficiency of 11.4%. Then, a receiving
system composed of the receiver, equatorial mount, data acquisition
module, and display module is presented for solar radio signal
processing. Finally, the designed MTM antenna and solar telescope are
simulated and measured. A good agreement between the simulation and
measurement is observed and can be used to verify this design.</description>
</item>
<item>
<title> Predictions of solar activity cycles 25 and 26 using non-linear autoregressive exogenous neural networks</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.523.1175K</link>
<description>This study presents new prediction models of the 11-yr solar activity
cycles (SC) 25 and 26 based on multiple activity indicator parameters.
The developed models are based on the use of non-linear autoregressive
exogenous (NARX) neural network approach. The training period of the
NARX model is from July 1749 to December 2019. The considered activity
indicator parameters are the monthly sunspot number time series (SSN),
the flare occurence frequency, the 10.7-cm solar radio flux, and the
total solar irradiance (TSI). The neural network models are fed by these
parameters independently and the prediction results are compared and
verified. The obtained training, validation, and prediction results show
that our models are accurate with an accuracy of about 90 per cent in
the prediction of peak activity values. The current models produce the
dual-peak maximum (Gnevyshev gap) very well. Based on the obtained
results, the expected solar peaks in terms of SSN (monthly averaged
smoothed) of the solar cycles 25 and 26 are R&lt;SUB&gt;SSN&lt;/SUB&gt; = 116.6
(February 2025) and R&lt;SUB&gt;SSN&lt;/SUB&gt; = 113.25 (October 2036),
respectively. The expected time durations of SC 25 and SC 26 cycles are
9.2 and 11 yr, respectively. The activity levels of SC 25 and 26 are
expected to be very close and similar to or weaker than SC 24. This
suggests that these two cycles are at the minimum level of the
Gleissberg cycle. A comparison with other reported studies shows that
our results based on the NARX model are in good agreement.</description>
</item>
<item>
<title> Investigating the effect of large solar flares on the ionosphere based on novel Digisonde data comparing three different methods</title>
<link>https://ui.adsabs.harvard.edu/abs/2023FrASS..1001625B</link>
<description>Increased solar radiation during solar flare events can cause additional
ionization and enhanced absorption of the electromagnetic (EM) waves in
the ionosphere leading to partial or even total radio fade-outs. In this
study, the ionospheric response to large solar flares has been
investigated using the ionosonde data from Juliusruh (54.63 N, 13.37
E), Prhonice (49.98 N, 14.55 E) and San Vito (40.6 N, 17.8 E)
Digisonde (DPS-4D) stations. We studied the effect of 13 intense (&gt;C4.8)
solar flares that occurred between 06:00 and 16:30 (UT, daytime LT =
UT+1 h) from 04 to 10 September 2017 using three different methods. A
novel method based on the amplitude data of the measured EM waves is
used to calculate and investigate the relative absorption changes
(compared to quiet period) occurring during the flares. The amplitude
data are compared with the variation of the fmin parameter (fmin, the
minimum measured frequency, it is considered as a qualitative proxy for
the "non-deviative" radio wave absorption). Furthermore, the signal-to-
noise ratio (SNR) measured by the Digisondes was used as well to
quantify and characterize the fade-out events and the ionospheric
absorption. In order to compare the three different methods, residuals
have been defined for all parameters, which provide the percentage
changes compared to the selected reference periods. Total and partial
radio fade-outs, increased values (+0.4%318%) of the fmin parameter,
and +20%1400% amplitude changes (measured at 2.5 and 4 MHz) were
experienced during and after the investigated flares. Generally, the
observed changes depended on the intensity, solar zenith angle and
duration of the flare events. Although the three different methods have
their own advantages/disadvantages and their limitations, the
combination of them seems to be an efficient approach to monitor the
ionospheric response to solar flares.</description>
</item>
<item>
<title> Research Progress of the Heliospheric Radio Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChA&amp;A..47..536C</link>
<description>The heliospheric radio emissions are the strongest radio emissions
phenomenon in the solar system, with a radiation power of at least
10&lt;SUP&gt;13&lt;/SUP&gt; W, which can provide important physical information of
high energy electron beam and magnetic plasma structure near the
heliospheric boundary. Since the first detection by the Voyager
spacecraft in 1983, those radio emissions have widely and continuously
attracted much attention from researchers. There are generally two types
of the heliospheric radio emissions: instantaneous or drifting emission
with relatively high frequency, and continuous emission or non-drifting
emission with relatively low frequency. Usually, both types of emissions
start from about 2 kHz. For the drifting emission, it has the
characteristic of drifting toward high frequency, the drifting rate is
about 1-3 kHz/yr, the frequency range is 1.8-3.6 kHz, and the duration
is about 100-300 days. For the non-drifting emission, it has no obvious
frequency drift, the frequency range is 1.8-2.6 kHz, and the duration is
about 3 yr. It is generally believed that the heliospheric radio
emissions are related to shock. In this paper, the possible source
region of the radio emissions, the emission mechanisms, and the source
of shock related to the emissions are introduced. Furthermore, the
existing scientific problems and the future perspectives on the research
of heliospheric radio emissions are discussed.</description>
</item>
<item>
<title> Study of Solar Flares in Centimeter Range by Dynamical Methods</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AzAJ...18a..54H</link>
<description>The article investigates oscillatory processes in solar flares based on
observational data obtained by a 12-meter radio telescope at a frequency
f=3 GHz belonging to the Ionosphere Institute of the Kazakhstan
Republic. The results of a brief review of methods for processing non-
stationary time series suggest that the requirement of adaptability is
also important. It is shown that this possibility is provided by the
method proposed by Norden Huang. For clarity, the method of implementing
EMD (Empirical Mode Decomposition) - the method of decomposing signals
into functions (modes) will be considered using the example of a digital
signal array x(t). In order to obtain more realistic results, the type
of series was determined using fractal analysis. It is shown that at
this stage, for the reliability of obtaining quasi-periodic pulsations
(QPPs), it is necessary to carry out visual control and compare the
results obtained by different methods</description>
</item>
<item>
<title> A Two-element Interferometer for Millimeter-wave Solar Flare Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJS..267...14Y</link>
<description>In this paper, we present the design and implementation of a two-element
interferometer operating in the millimeter-wave band (39.5-40 GHz) for
observing solar radio emissions through nulling interference. The system
is composed of two 50 cm aperture Cassegrain antennas installed on a
common equatorial mount, with a separation of 230 wavelengths. The
cross-correlation of the received signals effectively cancels out the
quiet solar component of the high flux density (~3000 sfu) that reduces
the detection limit due to atmospheric fluctuations. The system
performance is as follows: the noise factor of the analog front end in
the observation band is less than 2.1 dB, system sensitivity is
approximately 12.4 K (~34 sfu) with an integration time constant of 0.1
ms (default), the frequency resolution is 153 kHz, and the dynamic range
is 30 dB. Through actual testing, the nulling interferometer observes a
quiet Sun with a low level of output fluctuations (up to 50 sfu) and has
a significantly lower radiation flux variability (up to 190 sfu) than an
equivalent single-antenna system, even under thick cloud cover. As a
result, this new design can effectively improve observation sensitivity
by reducing the impact of atmospheric and system fluctuations during
observation.</description>
</item>
<item>
<title> Data-constrained Solar Modeling with GX Simulator</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJS..267....6N</link>
<description>To facilitate the study of solar flares and active regions, we have
created a modeling framework, the freely distributed GX Simulator IDL
package, that combines 3D magnetic and plasma structures with thermal
and nonthermal models of the chromosphere, transition region, and
corona. Its object-based modular architecture, which runs on Windows,
Mac, and Unix/Linux platforms, offers the ability to either import 3D
density and temperature distribution models, or to assign numerically
defined coronal or chromospheric temperatures and densities, or their
distributions, to each individual voxel. GX Simulator can apply
parametric heating models involving average properties of the magnetic
field lines crossing a given voxel, as well as compute and investigate
the spatial and spectral properties of radio, (sub)millimeter, EUV, and
X-ray emissions calculated from the model, and quantitatively compare
them with observations. The package includes a fully automatic model
production pipeline that, based on minimal users input, downloads the
required SDO/HMI vector magnetic field data, performs potential or
nonlinear force-free field extrapolations, populates the magnetic field
skeleton with parameterized heated plasma coronal models that assume
either steady-state or impulsive plasma heating, and generates non-LTE
density and temperature distribution models of the chromosphere that are
constrained by photospheric measurements. The standardized models
produced by this pipeline may be further customized through specialized
IDL scripts, or a set of interactive tools provided by the graphical
user interface. Here, we describe the GX Simulator framework and its
applications.</description>
</item>
<item>
<title> Morphology of Solar Type II Bursts Caused by Shock Propagation through Turbulent and Inhomogeneous Coronal Plasma</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...952...51K</link>
<description>Type II solar bursts are radio signatures of shock waves in the solar
corona driven by solar flares or coronal mass ejections (CMEs).
Therefore, these bursts present complex spectral morphologies in solar
dynamic spectra. Here, we report meter-decameter radio observations of a
type II burst on 2014 July 25 made with the Ukrainian radio telescopes
UTR-2 (8.25-33 MHz) and GURT (8.25-78 MHz). The burst demonstrates
fundamental and harmonic components, band splitting, a herringbone
structure, and a spectral break. These specific spectral features,
observed jointly in a single type II burst, are rarely detected. To
contribute to our understanding of such puzzling type II events, we
carried out a detailed analysis of the recorded type II dynamic
spectrum. In particular, the herringbone pattern has been exploited to
study electron density turbulence in the solar corona. We calculated the
power spectral densities of the flux variations in selected
herringbones. The spectral index is in the range of  = -1.69 to -2.00
with an average value of -1.897, which is slightly higher than the
Kolmogorov spectral index of -5/3 for fully developed turbulence. We
also recognized that the second type II burst consists of three drifting
lanes. The lane onset times coincide with the spectral break in the
first type II burst. We regard that the CME/shock passage through a
streamer caused the spectral break and triggered the multilane type II
radio emission. Thus, we support one of the proposed scenarios for type
II burst occurrence as being the result of CME/shock-streamer
interaction.</description>
</item>
<item>
<title> A 7 Day Multiwavelength Flare Campaign on AU Mic. I. High-time-resolution Light Curves and the Thermal Empirical Neupert Effect</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...951...33T</link>
<description>We present light curves and flares from a 7 day, multiwavelength
observational campaign of AU Mic, a young and active dM1e star with
exoplanets and a debris disk. We report on 73 unique flares between the
X-ray to optical data. We use high-time-resolution near-UV (NUV)
photometry and soft X-ray (SXR) data from the X-ray Multi-Mirror Mission
to study the empirical Neupert effect, which correlates the gradual and
impulsive phase flaring emissions. We find that 65% (30 of 46) flares do
not follow the Neupert effect, which is 3 times more excursions than
seen in solar flares, and propose a four-part Neupert effect
classification (Neupert, quasi-Neupert, non-Neupert types I and II) to
explain the multiwavelength responses. While the SXR emission generally
lags behind the NUV as expected from the chromospheric evaporation flare
models, the Neupert effect is more prevalent in larger, more impulsive
flares. Preliminary flaring rate analysis with X-ray and U-band data
suggests that previously estimated energy ratios hold for a collection
of flares observed over the same time period, but not necessarily for an
individual, multiwavelength flare. These results imply that one model
cannot explain all stellar flares and care should be taken when
extrapolating between wavelength regimes. Future work will expand
wavelength coverage using radio data to constrain the nonthermal
empirical and theoretical Neupert effects to better refine models and
bridge the gap between stellar and solar flare physics.</description>
</item>
<item>
<title> Type II radio bursts and their association with coronal mass ejections in solar cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...675A.102K</link>
<description>Context. Meter-wavelength type II solar radio bursts are thought to be
the signatures of shock-accelerated electrons in the corona. Studying
these bursts can give information about the initial kinematics,
dynamics, and energetics of coronal mass ejections (CMEs) in the absence
of white-light observations. &lt;BR /&gt; Aims: We investigate the occurrence
of type II bursts in solar cycles 23 and 24 and their association with
CMEs. We also explore whether type II bursts might occur in the absence
of a CME. &lt;BR /&gt; Methods: We performed a statistical analysis of type II
bursts that occurred between 200 and 25 MHz in solar cycles 23 and 24
and determined the temporal association of these radio bursts with CMEs.
We categorized the CMEs based on their linear speed and angular width
and studied the distribution of type II bursts with fast (500 km
s&lt;SUP&gt;1&lt;/SUP&gt;), slow (&lt; 500 km s&lt;SUP&gt;1&lt;/SUP&gt;), wide (60), and narrow
(&lt; 60) CMEs. We explored the dependence of type II bursts occurrence on
the phases of the solar cycle. &lt;BR /&gt; Results: Our analysis shows that
during solar cycles 23 and 24, 768 and 435 type II bursts occurred,
respectively. Of these, 79% were associated with CMEs in solar cycle 23,
and 95% were associated with CMEs in solar cycle 24. However, only 4%
and 3% of the total number of CMEs were accompanied by type II bursts in
solar cycle 23 and 24, respectively. Most of the type II bursts in both
cycles were related to fast and wide CMEs (48%). We also determined the
typical drift rate and duration for type II bursts, which is 0.06 MHz
s&lt;SUP&gt;1&lt;/SUP&gt; and 9 min. Our results suggest that type II bursts
dominate at heights 1.7  2.3  0.3 R&lt;SUB&gt;&lt;/SUB&gt;. A clear majority
have an onset height around 1.7  0.3 R&lt;SUB&gt;&lt;/SUB&gt; assuming the four-
fold Newkirk model. &lt;BR /&gt; Conclusions: The results indicate that most
of the type II bursts had a white-light CME counterpart, but a few type
II bursts lacked a clear CME association. There were more CMEs in cycle
24 than in cycle 23. However, cycle 24 contained fewer type II radio
bursts than cycle 23. The onset heights of type II bursts and their
association with wide CMEs reported in this study indicate that the
early lateral expansion of CMEs may play a key role in the generation of
these radio bursts.</description>
</item>
<item>
<title> A type II solar radio burst without a coronal mass ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...675A..98M</link>
<description>Context. The Sun produces the most powerful explosions in the Solar
System, solar flares, which can also be accompanied by large eruptions
of magnetised plasma, coronal mass ejections (CMEs). These processes can
accelerate electron beams up to relativistic energies through magnetic
reconnection processes during solar flares and CME-driven shocks.
Energetic electron beams can in turn generate radio bursts through the
plasma emission mechanism. CME shocks, in particular, are usually
associated with type II solar radio bursts. &lt;BR /&gt; Aims: However, on a
few occasions, type II bursts have been reported to occur either in the
absence of CMEs or shown to be more likely related with the flaring
process. It is currently an open question as to how a shock generating
type II bursts forms without the occurrence of a CME eruption. Here, we
aim to determine the physical mechanism responsible for a type II burst
that occurs in the absence of a CME. &lt;BR /&gt; Methods: By using radio
imaging from the Nanay Radioheliograph, combined with observations from
the Solar Dynamics Observatory and the Solar Terrestrial Relations
Observatory spacecraft, we investigate the origin of a type II radio
burst that appears to have no temporal association with a white-light
CME. &lt;BR /&gt; Results: We identify a typical type II radio burst with
band-split structure that is associated with a C-class solar flare. The
type II burst source is located above the flaring active region and
ahead of disturbed coronal loops observed in extreme-ultraviolet (EUV)
images. The type II burst is also preceded by type III radio bursts,
some of which are in fact J bursts, indicating that accelerated electron
beams do not all escape along open field lines. The type II sources show
single-frequency movement towards the flaring active region. The type II
burst is located ahead of a faint EUV front propagating through the
corona. &lt;BR /&gt; Conclusions: Since there is no CME detection, a shock
wave is most likely generated by the flaring process or the bulk plasma
motions associated with a failed eruption. The EUV front observed is
likely a freely propagating wave that expands into surrounding regions.
The EUV front propagates at an initial speed of approximately 450 km
s&lt;SUP&gt;1&lt;/SUP&gt; and it is likely to steepen into a shock wave in a region
of low Alfvn speed as determined from magneto-hydrodynamic modelling of
the corona. &lt;P /&gt;Movies are available at &lt;A href="https://www.aanda.org/
10.1051/0004-6361/202245515/olm"&gt;https://www.aanda.org&lt;/A&gt;.</description>
</item>
<item>
<title> Multiple injections of energetic electrons associated with the flare and CME event on 9 October 2021</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...675A..27J</link>
<description>Context. We study the solar energetic particle (SEP) event observed on 9
October 2021 by multiple spacecraft, including Solar Orbiter. The event
was associated with an M1.6 flare, a coronal mass ejection, and a shock
wave. During the event, high-energy protons and electrons were recorded
by multiple instruments located within a narrow longitudinal cone. &lt;BR
/&gt; Aims: An interesting aspect of the event was the multi-stage particle
energisation during the flare impulsive phase and also what appears to
be a separate phase of electron acceleration detected at Solar Orbiter
after the flare maximum. We aim to investigate and identify the multiple
sources of energetic electron acceleration. &lt;BR /&gt; Methods: We utilised
SEP electron observations from the Energetic Particle Detector (EPD) and
hard X-ray (HXR) observations from the Spectrometer/Telescope for
Imaging X-rays (STIX) on board Solar Orbiter, in combination with radio
observations at a broad frequency range. We focused on establishing an
association between the energetic electrons and the different HXR and
radio emissions associated with the multiple acceleration episodes. &lt;BR
/&gt; Results: We find that the flare was able to accelerate electrons for
at least 20 min during the non-thermal phase, observed in the form of
five discrete HXR pulses. We also show evidence that the shock wave
contributed to the electron acceleration during and after the impulsive
flare phase. The detailed analysis of EPD electron data shows that there
was a time difference in the release of low- and high-energy electrons,
with the high-energy release delayed. Also, the observed electron
anisotropy characteristics suggest a different connectivity during the
two phases of acceleration.</description>
</item>
<item>
<title> deARCE Method</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298...82B</link>
<description>We present in detail an automatic radio-burst detection system, based on
the AlexNet convolutional neural network, for use with any kind of solar
spectrogram. A full methodology for model training, performance
evaluation, and feedback to the model generator has been developed with
special emphasis on i) robustness tests against stochastic and
overfitting effects, ii) specific metrics adapted to the unbalanced
nature of the solar-burst scenario, iii) tunable parameters for
probability-threshold optimization, and iv) burst-coincidence cross
match among e-Callisto stations and with external observatories (NOAA-
SWPC). The resulting neural network configuration has been designed to
accept data from observatories other than e-Callisto, either ground- or
spacecraft-based. Typical False Negative and False Positive Scores in
single-observatory mode are, respectively, in the 10 - 16% and 6 - 8%
ranges, which improve further in cross-match mode. This mode includes
new services (deARCE, Xmatch) allowing the end-user to check at a glance
if a solar radio burst has taken place with a high level of confidence.</description>
</item>
<item>
<title> Slowly drifting radio fibres</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.522.1930C</link>
<description>The fine structure in the continuum radiation of type IV solar radio
bursts is very rich in various structures (zebra structure, fibres,
pulsations, spikes, etc.). So far, however, no attention has been paid
to the isolated fibres that occasionally appear in the metre and
decimetre ranges. Here we give and discuss examples of the dynamic
spectra of such bursts obtained many years ago (in the metre waveband
from 1969) as well in recent years (in the decimetre and microwave
wavebands from 2003-2013). Isolated fibres are observed mostly in the
decimetre range (although there are examples in both the metre and
microwave ranges), and they reveal a number of features of classical
fibre bursts. As a generation mechanism for such fibres, the process of
interaction of whistlers with Langmuir plasmons was suggested. An
analysis of conditions for the realization of this process in solar
magnetic arch structures and its efficiency was carried out. Estimates
of the intensity of low-frequency turbulence (whistlers) and magnetic
field strength in the solar corona were obtained using the data of radio
fibres.</description>
</item>
<item>
<title> Jupiter's equatorial X-ray emissions over two solar cycles</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.521.5596W</link>
<description>Jupiter's disc is bright in X-rays as H&lt;SUB&gt;2&lt;/SUB&gt; molecules in the
atmosphere are very effective at scattering solar X-rays. K-shell
fluorescence from carbon atoms in atmospheric methane is thought to also
provide a minor contribution. XMM-Newton has now observed Jupiter over a
span of nearly two solar cycles from 2003 to 2021, offering the
opportunity to determine whether Jupiter's disc emissions are driven by
solar activity or not. We compare the count rates of X-rays of energies
0.2-10.0, 0.2-2.0, 2.1-5.0, and 5.1-10.0 keV from the planet's
equatorial region, with the sunspot number and F&lt;SUB&gt;10.7&lt;/SUB&gt; adjusted
solar radio flux. The respective Pearson's correlation coefficients for
both are 0.88/0.84, 0.86/0.83, 0.40/0.34, and 0.29/0.22 for each energy
demonstrating that the low-energy X-ray disc emissions are indeed
controlled by the Sun's activity. This relationship is less clear for
the higher energy emissions, raising questions around the source of
these emissions.</description>
</item>
<item>
<title> Deciphering Faint Gyrosynchrotron Emission from a Coronal Mass Ejection Using Spectropolarimetric Radio Imaging</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...950..164K</link>
<description>Measurements of the plasma parameters of coronal mass ejections (CMEs),
particularly the magnetic field and nonthermal electron population
entrained in the CME plasma, are crucial to understand their
propagation, evolution, and geo-effectiveness. Spectral modeling of
gyrosynchrotron (GS) emission from CME plasma has been regarded as one
of the most promising remote-sensing techniques for estimating spatially
resolved CME plasma parameters. Imaging the very low flux density CME GS
emission in close proximity to the Sun with orders of magnitude higher
flux density has, however, proven to be rather challenging. This
challenge has only recently been met using the high dynamic range
imaging capability of the Murchison Widefield Array (MWA). Although
routine detection of GS is now within reach, the challenge has shifted
to constraining the large number of free parameters in GS models, a few
of which are degenerate, using the limited number of spectral points at
which the observations are typically available. These degeneracies can
be broken using polarimetric imaging. For the first time, we demonstrate
this using our recently developed capability of high-fidelity
polarimetric imaging on the data from the MWA. We show that
spectropolarimetric imaging, even when only sensitive upper limits on
circularly polarization flux density are available, is not only able to
break the degeneracies but also yields tighter constraints on the plasma
parameters of key interest than possible with total intensity
spectroscopic imaging alone.</description>
</item>
<item>
<title> A Continued Study</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...950...71S</link>
<description>In this paper, we reanalyze the X1.7 class limb flare that occurred on
2013 May 13 (SOL2013-05-13T01:56 UT), concentrating on the energy-
releasing process using microwave observations mainly made by Nobeyama
and X-ray observations made by RHESSI. The analysis was carried out in
the context of EUV observations made by the Atmospheric Imaging Assembly
on board Solar Dynamics Observatory. First, we complement the initiation
process by showing that the initiation occurred together with material
falling from a large-scale overlying prominence, a signature of drainage
instability. The usual downward and upward motions of the microwave and
X-ray sources are observed from their evolution. However, the microwave
source's height shows a recurrent decrease and increase during its
overall upward motion; it shows a kind of recurrent contraction and
expansion. The time period of the recurrent contraction and expansion
corresponds to the period of post-contraction oscillation of EUV loops,
and the oscillatory motions are closely correlated with four
microwave/hard X-ray peaks that unusually increased nonthermal emission
levels by several times. X-ray spectra get hardened during the
oscillation. In addition, the rapid contraction of magnetic loops
located on the outside of the erupting flux rope occurs 5 minutes after
the onset of the flare, showing that the contraction of the peripheral
magnetic loops is more likely due to the vortex and sink flows generated
by an upward erupting magnetic flux rope rather than a coronal
implosion. The results can provide more insight into the physics of
dynamic coronal magnetic field and particle acceleration during solar
flares.</description>
</item>
<item>
<title> Imaging Preflare Broadband Pulsations in the Decimetric-metric Wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...950....2L</link>
<description>Preflare activities contain critical information about the precursors
and causes of solar eruptions. Here we investigate the characteristics
and origin of a group of broadband pulsations (BBPs) in the decimetric-
metric wavelengths that took place during the preflare stage of the M7.1
flare on 2011 September 24. The event was recorded by multiple solar
instruments, including the Nanay Radioheliograh, that measure the
properties of the radio source. The BBPs started ~24 minutes before the
flare onset, extending from &lt;360 to above 800 MHz without a discernible
spectral drift. The BBPs consisted of two stages. During the first
stage, the main source remained stationary, and during the second stage,
it moved outward along with a steepening extreme-ultraviolet (EUV) wave
driven by the eruption of a high-temperature structure. In both stages,
we observe frequent EUV brightenings and jets originating from the flare
region. During the second stage, the BBPs became more frequent and
stronger in general, and the polarization level gradually increased from
&lt;20% to &gt;60% in the right-handed sense. These observations indicate that
the steepening EUV wave is important to the BBPs during the second
stage, while the preflare reconnections causing the jets and EUV
brightenings are important in both stages. This is the first time that
such a strong association of an EUV wave with BBPs is reported. We
suggest a scenario in which reconnection occurs together with a shock
that sweeps across the loops as the cause of the BBPs.</description>
</item>
<item>
<title> Analysis of the Possibilities of Short-Term Prediction of Geomagnetic Perturbations from Observations of Coronal Mass Ejections at the BSA LPI Radio Telescope</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ARep...67..607L</link>
<description>From April 2021 to October 2022, in the monitoring data obtained daily
at the Big Scanning Antenna radio telescope (BSA LPI), 11 events were
identified for which X-ray flares in the solar corona were followed by
magnetic storms on Earth. Interplanetary scintillation monitoring data
were considered together with data on solar flare activity and a simple
kinematic model of ejection propagation. Based on the estimated ejection
velocity between the Sun and the probed region, under the assumption of
a constant velocity, the time of arrival of the ejection to the Earth
was calculated. Of the 11 events considered, 7 are associated with
solitary flares followed by a coronal mass ejection (CME) and 4 are more
complex and possibly associated with corotating perturbations or a
superposition of corotating and flare perturbations. For the entire set
of events, the average time of the real onset of a magnetic storm after
the time predicted by the model was 3.6 h and the average time between
the onset of scintillation enhancement and the onset of a magnetic storm
was 20.1 h. For events associated with solitary flares, the magnetic
storm began, on average, 0.8 hours after the predicted time and 15.6
hours after the onset of scintillation enhancement. The delay of
magnetic storms with respect to the predicted time is apparently related
to the deceleration of the ejection between the probed region of the
solar wind and the Earth's orbit.</description>
</item>
<item>
<title> Langmuir waves associated with magnetic holes in the solar wind</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...674A.220B</link>
<description>Context. Langmuir waves (electrostatic waves near the electron plasma
frequency) are often observed in the solar wind and may play a role in
the energy dissipation of electrons. The largest amplitude Langmuir
waves are typically associated with type II and III solar radio bursts
and planetary foreshocks. In addition, Langmuir waves not related to
radio bursts occur in the solar wind, but their source is not well
understood. Langmuir waves have been observed inside isolated magnetic
holes, suggesting that magnetic holes play an important role in the
generation of Langmuir waves. &lt;BR /&gt; Aims: We provide the statistical
distribution of Langmuir waves in the solar wind at different
heliocentric distances. In particular, we investigate the relationship
between magnetic holes and Langmuir waves. We identify possible source
regions of Langmuir waves in the solar wind, other than radio bursts, by
analyzing the local plasma conditions. &lt;BR /&gt; Methods: We analyzed data
from Solar Orbiter's Radio and Plasma Waves (RPW) and Magnetometer (MAG)
instruments. We used the triggered electric field snapshots and onboard
statistical data (STAT) of the Time Domain Sampler (TDS) of RPW to
identify Langmuir waves and investigate their properties. The plasma
densities were derived from the spacecraft potential estimated by RPW.
The MAG data were used to monitor the background magnetic field and
detect magnetic holes, which are defined as regions with an isolated
decrease in |B| of 50% or more compared to the background level. The
statistical analysis was performed on data from 2020 to 2021, comprising
heliocentric distances between 0.5 AU and 1 AU. &lt;BR /&gt; Results: We show
that 78% of the Langmuir waves in the solar wind not connected to radio
bursts occur in regions of local magnetic field depletions, including
the regions classified as isolated magnetic holes. We also show that the
Langmuir waves occur more frequently inside magnetic holes than in any
other region in the solar wind, which indicates that magnetic holes are
important source regions of solar wind Langmuir waves. We find that
Langmuir waves associated with magnetic holes in the solar wind
typically have lower amplitudes than those associated with radio bursts.</description>
</item>
<item>
<title> Improved Type III solar radio burst detection using congruent deep learning models</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...674A.218S</link>
<description>Solar flares are energetic events in the solar atmosphere that are often
linked with solar radio bursts (SRBs). SRBs are observed at metric to
decametric wavelengths and are classified into five spectral classes
(Type I-V) based on their signature in dynamic spectra. The automatic
detection and classification of SRBs is a challenge due to their
heterogeneous form. Near-real time detection and classification of SRBs
has become a necessity in recent years due to large data rates generated
by advanced radio telescopes such as the LOw Frequency ARray (LOFAR).
For this study, we implemented congruent deep learning models to
automatically detect and classify Type III SRBs. We generated simulated
Type III SRBs, which were comparable to Type IIIs seen in real
observations, using a deep learning method known as the generative
adversarial network (GAN). This simulated data were combined with
observations from LOFAR to produce a training set that was used to train
an object detection model known as you only look once (YOLOv2). Using
this congruent deep learning model system, we can accurately detect Type
III SRBs at a mean Average Precision (mAP) value of 77.71%.</description>
</item>
<item>
<title> Evidence for a northward-shifted relic field</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...674A.182M</link>
<description>Context. Solar and heliospheric parameters occasionally depict notable
differences between the northern and southern solar hemisphere. Although
the hemispheric asymmetries of some heliospheric parameters vary
systematically with the Hale cycle, this has not been found to be
commonly valid for solar parameters. Also, no verified physical
mechanism exists that can explain possible systematic hemispheric
asymmetries. &lt;BR /&gt; Aims: We use a novel method of high heliolatitudinal
vantage points to increase the fraction of one hemisphere in solar 10.7
cm radio fluxes and sunspot numbers. We aim to explore the possibility
that solar radio fluxes and sunspot numbers, the two most fundamental
solar parameters, depict systematic, possibly mutually similar patterns
in their hemispheric activities during the last 75 yr. &lt;BR /&gt; Methods:
We used three different sets of time intervals with increasing mean
heliographic latitude and calculated corresponding hemispheric high-
latitude radio fluxes and sunspot numbers. We also normalized these
fluxes by yearly means in order to study the variation of fluxes in the
two hemispheres over the whole 75 yr time interval. &lt;BR /&gt; Results: We
find that cycle-maximum radio fluxes and sunspot numbers in each odd
solar cycle (19, 21, 23) are larger at northern high latitudes than at
southern high latitudes, while maximum fluxes and numbers in all even
cycles (18, 20, 22 24) are larger at southern high latitudes than at
northern high latitudes. This alternation indicates a new form of
systematic, Hale-cycle-related variation in solar activity. Hemispheric
differences at cycle maxima are 15% for radio flux and 23% for sunspot
numbers, on average. The difference is largest during cycle 19 and
smallest in cycle 24. Normalized radio fluxes depict a dominant Hale-
cycle variation in both hemispheres, with an opposite phase and overall
amplitude of about 5% in the north and 4% in the south. Thus, there is
systematic Hale-cycle alternation in magnetic flux emergence in both
hemispheres. &lt;BR /&gt; Conclusions: The hemispheric Hale cycle in flux
emergence can be explained if there is a northward-directed relic
magnetic field, which is slightly shifted northward. In that case, in
odd cycles, the northern hemisphere is enhanced more than the southern
hemisphere, and in even cycles, the northern hemisphere is reduced more
than the southern hemisphere, establishing the observed hemispheric
alternation. The temporal change of asymmetry during the seven cycles
can be explained if the relic shift oscillates at the 210 yr
Suess/deVries period, which also provides a physical cause to this
periodicity. Gleissberg cycles are explained as off-equator excursions
of the relic, each Gleissberg cycle forming one half of the full relic
shift oscillation cycle. Having a relic field in the Sun also offers
interesting possibilities for century-scale forecasting of solar
activity.</description>
</item>
<item>
<title> The 17 April 2021 widespread solar energetic particle event</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...674A.105D</link>
<description>Context. A complex and long-lasting solar eruption on 17 April 2021
produced a widespread solar energetic particle (SEP) event that was
observed by five longitudinally well-separated observers in the inner
heliosphere that covered distances to the Sun from 0.42 to 1 au:
BepiColombo, Parker Solar Probe, Solar Orbiter, STEREO A, and near-Earth
spacecraft. The event was the second widespread SEP event detected in
solar cycle 25, and it produced relativistic electrons and protons. It
was associated with a long-lasting solar hard X-ray flare that showed
multiple hard X-ray peaks over a duration of one hour. The event was
further accompanied by a medium-fast coronal mass ejection (CME) with a
speed of 880 km s&lt;SUP&gt;-1&lt;/SUP&gt; that drove a shock, an extreme
ultraviolet wave, and long-lasting and complex radio burst activity that
showed four distinct type III burst groups over a period of 40 min. &lt;BR
/&gt; Aims: We aim to understand the reason for the wide spread of elevated
SEP intensities in the inner heliosphere as well as identify the
underlying source regions of the observed energetic electrons and
protons. &lt;BR /&gt; Methods: We applied a comprehensive multi-spacecraft
analysis of remote-sensing observations and in situ measurements of the
energetic particles and interplanetary context to attribute the SEP
observations at the different locations to the various potential source
regions at the Sun. We used an ENLIL simulation to characterize the
complex interplanetary state and its role in the energetic particle
transport. The magnetic connection between each spacecraft and the Sun
was determined using ballistic backmapping in combination with potential
field source surface extrapolations in the lower corona. Using also a
reconstruction of the coronal shock front, we then determined the times
when the shock establishes magnetic connections with the different
observers. Radio observations were used to characterize the directivity
of the four main injection episodes, which were then employed in a 2D
SEP transport simulation to test the importance of these different
injection episodes. &lt;BR /&gt; Results: A comprehensive timing analysis of
the inferred solar injection times of the SEPs observed at each
spacecraft suggests different source processes being important for the
electron and proton events. Comparison among the characteristics and
timing of the potential particle sources, such as the CME-driven shock
or the flare, suggests a stronger shock contribution for the proton
event and a more likely flare-related source for the electron event. &lt;BR
/&gt; Conclusions: In contrast to earlier studies on widespread SEP events,
we find that in this event an important ingredient for the wide SEP
spread was the wide longitudinal range of about 110 covered by distinct
SEP injections, which is also supported by our SEP transport modeling.
&lt;P /&gt;Movies are available at &lt;A href="https://www.aanda.org/10.1051/0004
-6361/202345938/olm"&gt;https://www.aanda.org&lt;/A&gt;.</description>
</item>
<item>
<title> Diagnostics of Flare Loop Parameters in Shrinkage and Ascent Stages Using Radio, X-ray, and UV Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..261Z</link>
<description>We propose the diagnostics of plasma parameters in flare loops using the
data of multi-wavelength observations in both shrinkage and expansion
phases of the loops. The approach of a flare loop as an equivalent
electric circuit is applied. We show that depending on plasma loop
parameters, the shrinkage may be accompanied by an increase in the
electric current in the loop rather than a decrease. The number density,
temperature, electric current, radius, loop-top altitude, and loop
volume are determined for the flare events on 16 April 2002 and 24
August 2002.</description>
</item>
<item>
<title> Paired quasi-periodic pulsations of hard X-ray emission in a solar flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SCPMA..6659611Z</link>
<description>We investigate high time resolution data obtained by the Gravitational
wave high-energy Electromagnetic Counterpart All-sky Monitor (GECAM)
during the flare event on 2022 April 21 at 01:52 UT. Several subpeaks
with durations of 46s have been detected in the hard X-ray precursor
phase, and the key feature is that they appear in pairs and seem like
double-peak structures. These subpeaks are rarely observed in hard X-ray
band and confirmed by the microwave obtained by Nobeyama Radio
Polarimeters (NoRP) and Radio Solar Telescope Network (RSTN). While an
exponential function can describe the continuum component of the time
profile from the precursor to part of the impulsive phase. The periods
of quasi-periodic pulsations (QPPs) are detected to be about 7.3 and
12.8s for the precursor and impulsive phase, respectively, with at least
95% confidence level. The paired QPPs are assumed to be double-peak QPPs
and then the scenario of current loop coalescence model is found to be
in good agreement with our observation. The precursor phase can be
interpreted as the oscillating coalescence of two islands, while the
impulsive phase can be interpreted as more islands to coalesce one by
one to form larger islands.</description>
</item>
<item>
<title> Investigation on the Formation of Herringbone Structure in Type II Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RAA....23e5010A</link>
<description>We report detailed observation of the "herringbone" of a Type II solar
radio burst that occurred on 2010 November 3rd. Data from the Space
Weather Prediction Center, National Oceanic and Atmospheric
Administration, e-CALLISTO, and Nanay RadioHeliograph are analyzed. We
determine the brightness temperature and degree of circular polarization
of the "herringbone" burst. Correlations between the physical parameters
and the "herringbone" are examined. Based on the relationship, this is
the first study that suggested this "herringbone" was generated through
fundamental plasma.</description>
</item>
<item>
<title> A novel spectrogram visual security encryption algorithm based on block compressed sensing and five-dimensional chaotic system</title>
<link>https://ui.adsabs.harvard.edu/abs/2023NonDy.111.9607Y</link>
<description>Based on block compressed sensing theory, combined with a five-
dimensional chaotic system, we propose and analyze a novel spectrogram
visual security encryption algorithm. This research is devoted to
solving the compression, encryption and steganography problems of
spectrograms involving large data volumes and high complexity. First,
the discrete wavelet transform is applied to the spectrogram to generate
the coefficient matrix. Then, block compressed sensing is applied to
compress and preencrypt the spectrogram. Second, we design a new five-
dimensional chaotic system. Then, several typical evaluation methods,
such as the phase diagram, Lyapunov exponent, bifurcation diagram and
sample entropy, are applied to deeply analyze the chaotic behavior and
dynamic performance of the system. Moreover, the corresponding Simulink
model has been built, which proves the realizability of the chaotic
system. Importantly, the measurement matrix required for compressed
sensing is constructed by the chaotic sequence. Third, dynamic Josephus
scrambling and annular diffusion are performed on the secret image to
obtain the cipher image. Finally, an improved least significant bit
embedding method and alpha channel synchronous embedding are designed to
obtain a steganographic image with visual security properties. To make
the initial keys of each image completely different from other images,
the required keys are produced using the SHA-256 algorithm. The
experimental results confirm that the visual security cryptosystem
designed in this study has better compression performance, visual
security and reconstruction quality. Furthermore, it is able to
effectively defend against a variety of conventional attack methods,
such as statistical attacks and entropy attacks.</description>
</item>
<item>
<title> RFI flagging in solar and space weather low frequency radio observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.521..630Z</link>
<description>Radio spectroscopy provides a unique inspection perspective for solar
and space weather research, which can reveal the plasma and energetic
electron information in the solar corona and inner heliosphere. However,
radio-frequency interference (RFI) from human activities affects
sensitive radio telescopes, and significantly affects the quality of
observation. Thus, RFI detection and mitigation for the observations is
necessary to obtain high quality science-ready data. The flagging of RFI
is particularly challenging for the solar and space weather observations
at low frequency, because the solar radio bursts can be brighter than
the RFI, and may show similar temporal behaviour. In this work, we
investigate RFI flagging methods for solar and space weather
observations, including a strategy for AOLAGGER, and a novel method that
makes use of a morphology convolution. These algorithms can effectively
flag RFI while preserving solar radio bursts.</description>
</item>
<item>
<title> Research on Calibration Sources for a 35-40 GHz Millimeter-Wave Solar Radio Observation System</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ITAP...71.4094Z</link>
<description>The microwave spectra in the optically thin regime provide unique
information about the solar corona magnetic field; thus, a millimeter-
wave solar radio observation system (35-40-GHz) in the Chashan
observatory is newly established to obtain relevant data. Herein, we
design and develop a blackbody calibration source employing a metal cone
array and absorbing patch to calibrate the system and obtain accurate
solar observation data for analysis and decision-making. The
reflectivity of the calibration source is simulated and measured to
characterize its emissivity. The reflectivity is obtained by the finite-
integeral technique (FIT) method under various fitting conditions, i.e.,
the thickness of the absorbent patches and aspect ratios of the cone.
The temperature gradient of cones is determined by the finite-element
method (FEM). A $5\times $ 5 array microwave blackbody was developed
based on a cone with a low scattering coefficient and excellent
temperature uniformity. To reduce the influence of spurious signals, the
time-domain gate technique is used to test the reflectivity of the
target. The results demonstrate that the emissivity of the blackbody is
higher than 0.9995 in the 35-40-GHz band. The temperature difference
between the cone top and the cone bottom is 0.20 C.</description>
</item>
<item>
<title> Understanding the Relationship between Solar Coronal Abundances and F10.7 cm Radio Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...948..121T</link>
<description>Sun-as-a-star coronal plasma composition, derived from full-Sun spectra,
and the F10.7 radio flux (2.8 GHz) have been shown to be highly
correlated (r = 0.88) during solar cycle 24. However, this correlation
becomes nonlinear during increased solar magnetic activity. Here we use
cotemporal, high spatial resolution, multiwavelength images of the Sun
to investigate the underlying causes of the nonlinearity between coronal
composition (FIP bias) and F10.7 solar index correlation. Using the Karl
G. Jansky Very Large Array, Hinode/EIS (EUV Imaging Spectrometer), and
the Solar Dynamics Observatory, we observed a small active region, AR
12759, throughout the solar atmosphere from the photosphere to the
corona. The results of this study show that the magnetic field strength
(flux density) in active regions plays an important role in the
variability of coronal abundances, and it is likely the main
contributing factor to this nonlinearity during increased solar
activity. Coronal abundances above cool sunspots are lower than in
dispersed magnetic plage regions. Strong magnetic concentrations are
associated with stronger F10.7 cm gyroresonance emission. Considering
that as the solar cycle moves from minimum to maximum, the sizes of
sunspots and their field strength increase with the gyroresonance
component, the distinctly different tendencies of radio emission and
coronal abundances in the vicinity of sunspots is the likely cause of
saturation of Sun-as-a-star coronal abundances during solar maximum,
while the F10.7 index remains well correlated with the sunspot number
and other magnetic field proxies.</description>
</item>
<item>
<title> Machine learning based approach for modeling and forecasting of GPS-TEC during diverse solar phase periods</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AcAau.206..177Y</link>
<description>The ionosphere is a dispersive medium and it is the most important
source of error affecting radio communications. As a result, precise
improvements in ionospheric Total Electron Content (TEC) predictions and
early warning alerts are critical for space-based radio communication
and navigation systems services. In the present study, we examined the
Global Positioning System (GPS)-derived TEC observations of Bangalore
station (Geog. Lat. 13.02 N and Geog. Long. 77.57 E) during the 24th
solar cycle, which extends the 11 years from 2009 to 2019. Based on
Solar Radio Flux (sfu) and seasonal features, machine learning
frameworks have been developed to forecast monthly/hourly GPS-TEC
values. Motivated by the preliminary results, the problem of traditional
approaches for predicting ionospheric GPS-TEC values and improvements
using the machine learning approach is discussed. The Kernel extreme
learning machine (KELM) model has characteristics of accuracy and good
generalization performance compared with the traditional method of Holt-
Winters (HW) and (Auto Regressive Moving Average (ARMA). The
experimental results show that the statistical validations of the KELM
model are superior to the other statistical models, with average Mean
Absolute Error (MAE) and Root Mean Square Error values, which is of 0.94
and 1.305 TECU (KELM), 1.70 and 2.29 TECU (ARMA) and 2.91 and 3.86 TECU
(HW) during different phases of the solar cycle. In addition, the
proposed model is validated by comparison with global ionospheric models
(International Reference Ionosphere (IRI) -2016 and Global Ionosphere
Map (GIM). The results show that the proposed approach is superior to
other alternatives using prediction accuracy. This paper outlines a
machine learning framework for space weather predictions and recommends
KELM classifier could be used for other query functions in Active
Learning (AL) practice approaches and other datasets of the Global
Navigation Satellite System (GNSS).</description>
</item>
<item>
<title> Research Progress on Interplanetary Type III Radio Bursts Based on PSP Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AcASn..64...35M</link>
<description>Compared to solar radio bursts, interplanetary (IP) radio bursts with
lower radiation frequencies are generally believed to originate in the
interplanetary space far from the low corona. The cutoff by Earth's
ionosphere makes the ground-based observations for it impossible. Parker
Solar Probe (PSP), launched by the National Aeronautics and Space
Administration (NASA) to explore the Sun with the closer heliocentric
distance than any previous spacecraft, provides an opportunity to study
the low-frequency radio burst. The radio spectrometer it carries can
observe radio radiation in the frequency range of 10 kHz--19.17 MHz. PSP
can approach the radiation source region of the IP type III radio burst.
Therefore, it has an unprecedented advantage to observe the
interplanetary radio bursts. This paper reviews the studies about type
III radio bursts observed by PSP so far. These studies include the
occurrence rate, polarization, scattering, cutoff frequency, possible
radiation mechanisms, and related radiation source regions of radio
bursts and so on. Finally, future research prospects are discussed.</description>
</item>
<item>
<title> Research Progress of the Heliospheric Radio Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AcASn..64...33C</link>
<description>The heliospheric radio emissions are the strongest radio emissions
phenomenon in the solar system, with a radiation power of at least
10$^{13}$ W, which can provide important physical information of high
energy electron beam and magnetic plasma structure near the heliospheric
boundary. Since the first detection by the Voyager spacecraft in 1983,
those radio emissions have widely and continuously attracted much
attention from researchers. There are generally two types of the
heliospheric radio emissions: instantaneous or drifting emission with
relatively high frequency, and continuous emission or non-drifting
emission with relatively low frequency. Usually, both types of emissions
start from about 2 kHz. For the drifting emission, it has the
characteristic of drifting to high frequency, the drifting rate is about
1--3 kHz/yr, the frequency range is 1.8--3.6 kHz, and the duration is
about 100--300 days. For the non-drifting emission, it has no obvious
frequency drift, the frequency range is 1.8--2.6 kHz, and the duration
is about 3 yr. It is generally believed that the heliospheric radio
emissions are related to shock. In this paper, the possible source
region of the radio emissions, the emission mechanisms, and the source
of shock related to the emissions are introduced. Furthermore, the
existing scientific problems and the future perspectives on the research
of heliospheric radio emissions are discussed.</description>
</item>
<item>
<title> Electron Cyclotron Maser Emission in Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AcASn..64...32T</link>
<description>Radio bursts are ubiquitous in the cosmic plasma. Solar radio emission
mainly comes from the outer atmosphere of the sun. It is an induced
radiation phenomenon generated by the interaction between energetic
electrons and solar atmospheric plasma. Different dynamic spectra of
solar radio bursts (SRBs) contain physical information of the plasma
structure and state in the radiation source region. Therefore, the
radiative mechanism of radio bursts has always been the object of
research. There are two kinds of coherent radiation mechanisms related
to solar radio bursts: one is the plasma radiation mechanism based on
electron Langmuir frequency; the other is the electron cyclotron maser
(ECM) radiation mechanism based on the electron cyclotron frequency.
Although these two radiation mechanisms were proposed almost at the same
time, based on the understanding of the coronal environment and the ECM
mechanism at that time, the ECM radiation mechanism did encounter some
difficulties in explaining SRBs. Until 1979, Wu &amp; Lee introduced the
relativistic effect and used the ECM radiation to explain the earth's
Auroral Kilometric Radiation (AKR). Since then, the ECM emission has
attracted wide attention. Considering some difficulties in applying the
ECM emission mechanism to SRBs, we proposed a series of modified models
in recent years. Firstly, the cutoff in the energy spectrum of the
power-law electrons can effectively drive the ECM instability without
relying on the anisotropic distribution of electron velocity. Secondly,
considering the influence of Alfvn wave perturbations which are
prevalent in space and celestial plasmas, a self-consistent ECM emission
mechanism excited by energetic electron beams is developed. On this
basis, this paper summarizes the application of the ECM emission
mechanism in traditional SRB phenomena from type I to V and microwave
SRBs in recent years.</description>
</item>
<item>
<title> Preface</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AcASn..64...23C</link>
<description>Over 99.9% of the baryonic matter in the universe is plasma, hence
plasma astrophysics is an important branch of modern astrophysics, which
provides the sound foundation for us to understand the formation,
evolution, and various eruptive phenomena in astrophysical systems. The
14 papers in this Special Issue systematically introduce the research
progress in the solar and heliospheric plasmas made by the Plasma
Astrophysics group in Purple Mountain Observatory, with the aim to help
readers get a glimpse of the research frontiers and remaining questions.</description>
</item>
<item>
<title> Adiabatic Radio Emission Spectrum of the Sun's Coronal Holes</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ARep...67..513D</link>
<description>Coronal holes on the Sun have been observed at individual frequencies
for quite a long time in the wavelength range from radio to X-rays.
Observations in a wide range of radio frequencies are carried out with
the RATAN-600 radio telescope. An analysis of long-term spectral
observations of the RATAN-600 radio telescope showed that the emission
spectrum of coronal holes is radically different from the spectrum of
active formations above sunspots, but, differing markedly from the
spectrum of the quiet Sun, it also has similarities with it. It has been
established that the radio emission of coronal holes has an adiabatic
spectrum and does not contain noticeable coherent radiation, that is,
recombination radio lines and lines of the fine structure of hydrogen
and other elements.</description>
</item>
<item>
<title> Comparison of chromospheric diagnostics in a 3D model atmosphere. H linewidth and millimetre continua</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...673A.137P</link>
<description>Context. The H line, one of the most studied chromospheric diagnostics,
is a tracer of magnetic field structures, while the intensity of its
line core provides an estimate of the mass density. The interpretation
of H observations is complicated by deviations from local thermodynamic
equilibrium (LTE) or instantaneous statistical equilibrium conditions.
Meanwhile, millimetre (mm) continuum radiation is formed in LTE, and
therefore the brightness temperatures from Atacama Large Millimetre-
submillimetre Array (ALMA) observations provide a complementary view of
the activity and the thermal structure of stellar atmospheres. These two
diagnostics together can provide insights into the physical properties
of stellar atmospheres, such as their temperature stratification,
magnetic structures, and mass density distribution. &lt;BR /&gt; Aims: In this
paper, we present a comparative study between synthetic continuum
brightness temperature maps at mm wavelengths (0.3 mm to 8.5 mm) and the
width of the H 6565  line. &lt;BR /&gt; Methods: We used the 3D radiative-
transfer codes Multi3D and Advanced Radiative Transfer (ART) to
calculate synthetic spectra for the H line and the mm continua,
respectively, from an enhanced network atmosphere model with non-
equilibrium hydrogen ionisation generated with the state-of-the-art 3D
radiation magnetohydrodynamics (rMHD) code Bifrost. We use a Gaussian
point spread function (PSF) to simulate the effect of ALMA's limited
spatial resolution and calculate the H versus mm continuum correlations
and slopes of scatter plots for the original and degraded resolution of
the whole box, quiet sun, and enhanced network patches separately. &lt;BR
/&gt; Results: The H linewidth and mm brightness temperatures are highly
correlated and the correlation is highest at a wavelength of 0.8 mm,
that is, in ALMA Band 7. The correlation systematically increases with
decreasing resolution. On the other hand, the slopes decrease with
increasing wavelength. The degradation of resolution does not have a
significant impact on the calculated slopes. &lt;BR /&gt; Conclusions: With
decreasing spatial resolution, the standard deviations of the
observables, H linewidth, and brightness temperatures decrease and the
correlations between them increase, but the slopes do not change
significantly. These relations may therefore prove useful in calibrating
the mm continuum maps observed with ALMA.</description>
</item>
<item>
<title> Statistical study of type III bursts and associated HXR emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...673A..57J</link>
<description>Context. Flare-accelerated electrons may produce closely temporarily
related hard X-ray (HXR) emission while interacting with the dense solar
atmosphere and radio type III bursts when propagating from the low
corona to the interplanetary medium. The link between these emissions
has been studied in previous studies. We present here new results on the
correlation between the number and spectrum of HXR-producing electrons
and the type III characteristics (flux, starting frequency). &lt;BR /&gt;
Aims: The aim of this study is to extend the results from previous
statistical studies of radio type III bursts and associated HXR
emissions: in particular, to determine what kind of correlation, if any,
exists between the HXR-emitting electron numbers and the radio flux, as
well as whether any correlations between the electron numbers or energy
spectra are deduced from associated HXR emissions and type III starting
(stopping) frequencies. &lt;BR /&gt; Methods: This study is based on thirteen
years of data between 2002 and 2014. We shortlisted 200 events with a
close temporal association between HXR emissions and radio type III
bursts in the 450-150 MHz range. We used X-ray flare observations from
RHESSI and Fermi/GBM to calculate the number of electrons giving rise to
the observed X-ray flux and observations from the Nanay Radioheliograph
to calculate the peak radio flux at different frequencies in the 450-150
MHz range. Under the assumption of thick-target emissions, the number of
HXR-producing electrons and their energy spectra were computed. The
correlation between electron numbers, power-law indices, and the peak
radio fluxes at different frequencies were analysed as well as potential
correlations between the electron numbers and starting frequency of the
radio burst. Bootstrap analysis for the correlation coefficients was
performed to quantify the statistical significance of the fit. &lt;BR /&gt;
Results: The correlation between the number of HXR electrons and the
peak flux of the type III emission decreases with increasing frequency.
This correlation is larger when considering the electron number above 20
keV rather than the electron number above 10 keV. A weak anti-
correlation is also found between the absolute value of the electron
spectral index and the peak radio flux at 228 MHz. A rough correlation
is found between the HXR-producing electron number above 20 keV and the
type III starting frequency. This correlation is smaller if the electron
number above 10 keV is considered. All the results are discussed in the
framework of results from previous studies and in the context of
numerical simulations of bump-in-tail instabilities and subsequent radio
emissions.</description>
</item>
<item>
<title> Quasi-Periodic Pulsations in an M-Class Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..215X</link>
<description>We have studied the quasi-periodic pulsations (QPPs) of the M2.3 flare
that occurred in the active region NOAA 12172 on 23 September 2014.
Through the fast Fourier transform (FFT) method, we decompose the flare
light curves into fast- and slowly-varying components, and the cut-off
threshold is 100 s. We find that the QPPs have a period of 40 s at soft
X-ray (SXR), hard X-ray (HXR), radio and ultraviolet (UV). Based on the
Atmospheric Imaging Assembly (AIA) on the Solar Dynamics Observatory
(SDO), we find that the QPPs take place at the same time interval as the
flare ribbon separation, and that the QPPs seem to originate from the
flare ribbons. Our observations tend to support the mechanism of the
periodic nonthermal electron injection during the flare eruption.</description>
</item>
<item>
<title> What to Do When the F10.7 Goes Out?</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SpWea..2103392E</link>
<description>The solar radio flux at 10.7 cm, known as F10.7, is a critical
operational space weather index. However, without a clear backup, any
interruption to the service can result in substantial errors in model
outputs. In this paper we show the impact of one such outage in March
2022 on the models TIE-GCM and NeQuick, and present a number of
alternative solutions that could be used for future outages. The
analysis is extended to the F10.7 time series since 1951 and the
approach resulting in the smallest reconstruction error of F10.7 uses
the solar radio flux observations at alternative wavelengths (the best
giving a percentage error of 3.1%). Alternatively, use of Sunspot
Number, a regular, robust alternative observation, results in a mean
percentage error of 8.2% and is also a reliable fallback solution.
Additionally, analysis of the error on the use of the conversion between
the 12-month rolling sunspot number (R12) and its conversion to F10.7 is
included.</description>
</item>
<item>
<title> Research on interference and noise reduction technology of solar radio observation system</title>
<link>https://ui.adsabs.harvard.edu/abs/2023PhyS...98d5006Z</link>
<description>The dynamic spectrum of solar radio burst is a very important tool to
study the characteristics of solar radio burst. However, due to the
influence of the instruments noise of the solar radio telescope,
external interference, the change of ambient temperature, absorption of
clouds and so on, the sensitivity of the observation system will be
reduced. In particular, the weak solar radio burst signal is easily
submerged by various interference signals. In order to improve the
sensitivity of solar radio telescope to observe solar radio burst
signals and remove narrow-band interference signals, a spectrum data
processing algorithm of spectral subtraction method based on entropy and
energy threshold values (SSM-EE) is proposed in this article. There are
multiple processing steps of SSM-EE. The first step is to improve the
signal-to-noise ratio (SNR) through accumulating and averaging the
spectrum data. The second step is to eliminate narrowband interference.
The spectral kurtosis algorithm is used to calculate the spectral
kurtosis of the narrowband interference signal, and then whether to
smooth it is determined according to whether it is greater than the
threshold. The third step is to establish a noise model. Calculating the
power spectrum entropy and energy entropy of each frame of the processed
spectrum data, judge whether it is a noise signal by judging the
relationship between the power spectrum entropy and energy entropy and
the corresponding threshold. The update model for noise floor is used to
obtain the real-time noise floor data. The last step is to eliminate the
background noise through spectral subtraction. The new spectrum data are
obtained by subtraction method between the original spectrum data and
the noise floor data. After a large number of data simulation and
verification of the actual observation data, it shows that the method
proposed in this article has good practical value.</description>
</item>
<item>
<title> Microwave response to kink oscillations of a plasma slab</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.520.4147K</link>
<description>The modulation of the intensity of microwave emission from a plasma slab
caused by a standing linear kink fast magnetoacoustic wave is
considered. The slab is stretched along a straight magnetic field, and
can represent, for example, a current sheet in a flaring active region
in corona of the Sun, or a streamer or pseudostreamer stalk. The plasma
density is non-uniform in the perpendicular direction and described by a
symmetric Epstein profile. The plasma parameter  is taken to be zero,
which is a good approximation for solar coronal active regions. The
microwave emission is caused by mildly relativistic electrons which
occupy a layer within the oscillating slab and radiate via the
gyrosynchrotron (GS) mechanism. Light curves of the microwave emission
were simulated in the optically thin part of the GS spectrum, and their
typical Fourier spectra were analysed. It is shown that the microwave
response to a linear kink magnetohydrodynamic wave is non-linear. It is
found that, while the microwave light curves at the node oscillate with
the same frequency as the frequency of the perturbing kink mode, the
frequency of the microwave oscillations at the antinode is two times
higher than the kink oscillation frequency. Gradual transformation the
one type of the light curves to another occurs when sliding from the
node to the antinode. This result does not depend on the width of the
GS-emitting layer inside the oscillating slab. This finding should be
considered in the interpretation of microwave quasi-periodic pulsations
in solar and stellar flares.</description>
</item>
<item>
<title> The frequency ratio and time delay of solar radio emissions with fundamental and harmonic components</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.520.3117C</link>
<description>Solar radio bursts generated through the plasma emission mechanism
produce radiation near the local plasma frequency (fundamental emission)
and double the plasma frequency (harmonic). While the theoretical ratio
of these two frequencies is close to 2, simultaneous observations give
ratios ranging from 1.6 to 2, suggesting either a ratio different from
2, a delay of the fundamental emission, or both. To address this long-
standing question, we conducted high-frequency, high-time resolution
imaging spectroscopy of type III and type J bursts with fine structures
for both the fundamental and harmonic components with LOFAR between 30
and 80 MHz. The short-lived and narrow frequency-band fine structures
observed simultaneously at fundamental and harmonic frequencies give a
frequency ratio of 1.66 and 1.73, similar to previous observations.
However, frequency-time cross-correlations suggest a frequency ratio of
1.99 and 1.95 with a time delay between the F and H emissions of 1.00
and 1.67 s, respectively for each event. Hence, simultaneous frequency
ratio measurements different from 2 are caused by the delay of the
fundamental emission. Among the processes causing fundamental emission
delays, anisotropic radio-wave scattering is dominant. Moreover, the
levels of anisotropy and density fluctuations reproducing the delay of
fundamental emissions are consistent with those required to simulate the
source size and duration of fundamental emissions. Using these
simulations we are able to, for the first time, provide quantitative
estimates of the delay time of the fundamental emissions caused by
radio-wave propagation effects at multiple frequencies, which can be
used in future studies.</description>
</item>
<item>
<title> Radio Measurements of Coronal Magnetic Fields in Fan-Spine Configurations on the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2023LatJP..60b..52R</link>
<description>Recent interest of solar physicists in the analysis of the coronal mass
ejections and circular solar flares in fan-spine magnetic configurations
(FSCs) necessitates measurements of the corresponding coronal magnetic
fields. A dominant sunspot with the circumjacent magnetic flux of
opposite polarity produces a specific coronal region of the quasi-
transverse (QT-) propagation of microwaves. We make use of the theory of
QT-propagation to evaluate the strengths of coronal magnetic fields in
the active regions NOAA 11579, 12242, and 12488 while they are non-
flaring. Microwave polarization changes were observed with the RATAN-600
radio telescope, the Siberian Solar Radio Telescope, and the Nobeyama
Radioheliograph. Changes in the sign of circular radio polarization
provide the strengths of coronal fields in a QT-region if the coronal
plasma density N&lt;SUB&gt;e&lt;/SUB&gt; and the length scale of magnetic field
divergence L&lt;SUB&gt;d&lt;/SUB&gt; are known. We evaluate the length scale by
means of the potential-field source-surface (PFSS) model and the coronal
density from the Gaussian inversion of the differential emission measure
(from the Solar Dynamics Observatory observational data), obtaining
N&lt;SUB&gt;e&lt;/SUB&gt; L&lt;SUB&gt;d&lt;/SUB&gt; = (0.46-0.64)10&lt;SUP&gt;10&lt;/SUP&gt;
m&lt;SUP&gt;2&lt;/SUP&gt;. The resulting coronal fields of 1.410&lt;SUP&gt;3&lt;/SUP&gt; T
and 2.3410&lt;SUP&gt;3&lt;/SUP&gt; T are attributed to the heights of 100 Mm and
50.2 Mm. We discuss the validity and consistency of the involved values
to draw conclusions on the feasibility of coronal radio magnetography of
FSCs.</description>
</item>
<item>
<title> The Predicition of Solar Flares Using Millimeter Radio Brightenings</title>
<link>https://ui.adsabs.harvard.edu/abs/2023LatJP..60b..43K</link>
<description>Solar activity could have significant impacts on various Earth and near-
Earth space systems, such as satellite communication and power grid
systems. The prediction of solar activity and active solar events plays
a major role when preparing for these disturbances. Various satellite-
based instruments constantly observe the Sun. However, only a few
ground-based solar instruments could provide versatile enough
information for the space weather prediction. Metshovi Radio
Observatory of Aalto University (Finland) has a unique collection of
millimetre (8 mm) solar radio maps over the past 40 years, and even
denser observational solar radio data catalogue since 2011. About 75-80
% days yearly are covered nowadays. This gives opportunity to make
statistical estimation of solar flare occurrence based on solar radio
maps. In this study, we had 2253 days when both solar radio map and GOES
(Geostationary Operational Environmental Satellites) classified solar
flare were observed. In this work, we used solar flare classification
done by the Space Weather Centre (SWC) of the National Oceanic and
Atmospheric Administration (NOAA). The data were observed between 1
January 2011 and 12 September 2022. Our study shows that the maximum
intensity of radio brightenings is a good indicator to tell which kind
of GOES classified solar flare could be expected to happen. The article
presents that intense radio brightening is needed to produce a certain
GOES classified solar flare.</description>
</item>
<item>
<title> Validation of F2-layer critical frequency variations in the ionosphere with radio observations of solar bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JASTP.24506056S</link>
<description>The high-frequency (HF) ionospheric cutoff restricts the possibilities
of radio astronomical observations from the Earth, but on the other
hand, it allows one to estimate the F2-layer critical frequency of the
ionosphere. This effect has been measured using a new active antenna
meant for receiving cosmic radio emission in the frequency range 1-40
MHz. The instrument was implemented near the Ukrainian T-shape
Radiotelescope, second modification (UTR-2) and serves as a prototype of
the HF antenna for a future radio array on the farside of the Moon. We
detected directly a storm of solar radio bursts on May 22, 2021 and
observed clearly their cutoff due to the ionosphere. For comparison our
analysis of the experimental data was supplemented by simultaneous
measurements from ionosondes located close to the UTR-2. The distance
between the closest ionosonde near Zmiiv (Kharkiv region, Ukraine) and
the radio astronomical antenna used in the experiment is 46.5 km.
Results obtained from the solar radio records are consistent with the
ionosonde data. We show that such an antenna implementation provides us
with new opportunities to study the F2-layer critical frequency of the
ionosphere.</description>
</item>
<item>
<title> Fine Structures of Type-IV Solar Radio Bursts Associated with Stationary and Moving Sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..153F</link>
<description>Various types of fine structure in the continuum emission of type-IV
radio bursts are considered as applied to different types of radiation
sources, both stationary and moving. In the case of stationary sources,
the origin of the fine structure is associated both with processes in
individual magnetic loops (quasi-periodic acceleration and
magnetohydrodynamic waves), and with large-scale processes associated
with the propagation of magnetohydrodynamic disturbances, the formation
of loop arcades, and processes of discrete acceleration of particles
synchronous with them, causing the pulsating nature of radio emissions.
For the case of a moving source, the generation mechanism largely
depends on the magnetic structure of the source (an expanding magnetic
arc or an isolated plasma cloud). In this case, the connection with
coronal mass ejections and shock waves is also important. Secondary
pulsations are explained by a magnetohydrodynamic fluctuation source in
the form of a magnetic loop or cloud. The absence of other fine
structures in the continuum of moving type-IV bursts may be due to the
critical angle of the loss cone for the excitation of whistlers.</description>
</item>
<item>
<title> Dependence of NmF2 Local Annual Asymmetry Index on Local Time and Solar Activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63..121D</link>
<description>An analysis of the dependence of the local annual asymmetry R index on
local time and solar activity has been performed for 19632013 based on
the data of the medians of the maximum electron density of F2-layer NmF2
at the pair of the ionospheric stations BoulderHobart where the R index
is the JanuaryJuly ratio of the total NmF2 concentration (for this pair
of stations) at a fixed local time. As an indicator of solar activity
for the median NmF2, the F index is used, i.e. the 81-day average value
of the solar radio emission flux at a wavelength of 10.7 cm, which is
centered on the middle of the given month. It was found that for the
dependence of the R index on the local time LT, a semidiurnal mode
prevails with maxima near noon and midnight and minima in the morning
and evening. The lowest R values, R = 1, are observed at low solar
activity in a narrow interval of 1919.5 LT. Annual asymmetry in the
NmF2 median exists (R &gt; 1) for all other hours of local time at any
level of solar activity. Near noon the R index increases with solar
activity with a tendency to saturation at a high level of this activity.
Around midnight for the dependence of the R index on F there is a
maximum near F = 140, above which R decreases with growth of F. High R
index values at noon and midnight are mainly due to relatively high
values of NmF2 in January in the Northern Hemisphere (local winter,
Boulder) at noon and in the Southern Hemisphere (local summer, Hobart)
at midnight.</description>
</item>
<item>
<title> The Efficiency of Electron Acceleration during the Impulsive Phase of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...947L..13K</link>
<description>Solar flares are known to be prolific electron accelerators, yet
identifying the mechanism(s) for such efficient electron acceleration in
solar flare (and similar astrophysical settings) presents a major
challenge. This is due in part to a lack of observational constraints
related to conditions in the primary acceleration region itself.
Accelerated electrons with energies above ~20 keV are revealed by hard
X-ray (HXR) bremsstrahlung emission, while accelerated electrons with
even higher energies manifest themselves through radio gyrosynchrotron
emission. Here, we show, for a well-observed flare on 2017 September 10,
that a combination of RHESSI HXR and and the Solar Dynamics
Observatory/Atmospheric Imaging Assembly (SDO/AIA) EUV observations
provides a robust estimate of the fraction of the ambient electron
population that is accelerated at a given time, with an upper limit of
10&lt;SUP&gt;-2&lt;/SUP&gt; on the number density of nonthermal (20 keV)
electrons, expressed as a fraction of the number density of ambient
protons in the same volume. This upper limit is about 2 orders of
magnitude lower than previously inferred from microwave observations of
the same event. Our results strongly indicate that the fraction of
accelerated electrons in the coronal region at any given time is
relatively small but also that the overall duration of the HXR emission
requires a steady resupply of electrons to the acceleration site.
Simultaneous measurements of the instantaneous accelerated electron
number density and the associated specific electron acceleration rate
provide key constraints for a quantitative study of the mechanisms
leading to electron acceleration in magnetic reconnection events.</description>
</item>
<item>
<title> Parametric study of the kinematic evolution of coronal mass ejection shock waves and their relation to flaring activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...672A.127J</link>
<description>Context. Coronal and interplanetary shock waves produced by coronal mass
ejections (CMEs) are major drivers of space-weather phenomena, inducing
major changes in the heliospheric radiation environment and directly
perturbing the near-Earth environment, including its magnetosphere. A
better understanding of how these shock waves evolve from the corona to
the interplanetary medium can therefore contribute to improving
nowcasting and forecasting of space weather. Early warnings from these
shock waves can come from radio measurements as well as coronagraphic
observations that can be exploited to characterise the dynamical
evolution of these structures. &lt;BR /&gt; Aims: Our aim is to analyse the
geometrical and kinematic properties of 32 CME shock waves derived from
multi-point white-light and ultraviolet imagery taken by the Solar
Dynamics Observatory (SDO), Solar and Heliospheric Observatory (SoHO),
and Solar-Terrestrial Relations Observatory (STEREO) to improve our
understanding of how shock waves evolve in 3D during the eruption of a
CME. We use our catalogue to search for relations between the shock
wave's kinematic properties and the flaring activity associated with the
underlying genesis of the CME piston. &lt;BR /&gt; Methods: Past studies have
shown that shock waves observed from multiple vantage points can be
aptly reproduced geometrically by simple ellipsoids. The catalogue of
reconstructed shock waves provides the time-dependent evolution of these
ellipsoidal parameters. From these parameters, we deduced the lateral
and radial expansion speeds of the shocks evolving over time. We
compared these kinematic properties with those obtained from a single
viewpoint by SoHO in order to evaluate projection effects. Finally, we
examined the relationships between the shock wave and the associated
flare when the latter was observed on the disc by considering the
measurements of soft and hard X-rays. &lt;BR /&gt; Results: We find that at
around 25 solar radii (R&lt;SUB&gt;&lt;/SUB&gt;), the shape of a shock wave is very
spherical, with a ratio between the lateral and radial dimensions (minor
radii) remaining at around b/a  1.03 and a radial to lateral speed
ratio (V&lt;SUB&gt;R&lt;/SUB&gt;/V&lt;SUB&gt;L&lt;/SUB&gt;)1.44. The CME starts to slow down a
few tens of minutes after the first acceleration and then propagates at
a nearly constant speed. We revisit past studies that show a relation
between the CME speed and the soft X-ray emission of the flare measured
by the Geostationary Operational Environmental Satellite (GOES) and
extend them to higher flare intensities and shock speeds. The time lag
between the peak of the flare and of the CME speed is up to a few tens
of minutes. We find that for several well-observed shock onsets, a clear
correlation is visible between the derivative of the soft X-ray flux and
the acceleration of the shock wave.</description>
</item>
<item>
<title> Solar Radio Emissions and Ultralight Dark Matter</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9..142A</link>
<description>Ultralight axions and dark photons are well-motivated dark matter
candidates. Inside the plasma, once the mass of ultralight dark matter
candidates equals the plasma frequency, they can resonantly convert into
electromagnetic waves, due to the coupling between the ultralight dark
matter particles and the standard model photons. The converted
electromagnetic waves are monochromatic. In this article, we review the
development of using radio detectors to search for ultralight dark
matter conversions in the solar corona and solar wind plasma.</description>
</item>
<item>
<title> Impacts of Extreme Space Weather Events on September 6th, 2017 on Ionosphere and Primary Cosmic Rays</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RemS...15.1403K</link>
<description>The strongest X-class solar flare (SF) event in 24th solar cycle, X9.3,
occurred on 6 September 2017, accompanied by earthward-directed coronal
mass ejections (CMEs). Such space weather episodes are known to cause
various threats to human activities ranging from radio communication and
navigation disturbances including wave blackout to producing geomagnetic
storms of different intensities. In this study, SFs' ionospheric impacts
and effects of accompanied heliospheric disturbances on primary cosmic
rays (CR) are investigated. This work offers the first detailed
investigation of characteristics of these extreme events since they were
inspected both from the perspective of their electromagnetic nature,
through very low frequency (VLF) radio waves, and their corpuscular
nature of CR by multi-instrumental approach. Aside data recorded by
Belgrade VLF and CR stations, data from GOES and SOHO space probes were
used for modeling and analysis. Conducted numerical simulations revealed
a significant change of ionospheric parameters (sharpness and effective
reflection height) and few orders of magnitude increase of electron
density. We compared our findings with those existing in the literature
regarding the ionospheric response and corresponding parameters. In
addition, Forbush decrease (FD) magnitude, corrected for magnetospheric
effect, derived from measurements, and one predicted from power
exponents used to parametrize the shape of energetic proton fluence
spectra at L1 were compared and found to be in good agreement. Presented
findings could be useful for investigation of atmospheric plasma
properties, particles' modeling, and prediction of extreme weather
impacts on human activities.</description>
</item>
<item>
<title> sunspot oscillations in 3-6 GHz band</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.519.4397S</link>
<description>We present the first observations of spatially resolved oscillation
sources obtained with the Siberian Radioheliograph at 3-6 GHz. We have
found significant flux oscillations with periods of about 3, 5, and 13
min emitted from AR12833. The 3-min periodicity dominates at higher
frequencies. It was found that the apparent level of oscillations
depends on the active region location on the disc, and scales down
towards the limbs. The oscillations were studied in detail during 1 h
interval on 2021 June 19. We found that sources of 3-min oscillations
were located above the umbra and their emission is extraordinary
polarized. The 5- and 13-min periods were manifested in emission at
lower frequencies, down to 2.8 GHz. Sources with 5-min periodicity were
located near the umbra/penumbra boundary and in the pore region.
Positions of sources with 13-min oscillations were different at 3.1 and
4.7 GHz. We found consistency between spatial location of the
oscillation sources in radio and ultraviolet at 171 and 304 . There is
significant correlation of signals in two ranges. Time delays between
microwave oscillations increase as the frequency decreases, which can be
explained by upward propagation of periodic disturbances. The
localization of oscillation sources is probably related to magnetic
structures with different wave cut-off frequencies at different heights.</description>
</item>
<item>
<title> Analyses for the Mechanism of Solar Radio Burst Interfering Satellite Navigation Signal and Influence Presentation.</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChJSS..43..321D</link>
<description>Solar radio bursts are a potential interference factor in navigation
systems. From the navigation signal model is derived in this paper, the
paper analyzes the solar radio burst interference mechanism of
navigation signal, the interference effects exist three effects, namely
with the solar radio burst flux, receiver performance, and the Angle of
the Sun-navigation antenna height, synthesize the proposed the influence
of solar radio burst interfere with communication navigation equation.
It is concluded that the total integrated power of the solar burst flow
in the navigation communication frequency band is positively correlated
with the decrease of the signal to noise ratio of the communication
signal, and is affected by the modulation of the height Angle of the
sun-antenna and the effective area of the antenna, and has a convolution
relationship with the response function of the loop filter of the
navigation receiver. Then, this paper further analyzed the GPS lock-out
signal during the solar radio bursts on 28 October 2003, 6 December 2006
and 4 November 2015. It is found that the loss-rate of different
receivers at the same site is different in the same event (receiver
performances effect). The loss-of-lock rate of the same receiver at
different latitudes in the same event is different (Sun-antenna height
Angle effect). In addition, under the condition of non-uniform spectrum
of L-band (12 GHz) solar radio bursts in the same event (solar radio
burst flow distribution effect), the decrease of signal to noise ratio
of L1 and L2 band communication signals is also different. Therefore,
the analytical correctness of the above influence equation is verified
by the observation characterization of the above three events.</description>
</item>
<item>
<title> 10.7 cm10.7 cmSolar Full-disk Flare Forecasting Model Based on 10.7 cm Solar Radio Flux.</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChJSS..43..212L</link>
<description>Solar flare is an important solar active phenomenon, which is manifested
as electromagnetic radiant enhancement in almost all wave bands. The
statistics indicate that the solar flare is positively associated with
the solar active levels. In this paper, a method for predicting the
probability of solar flare is established based on the statistical
relationship between 10.7 cm flux and solar flare during 1975 to 2007.
The forecasting model can be used to predict the probability of C, M and
X class flares. During 2008 to 2016, the predicted errors of the model
for C, M and X class flares are 0.113, 0.087 and 0.012, respectively,
and the predicted skill scores are 0.250, 0.106 and 0.012, respectively.
It means that our method has less predicted errors and more skill scores
than the average model for predicting C, M and X class flares. During
the period from 2008 to 2016, the predicted results of the model are
similar to that of Space Environment Prediction Center in National Space
Science Center. It indicates that the model is feasible in the actual
space environment prediction.</description>
</item>
<item>
<title> Solar Radio Spikes and Type IIIb Striae Manifestations of Subsecond Electron Acceleration Triggered by a Coronal Mass Ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...946...33C</link>
<description>Understanding electron acceleration associated with magnetic energy
release at subsecond scales presents major challenges in solar physics.
Solar radio spikes observed as subsecond, narrow-bandwidth bursts with
f/f ~ 10&lt;SUP&gt;-3&lt;/SUP&gt;-10&lt;SUP&gt;-2&lt;/SUP&gt; are indicative of a subsecond
evolution of the electron distribution. We present a statistical
analysis of frequency- and time-resolved imaging of individual spikes
and Type IIIb striae associated with a coronal mass ejection (CME).
LOFAR imaging reveals that the cotemporal (&lt;2 s) spike and striae
intensity contours almost completely overlap. On average, both burst
types have a similar source size with a fast expansion at millisecond
scales. The radio source centroid velocities are often superluminal and
independent of frequency over 30-45 MHz. The CME perturbs the field
geometry, leading to increased spike emission likely due to frequent
magnetic reconnection. As the field restores itself toward the prior
configuration, the observed sky-plane emission locations drift to
increased heights over tens of minutes. Combined with previous
observations above 1 GHz, the average decay time and source size
estimates follow a ~1/f dependence over three decades in frequency,
similar to radio-wave scattering predictions. Both time and spatial
characteristics of the bursts between 30 and 70 MHz are consistent with
radio-wave scattering with a strong anisotropy of the density
fluctuation spectrum. Consequently, the site of the radio-wave emission
does not correspond to the observed burst locations and implies
acceleration and emission near the CME flank. The bandwidths suggest
intrinsic emission source sizes &lt;1 at 30 MHz and magnetic field
strengths a factor of two larger than average in events that produce
decameter spikes.</description>
</item>
<item>
<title> Automated detection and statistical study of solar radio spikes</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ap&amp;SS.368...14L</link>
<description>The most typical observational features of solar radio spikes are their
short duration and narrow bandwidth. We have improved the YOLOv5s
network model for these characteristics by adding inclined bounding
frames and attention and feature fusion mechanism modules. The
decimeter- and meter-wavelength spikes observed by the Solar Broad-band
Radio Spectrometer in Huairou and the Chashan Solar Radio Observatory
spectrograph are used to carry out experiments, respectively. The
results demonstrate that the AP value obtained by the improved network
is 74%, which is almost 14% higher than the original network. The
improved network detects 9709 (1379) decimeter- (meter-) wavelength
spikes in two events with durations, bandwidths, relative bandwidths,
and frequency-drift rates. The spikes at decimeter and meter wavelengths
are again categorized based on their frequency-drift rates, such as
positive, negative, and no measurable frequency-drift rates. We have
carried out a statistical study on these categorized spikes. These
statistical results and findings constrain solar radio spikes'
formation.</description>
</item>
<item>
<title> Analysis of ionospheric TEC response to solar and geomagnetic activities at different solar activity stages</title>
<link>https://ui.adsabs.harvard.edu/abs/2023AdSpR..71.2225F</link>
<description>Studying the relationship of total electron content (TEC) to solar or
geomagnetic activities at different solar activity stages can provide a
reference for ionospheric modeling and prediction. On the basis of solar
activity indices, geomagnetic activity parameters, and ionospheric TEC
data at different solar activity stages, this study analyzes the overall
variation relationships of solar and geomagnetic activities with
ionospheric TEC, the characteristics of the quasi-27-day periodic
oscillations of the three variables at different stages, and the delayed
TEC response of solar activity by conducting correlation analysis,
Butterworth band-pass filtering, Fourier transform, and time lag
analysis. The following results are obtained. (1) TEC exhibits a
significant linear relationship with solar activity at different solar
activity stages. The correlation coefficients |R| are arranged as
follows: |R|&lt;SUB&gt;EUV&lt;/SUB&gt; &gt; |R|&lt;SUB&gt;F10.7&lt;/SUB&gt; &gt; |R|&lt;SUB&gt;sunspot
number&lt;/SUB&gt;. No significant linear relationship exists between TEC and
geomagnetic activity parameters (|R| &lt; 0.35). (2) TEC, solar activity
indices, and geomagnetic activity parameters have a period of 10.5
years. The maximum amplitudes of the Fourier spectrum for TEC and solar
activity indices are nearly 27 days and those of geomagnetic activity
parameters are nearly 27 and 13.5 days. (3) The deviations of the
quasi-27-day significant periodic oscillation of TEC and solar activity
indices are consistent. (4) No evident relationship exists between the
quasi-27-day periodic oscillation of TEC and geomagnetic activity
parameters. (5) The delay time of TEC for the 10.7 cm solar radio flux
and extreme ultraviolet is always consistent, whereas that for sunspot
number varies at each stage.</description>
</item>
<item>
<title> The Sun at millimeter wavelengths. IV. Magnetohydrodynamic waves in small-scale bright features</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...671A..69G</link>
<description>&lt;BR /&gt; Aims: We used solar observations of a plage-enhanced network with
the Atacama Large Millimeter/sub-millimeter Array (ALMA) in Band 3 and
Band 6, together with synthetic continuum maps from numerical
simulations with Bifrost in the same bands, to carry out a detailed
study of bright small-scale magnetic features. &lt;BR /&gt; Methods: We made
use of an algorithm to automatically identify and trace bright features
within the field of view (FoV) of the ALMA observations and the
simulation. In particular, the algorithm recovers information of the
time evolution of the shape, motion of the centre of gravity,
temperature, and size for each feature. These quantities are used to
determine the oscillatory properties of each feature utilising wavelets
analysis. &lt;BR /&gt; Results: We found 193 and 293 features in the Bands 3
and 6 observations, respectively. In the degraded simulation, the total
number of features were 24 for Band 3 and 204 for Band 6. In the
original simulation, the total number of features were 36 for Band 3 and
392 for Band 6. Based on the simulation, we confirm the magnetic nature
of the features. We have obtained average oscillation periods of 30-99 s
for the temperature, 37-92 s for size, and 37-78 s for horizontal
velocity. There are indications for the possible presence of transverse
(kink) waves with average amplitude velocities of 2.1-5.0 km
s&lt;SUP&gt;1&lt;/SUP&gt;. We find a predominant anti-phase behaviour between
temperature and size oscillations suggesting that the variations of the
bright features are caused by compressible fast-sausage
magnetohydrodynamics (MHD) modes. For the first time to our knowledge,
we estimated the flux of energy of the fast-sausage waves at the
chromospheric heights sampled by ALMA as 453-1838 W m&lt;SUP&gt;2&lt;/SUP&gt; for
Band 3 and 3640-5485 W m&lt;SUP&gt;2&lt;/SUP&gt; for Band 6. &lt;BR /&gt; Conclusions: We
have identified MHD waves, both transverse (kink) and compressible
sausage modes, in small-scale (magnetic) structures, independently, in
both ALMA Band 3 and Band 6 observations, along with their corresponding
synthetic images from simulations. The decrease of wave energy-flux with
height (from Band 6 to Band 3) could possibly suggest energy dissipation
at chromospheric heights, namely, wave heating, with the assumptions
that the identified small-scale waves are typical at each band and they
propagate upward through the chromosphere.</description>
</item>
<item>
<title> Temporal and spatial association between microwaves and type III bursts in the upper corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...671A..30A</link>
<description>One of the most important tasks in solar physics is the study of
particles and energy transfer from the lower corona to the outer layers
of the solar atmosphere. The most sensitive methods for detecting fluxes
of non-thermal electrons in the solar atmosphere is observing their
radio emission using modern large radioheliographs. We analyzed joint
observations from the 13 April 2019 event observed by LOw-Frequency
ARray (LOFAR) at meter wavelengths, and the Siberian Radio Heliograph
(SRH) and the Badary Broadband Microwave Spectropolarimeter (BBMS)
spectropolarimeter in microwaves performed at the time of the second PSP
perihelion. During a period without signatures of non-thermal energy
release in X-ray emission, numerous type III and/or type J bursts were
observed. During the same two hours we observed soft X-ray brightenings
and the appearance of weak microwave emission in an abnormally narrow
band around 6 GHz. At these frequencies the increasing flux is well
above the noise level, reaching 9 sfu. In the LOFAR dynamic spectrum of
5380 MHz a region is found that lasts about an hour whose emission is
highly correlated with 6 GHz temporal profile. The flux peaks in the
meter waves are well correlated with extreme UV (EUV) emission
variations caused by repeated surges from the bright X-point. We argue
that there is a common source of non-thermal electrons located in the
tail of the active region, where two loop systems of very different
sizes interacted. The frequencies of type III and/or type J bursts are
in accordance with large loop heights around 400 Mm, obtained by the
magnetic field reconstruction. The microwave coherent emission was
generated in the low loops identified as bright X-ray points seen in
soft X-ray and EUV images, produced by electrons with energies several
tens of keV at about twice the plasma frequency.</description>
</item>
<item>
<title> Multi-Periodicity of High-Frequency Type III Bursts as a Signature of the Fragmented Magnetic Reconnection</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Univ....9...92K</link>
<description>Using the radio spectra of the 2 April 2022 eruptive flare, we analyze a
group of highfrequency type III bursts by our new wavelet method. In
this analysis, we found a multi-periodicity of these bursts that is
interpreted by the electron beams accelerated in the fragmented magnetic
reconnection in the rising magnetic rope. We propose that each period in
these type III bursts is a result of the periodic interaction of sub-
ropes formed in the rising magnetic rope. In each interaction, the
period depends on the diameter of interacting sub-ropes and local Alfvn
velocity. This interpretation is supported by detection of the specific
EUV structure which was, according to our knowledge, observed for the
first time. All proposed processes occur in the rising magnetic rope.
Thus, this flare deviates from the standard flare model, where the main
magnetic reconnection is located below the rising magnetic rope.</description>
</item>
<item>
<title> Parametric Evolution of Power-law Energy Spectra of Energetic Electrons in the Coronal Loops</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RAA....23b5009T</link>
<description>Fast electron beams (FEBs) are one of the main products of various
active events and are ubiquitous in solar, space and cosmic plasmas.
They reveal themselves in hard X-ray and radio emissions. The observed
characteristics of X-ray and radio emissions sensitively depend on the
energy distribution of FEBs, which usually have a power-law energy
spectrum. As FEBs travel in the solar atmosphere, their energy
distribution can considerably vary due to the interaction with ambient
plasmas. Tang et al. investigated the evolution of the energy spectrum
of the FEBs traveling along a flare loop and discussed the possible
effects on associated hard X-ray (HXR) and radio emissions. Considering
the ubiquitous coronal loops in active regions, in the present paper, we
investigate the parametric evolution of the energy spectra of FEBs when
propagating along coronal loops. Here, we take the sunpot atmospheric
model as an approximate coronal loop atmosphere model. The results show
that the energy loss has an important impact on the cutoff behavior and
energy spectra of FEBs when precipitating in a coronal loop with density
ratio n &lt;SUB&gt; b &lt;/SUB&gt;/n &lt;SUB&gt; e &lt;/SUB&gt; = 0.01. The initially single
power-law spectrum with a steepness cutoff can evolve into a more
complex double power-law spectrum or two "knees" power-law spectrum with
a flattened steepness cutoff behavior or saturation cutoff behavior. Our
calculations also demonstrate that the energy spectrum evolution is not
obvious if n &lt;SUB&gt; b &lt;/SUB&gt;/n &lt;SUB&gt;0&lt;/SUB&gt; = 0.001 as Tang et al.
asserted. The present results are helpful for a more comprehensive
understanding of the dynamic spectra of HXR and radio emissions from
FEBs.</description>
</item>
<item>
<title> Prediction of TEC and Range Error using Low-latitude GPS Data during January to April 2022 Solar Flare Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2023Ge&amp;Ae..63...17K</link>
<description>The effects of solar, geomagnetic, and ionospheric anomalies on
satellite communication are inextricable. Range Error (RE) is the most
common fault that is faced by the navigational receivers during solar
flares. Since RE always depends on the Total Electron Content (TEC)
available across the satellite ray path, a prediction model capable of
predicting the TEC in advance will be an excellent deterrent during
adverse space weather conditions. In this research, Cokriging based
Surrogate Model (COKSM) is constructed for predicting the TEC variations
that occurred during the month of January 2022 to April 2022 over
Hyderabad region. The input data used in the construction of the model
includes F10.7 radio flux, Sunspot number (SSN), Geomagnetic index Kp
and Ap along with Vertical TEC (VTEC) data collected from Hyderabad
station located in 17.31 N latitude and 78.55 E longitude. The data is
collected in hourly averaged resolution for a period of 120 days
covering January to April 2022. The variations in Ionospheric TEC due to
solar flares and geomagnetic anomalies that occurred during the selected
observation dates are principally analyzed in order to evaluate the
prediction capability of the COKSM program during adverse conditions.
The performance of the model is evaluated using metrics like Root Mean
Square Percentage error (RMSPE), Correlation Coefficient (), CHI-
Squared goodness of fit test and R-squared. The results that are plotted
as a linear regression scatter plot clearly shows that with very small
residuals the proposed prediction model is performing well for TEC
prediction. The overall RE predicted by the model is within the scale of
112 meters. The error parameters calculated between true TEC and
predicted TEC is found out to be in the scale of 0.88 to 5.06% for
RMSPE, 0.9308 to 0.9981 for correlation coefficient, 4.97 to 107.94
(TECU) for chi squared and 0.78 to 0.98 (TECU) for R squared.</description>
</item>
<item>
<title> Spectroradiometry of the Solar Corona on the RATAN-600</title>
<link>https://ui.adsabs.harvard.edu/abs/2023CosRe..61...27B</link>
<description>Modern studies of solar radio emission are complicated by continuous
power amplification and multifrequency external interference, which
often completely overlap important frequency ranges. Many topical
problems in solar radio astronomy require large effective areas of radio
telescopes, high frequency and time resolutions, accurate spatial
measurements, and a large dynamic range. It becomes relevant to change
the concept of receiving recording equipment. This paper deals with
topical problems of the physics of the solar corona in combination with
optimal methods of observation with large instruments. The features and
difficulties of combining high parametersdynamic, spatial, temporal,
and frequency resolutionsare considered. The proposed solutions of the
new-generation observation complex implement the possibilities of
intelligent selection of registration conditions in a multioctave mode
with multichannel over 8000 channels/GHz with temporary permission up to
8 ms/spectrum. A multiobject observation mode becomes available from
powerful flaring objects to faint structures of various nature. High-
speed data processing makes it possible to implement an online mode of
interference elimination, which is based on a fast statistical analysis
of the spectrum with the selection of non-Gaussian (interference)
structures. Methods for high-speed analysis of large-volume data (the
principal component analysis method) and their presentation to the user
are proposed. Examples of the operation of the complex in the range of
1-3 GHz are given. The prospects of a new approach for multiobject radio
astronomy observations in the implementation of the RATAN-600 tracking
mode are considered: from recombination lines to wide-range spectra,
from low-contrast fluctuations to fast changes in flares, etc.</description>
</item>
<item>
<title> Modeling Hadronic Gamma-Ray Emissions from Solar Flares and Prospects for Detecting Nonthermal Signatures from Protostars</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...944..192K</link>
<description>We investigate gamma-ray emission in the impulsive phase of solar flares
and the detectability of nonthermal signatures from protostellar flares.
Energetic solar flares emit high-energy gamma rays of GeV energies, but
their production mechanism and emission site are still unknown. Young
stellar objects, including protostars, also exhibit luminous X-ray
flares, but the triggering mechanism of the flaring activity is still
unclear owing to the strong obscuration. Nonthermal signatures in
millimeter/submillimeter and gamma-ray bands are useful to probe
protostellar flares owing to their strong penetration power. We develop
a nonthermal emission model of the impulsive phase of solar flares,
where cosmic-ray protons accelerated at the termination shock produce
high-energy gamma rays via hadronuclear interaction with the evaporation
plasma. This model can reproduce gamma-ray data in the impulsive phase
of a solar flare. We apply our model to protostellar flares and show
that the Cherenkov Telescope Array will be able to detect gamma rays of
TeV energies if particle acceleration in protostellar flares is
efficient. Nonthermal electrons accelerated together with protons can
emit strong millimeter and submillimeter signals via synchrotron
radiation, whose power is consistent with the energetic
millimeter/submillimeter transients observed from young stars. Future
gamma-ray and millimeter/submillimeter observations from protostars,
coordinated with a hard X-ray observation, will unravel the nonthermal
particle production and triggering mechanism of protostellar flares.</description>
</item>
<item>
<title> Effects of Fully Relativistic Condition on Electron Cyclotron Maser Emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...944...37Z</link>
<description>The electron cyclotron maser (ECM) instability is a very important
nonthermal radiation mechanism. It has been developed by proposing
various electron distribution functions as well as the relativistic
resonance condition, called the semirelativistic correction. Taking
account of the relativistic effects of both the velocity distribution of
energetic electrons and the resonance condition, called the fully
relativistic correction, the present paper investigates the ECM
instability driven by a power-law electron distribution with a low-
energy cutoff. The results show that (1) both in the semirelativistic
and fully relativistic cases, the growth rate and relative frequency
bandwidth of ordinary (O) and extraordinary (X) modes show a positive
correlation with cutoff energy E &lt;SUB&gt; c &lt;/SUB&gt;, i.e., the peak
frequency decreases with increasing E &lt;SUB&gt; c &lt;/SUB&gt;; (2) the peak
frequency ratio (H &lt;SUB&gt;peak&lt;/SUB&gt;/F &lt;SUB&gt;peak&lt;/SUB&gt;) of the harmonic
and fundamental waves is always ~2; (3) compared with the
semirelativistic case, the fully relativistic case has a larger growth
rate (for both the O and X mode) and a smaller peak frequency (only for
the O mode) for energy &gt; 50 keV, and there is almost no difference at
lower energy for the two cases; (4) the peak frequency of the X1 mode
can be higher than its cutoff frequency in a strongly magnetized plasma,
implying that the X1 mode emission may escape more easily for a higher E
&lt;SUB&gt; c &lt;/SUB&gt; and stronger magnetic field. These results can be helpful
for us to understand better the physics of radio bursts from the Sun and
other objects.</description>
</item>
<item>
<title> Possible Application to Quasiperiodic Pulsations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...943L..19S</link>
<description>Magnetohydrodynamic (MHD) waves are often invoked to interpret
quasiperiodic pulsations (QPPs) in solar flares. We study the response
of a straight flare loop to a kink-like velocity perturbation using
three-dimensional MHD simulations and forward model the microwave
emissions using the fast gyrosynchrotron code. Kink motions with two
periodicities are simultaneously generated, with the long-period
component (P &lt;SUB&gt;L&lt;/SUB&gt; = 57 s) being attributed to the radial
fundamental kink mode and the short-period component (P &lt;SUB&gt;S&lt;/SUB&gt; =
5.8 s) to the first leaky kink mode. Forward modeling results show that
the two-periodic oscillations are detectable in the microwave
intensities for some lines of sight. Increasing the beam size to
(1)&lt;SUP&gt;2&lt;/SUP&gt; does not wipe out the microwave oscillations. We
propose that the first leaky kink mode is a promising candidate
mechanism to account for short-period QPPs. Radio telescopes with high
spatial resolutions can help distinguish between this new mechanism and
such customary interpretations as sausage modes.</description>
</item>
<item>
<title> Synchrotron Radiation by Galactic Cosmic-Ray Electrons</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...943..173O</link>
<description>The quiet Sun, i.e., in its nonflaring state or nonflaring regions,
emits thermal radiation from radio to ultraviolet. The quiet Sun also
produces nonthermal radiation observed in gamma rays due to interactions
of Galactic cosmic rays (GCRs) with the solar atmosphere and photons. We
report on a new component: the synchrotron emission by GCR electrons in
the solar magnetic field. To the best of our knowledge this is the first
time this emission has been theoretically claimed and modeled. We find
that the measured GCR electrons with energies from tens of GeV to a few
TeV produce synchrotron emission in X-rays, which is a few orders of
magnitude lower than current upper limits of the quiet Sun set by RHESSI
and FOXSI, with no energy losses included. For a radially decreasing
solar magnetic field we find the expected synchrotron intensity to be
almost constant in the solar disk, to peak in the close proximity of the
Sun, and to quickly drop away from the Sun. We also estimate the
synchrotron emission from radio to gamma rays, and we compare it with
current observations, especially with LOFAR. While it is negligible from
radio to UV compared to the solar thermal radiation, this emission can
potentially be observed at high energies with NuSTAR and more promising
future FOXSI observations. This could potentially allow for constraining
GCR densities and magnetic-field intensities at the Sun. This study
provides a more complete description and a possible new way for
understanding the quiet Sun and its environment.</description>
</item>
<item>
<title> Probing, Statistics, and Implications</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...943..160F</link>
<description>A strong coronal magnetic field, when present, manifests itself as
bright microwave sources at high frequencies produced by the
gyroresonant (GR) emission mechanism in thermal coronal plasma. The
highest frequency at which this emission is observed is proportional to
the absolute value of the strongest coronal magnetic field on the line
of sight. Although no coronal magnetic field larger than roughly 2000 G
has been expected, recently a field at least 2 times larger has been
reported. Here, we report on a search for and a statistical study of
such strong coronal magnetic fields using high-frequency GR emission. A
historic record of spatially resolved microwave observations at high
frequencies, 17 and 34 GHz, is available from the Nobeyama
RadioHeliograph for a period covering more than 20 yr (1995-2018). Here,
we employ this data set to identify sources of bright GR emission at 34
GHz and perform a statistical analysis of the identified GR cases to
quantify the strongest coronal magnetic fields during two solar cycles.
We found that although active regions with a strong magnetic field are
relatively rare (less than 1% of all active regions), they appear
regularly on the Sun. These active regions are associated with prominent
manifestations of solar activity.</description>
</item>
<item>
<title> Study of Radio Transients from the Quiet Sun during an Extremely Quiet Time</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...943..122M</link>
<description>In this work, we study a class of recently discovered meter-wave solar
transients referred to as Weak Impulsive Narrowband Quiet Sun Emission
(WINQSEs). Their strength is a few percent of the quiet Sun background
and is characterized by their very impulsive, narrowband, and ubiquitous
presence in quiet Sun regions. Mondal et al. (2020) hypothesized that
these emissions might be the radio counterparts of nanoflares, and their
potential significance warrants detailed studies. Here we present an
analysis of data from an extremely quiet time and with improved
methodology over the previous work. As before, we detect numerous
WINQSEs, which we have used for their further characterization. Their
key properties, namely, their impulsive nature and ubiquitous presence
in the quiet Sun, are observed in these data as well. Interestingly, we
also find some of the observed properties to differ significantly from
the earlier work. With this demonstration of routine detection of
WINQSEs, we hope to engender interest in the larger community to build a
deeper understanding of WINQSEs.</description>
</item>
<item>
<title> Imaging-spectroscopy of a band-split type II solar radio burst with the Murchison Widefield Array</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...670A.169B</link>
<description>Type II solar radio bursts are caused by magnetohydrodynamic (MHD)
shocks driven by solar eruptive events such as coronal mass ejections
(CMEs). Often, both fundamental and harmonic bands of type II bursts are
split into sub-bands, which are generally believed to be coming from
upstream and downstream regions of the shock; however, this explanation
remains unconfirmed. Here, we present combined results from imaging
analyses of type II radio burst band splitting and other fine structures
observed by the Murchison Widefield Array (MWA) and extreme ultraviolet
observations from Solar Dynamics Observatory (SDO)/Atmospheric Imaging
Assembly (AIA) on 28 September 2014. The MWA provides imaging-
spectroscopy in the range 80300 MHz with a time resolution of 0.5 s and
frequency resolution of 40 kHz. Our analysis shows that the burst was
caused by a piston-driven shock with a driver speed of 112 km
s&lt;SUP&gt;1&lt;/SUP&gt; and shock speed of 580 km s&lt;SUP&gt;1&lt;/SUP&gt;. We provide
rare evidence that band splitting is caused by emission from multiple
parts of the shock (as opposed to the upstream-downstream hypothesis).
We also examine the small-scale motion of type II fine structure radio
sources in MWA images, and suggest that this motion may arise because of
radio propagation effects from coronal turbulence, and is not due to the
physical motion of the shock location. We present a novel technique that
uses imaging spectroscopy to directly determine the effective length
scale of turbulent density perturbations, which is found to be 12 Mm.
The study of the systematic and small-scale motion of fine structures
may therefore provide a measure of turbulence in different regions of
the shock and corona.</description>
</item>
<item>
<title> Differences in physical properties of coronal bright points and their ALMA counterparts within and outside coronal holes</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...670A.146M</link>
<description>&lt;BR /&gt; Aims: This study investigates and compares the physical
properties, such as intensity and area, of coronal bright points (CBPs)
inside and outside of coronal holes (CHs) using the Atacama Large
Millimeter/submillimeter Array (ALMA) and Solar Dynamics Observatory
(SDO) observations. &lt;BR /&gt; Methods: The CBPs were analysed using the
single-dish ALMA Band 6 observations, combined with extreme-ultraviolet
(EUV) 193  filtergrams obtained by the Atmospheric Imaging Assembly
(AIA) and magnetograms obtained by the Helioseismic and Magnetic Imager
(HMI), both on board SDO. The CH boundaries were extracted from the
SDO/AIA images using the Collection of Analysis Tools for Coronal Holes
(CATCH) and CBPs were identified in the SDO/AIA, SDO/HMI, and ALMA data.
Measurements of brightness and areas in both ALMA and SDO/AIA images
were conducted for CBPs within CH boundaries and quiet Sun regions
outside CHs. Two equal size CBP samples, one inside and one outside CHs,
were randomly chosen and a statistical analysis was conducted. The
statistical analysis was repeated 200 times using a bootstrap technique
to eliminate the results based on pure coincidence. &lt;BR /&gt; Results: The
boundaries of five selected CHs were extracted using CATCH and their
physical properties were obtained. Statistical analysis of the measured
physical CBP properties using two different methods resulted in a lower
average intensity in the SDO/AIA data, or brightness temperature in the
ALMA data, for CBPs within the boundaries of all five CHs. Depending on
the CBP sample size, the difference in intensity for the SDO/AIA data,
and brightness temperature for the ALMA data, between the CBPs inside
and outside CHs ranged from between 2 and 4.5, showing a statistically
significant difference between those two CBP groups. We also obtained
CBP areas, where CBPs within the CH boundaries showed lower values for
the measured areas, with the observed difference between the CBPs inside
and outside CHs between 1 and 2 for the SDO/AIA data, and up to 3.5
for the ALMA data, indicating that CBP areas are also significantly
different for the two CBP groups. We also found that, in comparison to
the SDO/AIA data, the measured CBP properties in the ALMA data show a
small brightness temperature difference and a higher area difference
between the CBPs within and outside of CHs, possibly because of the
modest spatial resolution of the ALMA images. &lt;BR /&gt; Conclusions: Given
the measured properties of the CBPs, we conclude that the CBPs inside
CHs tend to be less bright on average, but also smaller in comparison to
those outside of CHs. This conclusion might point to the specific
physical conditions and properties of the local CH region around a CBP
limiting the maximum achievable intensity (temperature) and size of a
CBP. The need for the interferometric ALMA data is also emphasised to
get more precise physical CBP property measurements at chromospheric
heights.</description>
</item>
<item>
<title> Identifying the energy release site in a solar microflare with a jet</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...670A..56B</link>
<description>Context. One of the main science questions of the Solar Orbiter and
Parker Solar Probe missions deals with understanding how electrons in
the lower solar corona are accelerated and how they subsequently access
interplanetary space. &lt;BR /&gt; Aims: We aim to investigate the electron
acceleration and energy release sites as well as the manner in which
accelerated electrons access the interplanetary space in the case of the
SOL2021-02-18T18:05 event, a GOES A8 class microflare associated with a
coronal jet. &lt;BR /&gt; Methods: This study takes advantage of three
different vantage points, Solar Orbiter, STEREO-A, and Earth, with
observations drawn from eight different instruments, ranging from radio
to X-ray. Multi-wavelength timing analysis combined with UV/EUV imagery
and X-ray spectroscopy by Solar Orbiter/STIX (Spectrometer/Telescope for
Imaging X-rays) is used to investigate the origin of the observed
emission during different flare phases. &lt;BR /&gt; Results: The event under
investigation satisfies the classical picture of the onset time of the
acceleration of electrons coinciding with the jet and the radio type III
bursts. This microflare features prominent hard X-ray (HXR) nonthermal
emission down to at least 10 keV and a spectrum that is much harder than
usual for a microflare with  = 2.9  0.3. From Earth's vantage point,
the microflare is seen near the limb, revealing the coronal energy
release site above the flare loop in EUV, which, from STIX spectroscopic
analysis, turns out to be hot (i.e., at roughly the same temperature of
the flare). Moreover, this region is moving toward higher altitudes over
time (30 km s&lt;SUP&gt;1&lt;/SUP&gt;). During the flare, the same region
spatially coincides with the origin of the coronal jet. Three-
dimensional (3D) stereoscopic reconstructions of the propagating jet
highlight that the ejected plasma moves along a curved trajectory. &lt;BR
/&gt; Conclusions: Within the framework of the interchange reconnection
model, we conclude that the energy release site observed above-the-loop
corresponds to the electron acceleration site, corroborating that
interchange reconnection is a viable candidate for particle acceleration
in the low corona on field lines open to interplanetary space.</description>
</item>
<item>
<title> Structured type III radio bursts observed in interplanetary space</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...670A..20J</link>
<description>Context. The last few decades have seen numerous studies dedicated to
fine structures of type III radio bursts observed in the meter-decameter
wavelengths. Most of the explanations of the structured radio emission
involve the propagation of electron beams through the strongly
inhomogeneous plasma in the low corona. To date, only a few type III
bursts with fine structures, observed at hecto-kilometric wavelengths,
have been reported. &lt;BR /&gt; Aims: We report here the existence of
numerous structured type III radio bursts observed during the STEREO era
by all three WAVES instruments on board STEREO A, B, and Wind. The aim
of the study is to report and classify structured type III bursts, and
to present the characteristics of their fine structures. The final goal
is to try to understand the physical mechanism responsible for the
generation of structured radio emission. &lt;BR /&gt; Methods: In this study
we used data from all available spacecraft, specifically STEREO and
Wind. We employed 1D density models to obtain the speed of the source of
type III radio emission, the electron beam. We also performed a spectral
analysis of the fine structures in order to compare their
characteristics with the metric-decametric fine structures. &lt;BR /&gt;
Results: The presented similarities of the type III fine structures in
the metric to decametric and interplanetary wavelengths indicate that
the physical processes responsible for the generation of structured type
III radio bursts could be the same, at heights from the low corona to
the interplanetary range. We show that the observed structuring and
intermittent nature of the type III bursts can be explained by the
variation in the level of density fluctuations, at different distances
from the Sun.</description>
</item>
<item>
<title> Automatic detection of solar radio bursts in NenuFAR observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04055M</link>
<description>Solar radio bursts are some of the brightest emissions at radio
frequencies in the solar system. The emission mechanisms that generate
these bursts offer a remote insight into physical processes in solar
coronal plasma, while fine spectral features hint at its underlying
turbulent nature. During radio noise storms many hundreds of solar radio
bursts can occur over the course of a few hours. Identifying and
classifying solar radio bursts is often done manually although a number
of automatic algorithms have been produced for this purpose. The use of
machine learning algorithms for image segmentation and classification is
well established and has shown promising results in the case of
identifying Type II and Type III solar radio bursts. Here we present the
results of a convolutional neural network applied to dynamic spectra of
NenuFAR solar observations. We highlight some initial success in
segmenting radio bursts from the background spectra and outline the
steps necessary for burst classification.</description>
</item>
<item>
<title> Five years of solar observations with LOFAR station in Baldy</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04054D</link>
<description>We present exemplary observations of solar radio bursts collected in
2017  2021 with the use of LOFAR station PL612 located in Baldy
(Poland), operating in local mode. In that period, the Sun was observed
for 1190.3 hours over 235 days. We gathered high time (8 ms) and
frequency (0.4 MHz) resolution spectra in the band 10  250 MHz. Despite
the fact that this period can be characterized with relatively low solar
activity, we managed to observe quite a large number of various bursts.
Detailed analysis of these events will undoubtedly contribute to
expanding our knowledge about physical properties of solar activity.
Additionally, a single LOFAR station can be used to continuously monitor
radio bursts in order to analyze the mechanisms affecting the so-called
space weather.</description>
</item>
<item>
<title> A method for the automatic detection of solar type III radio bursts with Wind/Waves</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04053W</link>
<description>Solar type III radio bursts have a characteristic signature in
frequency-time dynamic spectrograms and provide important insight into
the dynamics of the Sun and solar wind. Direct physical inferences of
the source electrons or their propagation can be made, but radio
observations typically contain multiple emission sources which must be
accounted for. As well as this, the emission feature of interest must be
selected, which can be problematic if done manually, particularly with a
large amount of data. The WAVES instrument onboard the Wind spacecraft
has accumulated almost thirty years of solar and terrestrial
observations, with the majority from L1. Our previous work (Waters et
al., 2021b) has focused on the extraction of terrestrial auroral
kilometric radiation (AKR) from the Wind/WAVES data, and the removal of
noise. In this study we use a similar concept, separating the radio
sources by the measured signal variability during a spacecraft spin, but
focusing on the parameter space containing interplanetary (IP) type III
bursts below 1 MHz. Using an inverse threshold of the spin variability
metric and a signal-to-noise ratio (SNR) threshold, the radio data is
filtered to return mostly Type III emission above 200 kHz. Integrating
the flux density between 500-1045 kHz and choosing a threshold of 1 
109 W sr1 to select start times of Type III bursts between 1995 and
2021 yields the detection of 120560 events. Annual event occurrence
shows good correlation with yearly-averaged sunspot number across the
two solar cycles examined here (P=0.94). Evaluating classification
statistics of the selection via visual examination of a random sample of
50 days of Wind data returns a true positive rate of 0.9 and a positive
predictive value of 0.4, indicating that the majority of observed Type
III bursts are returned. This technique thus provides an initial step to
broad statistical examination of the physical properties of Type III
bursts using observations from Wind/WAVES or other instruments.</description>
</item>
<item>
<title> a constellation of CubeSats around the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04052W</link>
<description>One of the greatest challenge facing current space weather monitoring
operations is forecasting the arrival of coronal mass ejections (CMEs)
and Solar Energetic Particles (SEPs) within their Earth-Sun propagation
timescales. Current campaigns mainly rely on extreme ultra-violet and
white light observations to create forecasts, missing out many potential
events that may be hazardous to Earth's infrastructure undetectable at
these wavelengths. Here we introduce the SURROUND mission, a
constellation of CubeSats each with identical radio spectrometers, and
the results of the initial Phase-0 study for the concept. The main goal
of SURROUND is to monitor and track solar radio bursts (SRBs), widely
utilised as a useful diagnostic for space weather activity, and
revolutionise current forecasting capabilities. The Phase-0 study
concludes that SURROUND can achieve its mission objectives using 3 - 5
spacecraft using current technologies with feasible SEP and CME
forecasting potential: a first for heliospheric monitors.</description>
</item>
<item>
<title> Solar/stellar atmospheric tomography with mm-radio snapshot spectroscopic imaging</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04051M</link>
<description>Millimeter (mm) frequencies are primarily sensitive to thermal emission
from layers across the stellar chromosphere up to the transition region,
while metrewave (radio) frequencies probe the coronal heights. Together
the mm and radio band spectroscopic snapshot imaging enables the
tomographic exploration of the active atmospheric layers of the cool
main-sequence stars (spectral type: FGKM), including our Sun. Sensitive
modern mm and radio interferometers let us explore solar/stellar
activity covering a range of energy scales at sub-second and sub-MHz
resolution over wide operational bandwidths. The superior uv-coverage of
these instruments facilitate high dynamic range imaging, letting us
explore the morphological evolution of even energetically weak events on
the Sun at fine spectro-temporal cadence. This article will introduce
the current advancements, the data analysis challenges and available
tools. The impact of these tools and novel data in field of
solar/stellar research will be summarised with future prospects.</description>
</item>
<item>
<title> Auroral emissions and inner magnetospheric dynamics during Earth's response to the 28th October 2021 Coronal Mass Ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2023pre9.conf04047W</link>
<description>On 28th October 2021 the Sun released a large Coronal Mass Ejection
(CME) in Earth's direction. An X1.0 class solar flare and a rare ground
level enhancement (GLE) were observed, along with bright solar radio
bursts. Here we examine data from the near-Earth environment to
investigate the terrestrial response to this solar event, using newly
accessible Wind Auroral Kilometric Radiation (AKR) observations. The CME
arrival is tracked at ~1 AU using remote radio observations from Wind,
along with in-situ interplanetary magnetic field (IMF) and solar wind
measurements from OMNI. Geomagnetic activity is studied with SYM-H,
SuperMAG and PC indices. The auroral response is monitored for the first
time with Wind AKR observations from L1 (Lagrange point 1), UV auroral
emissions and field-aligned current densities, exploring the AKR source
location and inner magnetospheric dynamics. We thus quantify the
timeline for solar windmagnetosphereionosphere coupling and address
the visibility of AKR sources from Wind's position on the dayside at L1.</description>
</item>
<item>
<title> Deriving Large Coronal Magnetic Loop Parameters Using LOFAR J Burst Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298....7Z</link>
<description>Large coronal loops around one solar radius in altitude are an important
connection between the solar wind and the low solar corona. However,
their plasma properties are ill-defined, as standard X-ray and UV
techniques are not suited to these low-density environments. Diagnostics
from type J solar radio bursts at frequencies above 10 MHz are ideally
suited to understand these coronal loops. Despite this, J-bursts are
less frequently studied than their type III cousins, in part because the
curvature of the coronal loop makes them unsuited for using standard
coronal density models. We used LOw-Frequency-ARray (LOFAR) and Parker
Solar Probe (PSP) solar radio dynamic spectrum to identify 27 type III
bursts and 27 J-bursts during a solar radio noise storm observed on 10
April 2019. We found that their exciter velocities were similar,
implying a common acceleration region that injects electrons along open
and closed magnetic structures. We describe a novel technique to
estimate the density model in coronal loops from J-burst dynamic
spectra, finding typical loop apex altitudes around 1.3 solar radius. At
this altitude, the average scale heights were 0.36 solar radius, the
average temperature was around 1 MK, the average pressure was 0.7
mdyncm&lt;SUP&gt;2&lt;/SUP&gt;, and the average minimum magnetic field strength was
0.13 G. We discuss how these parameters compare with much smaller
coronal loops.</description>
</item>
<item>
<title> Simulating Solar Radio Bursts Using Generative Adversarial Networks</title>
<link>https://ui.adsabs.harvard.edu/abs/2023SoPh..298....6S</link>
<description>Solar flares are one of the most extreme drivers of space weather in our
solar system. The impulsive solar radio emission associated with a solar
flare is known as a solar radio burst (SRB). They are generally studied
in dynamic spectra and are classified into five major spectral classes,
ranging from Type I to Type V, based on their form and frequency, and
time duration. Due to their intricate characterisation, generating a
training set for object-detection and classification models of such
phenomena is a difficulty in machine learning. Current algorithms
implement parametric modelling where the quantity, grouping, intensity,
drift rate, heterogeneity, start-end frequency and start-end time of
Type-III and Type-II radio bursts are all random. However, this model
does not factor in the true shape or general features seen in real
dynamic spectra observations of the Sun, which can be crucial when
training classification or object-detection algorithms. In this
research, we introduce a methodology named a Generative Adversarial
Network (GAN) for generating realistic SRB simulations. By using real
examples of Type-III and Type-II SRB data, we can train GANs to generate
images almost comparable to real observed data. Furthermore, we evaluate
the results of the generated model using human perception, then we
compare and contrast the results using a metric known as the Frchet
Inception Distance.</description>
</item>
<item>
<title> VLF Signal Variations Seen in the Bucharest Observatory Recordings</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RoAJ...33..239B</link>
<description>This paper presents a new instrument setup at the Bucharest Observatory
of the Astronomical Institute of the Romanian Academy, as well as
preliminary results using this setup. It consists of records of VLF
(very low frequency) perturbations using a superSID instrument. During
March and December 2022 various mounts and settings tests have been
performed. Starting October we obtained satisfactory data. We report on
detecting the signature of moderate to intense solar flares (M and
Xclass). In this configuration, the Cclass solar flares are less
distinguishable from the background noise.</description>
</item>
<item>
<title> Observations of Ionospheric Clutter at Near Equatorial High Frequency Radar Stations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RemS...15..603C</link>
<description>The temporal variation of received clutter and noise at a pair of
oceanographic high frequency radars (HFR) operating near the geomagnetic
equator in the Republic of Palau is investigated. Oceanographic HFRs
process range-gated Doppler spectra from groundwave signals that are
backscattered from the ocean's surface to derive maps of ocean currents.
The range performance of the radars exhibited a regular diurnal signal
which is determined to be a result of both ionospheric clutter and
noise. The increased Clutter plus Noise Floor (C+NF) decreases the
Signal to Clutter plus Noise Ratio (SCNR) which, in turn, reduces the
range and quality of ocean surface current measurement. Determining the
nature and origin of this degradation is critical to QA/QC of existing
HFR deployments as well as performance predictions of future
installations. Nighttime impacts are most severe and negatively affect
ocean surface current measurements as low SCNR is found to extend across
the Doppler spectra at all ranges, challenging the ability of HFR to map
the ocean surface current. Daytime degradation is less severe and
presents itself in a way consistent with independent observations of
ionospheric clutter, specifically the diurnal temporal pattern and range
where the C+NF features occur. A timeseries analysis of SCNR and C+NF is
pursued to understand this relationship using received range-dependent
Doppler spectra and C+NF features using image segmentation techniques.
Clutter plus noise features are classified into daytime, nighttime, and
no-noise feature types. The diurnal structure and variability of these
features are examined, and the occurrences of each feature type are
calculated. The occurrences are compared with space weather indices
including a measure of geomagnetic activity, namely the EE (Equatorial
Electro Jet) index (determined from magnetometers measuring the earth's
magnetic field), as well as solar impacts using the F10.7 solar radio
clutter index to assess the relationship of ionospheric conditions with
HFR ocean surface current measurement.</description>
</item>
<item>
<title> Progress in the Study of Decameter-Wavelength Solar Radio Emission with Ukrainian Radio Telescopes. Part 1. (Invited paper)</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RPRA...28...95S</link>
<description>Subject and Purpose. Results are presented of the solar corona
investigations performed with the world famous Ukrainian radio
telescopes. The work has been aimed at offering a consistent review of
recent achievements in observations of a variety of low-frequency radio
emissions from the Sun. Methods and Methodology. The studies of the
quiet (thermal) and sporadic (burst-like) radio emissions from the Sun
have been car- ried out with the decameter-wavelength radio telescopes
UTR-2, GURT and URAN-2. Specific features of the low-frequency solar
radio emissions from a variety of sources are presented, with
characterization of the optimized techniques that were applied in each
case for evaluating physical parameters of the corona in the areas of
decameter-wavelength radio wave generation. Results. The analysis of
temporal, frequency and spatial characteristics of solar radio emissions
has allowed suggesting a number of models for the coronal electron
density distribution, and evaluating magnetic field strengths in the
corona. Also, our experimental results have proven to be consistent with
the observational data obtained in different frequency ranges and with
the use of both ground based and space-borne instruments. Conclusions.
The radio observations performed with Ukrainian radio telescopes have
permitted studying, with high temporal, fre- quency and spatial
resolutions, solar radio frequency emissions from various localized
sources. Along with the large effective area and high sensitivity of the
antennas, this permits application of a wide range of methods and tools
aimed at detecting and analyzing solar bursts, of both strong and weak
intensity, against the background of terrestrial interference of natural
or artificial origin</description>
</item>
<item>
<title> Estimation of Solar Observations with the Five-hundred-meter Aperture Spherical Radio Telescope (FAST)</title>
<link>https://ui.adsabs.harvard.edu/abs/2023RAA....23a1001Q</link>
<description>We present the estimation of solar observation with the Five-hundred-
meter Aperture Spherical radio Telescope (FAST). For both the quiet Sun
and the Sun with radio bursts, when pointing directly to the Sun, the
total power received by FAST would be out of the safe operational range
of the signal chain, even resulting in damage to the receiver. As a
conclusion, the Sun should be kept at least ~2 away from the main beam
during observations at ~1.25 GHz. The separation for lower frequency
should be larger. For simplicity, the angular separation between the
FAST beam and the Sun is suggested to be ~5 for observations at 200 MHz
or higher bands.</description>
</item>
<item>
<title> Deciphering Radio Emission from Solar Coronal Mass Ejections using High-fidelity Spectropolarimetric Radio Imaging</title>
<link>https://ui.adsabs.harvard.edu/abs/2023PhDT........27K</link>
<description>Solar coronal mass ejections (CMEs) are large-scale expulsions of plasma
and magnetic field from the Sun into the heliosphere and are the most
important driver of space weather. The geo-effectiveness of a CME is
primarily determined by its magnetic field strength and topology. The
evolution of CMEs while propagating through the corona and the
heliosphere complicates the prediction/extrapolation of the vector
magnetic field of the CMEs near the Earth based essentially on
photospheric measurements. Hence, the measurement of CME magnetic
fields, both in the corona and heliosphere, is essential for improving
space weather forecasting. Although CMEs are routinely observed by
white-light coronagraphs, these observations cannot provide a direct
measure of the CME-entrained vector magnetic fields. Observations at
radio wavelengths, however, can provide several remote measurement tools
for estimating both strength and topology of the CME magnetic fields.
Among them, gyrosynchrotron (GS) emission produced by mildly-
relativistic electrons trapped in CME magnetic fields is one of the
promis- ing methods to estimate magnetic field strength and other plasma
parameters of CMEs at lower and middle coronal heights. However, GS
emissions from some parts of the CME are much fainter than the quiet Sun
emission and require high dynamic range (DR) imaging for their
detection. This thesis presents a state- of-the-art calibration and
imaging algorithm capable of routinely producing high DR
spectropolarimetric snapshot solar radio images using data from a new
technology radio telescope, the Murchison Widefield Array (MWA). This
allows us to detect much fainter GS emissions from CME plasma at much
higher coronal heights than before. For the first time, robust circular
polarization measurements have been jointly used with total intensity
measurements to constrain the GS model parameters, which has
significantly improved the robustness of the estimated GS model
parameters. A piece of observational evidence is also found that the
routinely used homogeneous and isotropic GS models may not always be
sufficient to model the observations. In the future, with more sensitive
measurements from the upcoming new generation telescopes and physics-
based forward models, it should be possible to relax some of these
assumptions and make this method more robust for estimating CME plasma
parameters at coronal heights.</description>
</item>
<item>
<title> The Relationship of the Intensity of the SCR Proton Flux with the Parameters of Type II Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023OAP....36..161I</link>
<description>112 solar proton events (SPEs) were processed for the period from
November 24, 2000 to December 20, 2014, which were accompanied by type
II radio bursts. For the analysis, used original records of solar radio
emission from a solar radio spectrograph in the range of 25180 MHz, as
well as original records of the flux intensity proton of solar cosmic
rays (SCR) protons I&lt;SUB&gt;p&lt;/SUB&gt; with energy E&lt;SUB&gt;p&lt;/SUB&gt; in the range
&gt; 0.8-850 MeV according to data from the GOES series of devices. In this
case, superimposed proton events were always separated and identified
with the corresponding solar proton flares, and the maximum proton flux
intensity I&lt;SUB&gt;p&lt;/SUB&gt; of superimposed proton events was determined
from the level of the previous proton event. &lt;P /&gt;Based on data from the
solar radio spectrograph, regression models were obtained for 91 type II
bursts that established the relationship between the frequency drift
velocity V&lt;SUB&gt;i,j&lt;/SUB&gt; and the frequency of type II bursts
f&lt;SUB&gt;i,j&lt;/SUB&gt;, and for 73 type II bursts it was possible to obtain
regression models which established the relationship between the
intensity of type II bursts I&lt;SUB&gt;i,j&lt;/SUB&gt; and type II burst frequency
f&lt;SUB&gt;i,j&lt;/SUB&gt; in the range 25-180 MHz. Detailed studies have shown
that the intensity of type II bursts I&lt;SUB&gt;i,j&lt;/SUB&gt;, as well as the
frequency drift velocity V&lt;SUB&gt;i,j&lt;/SUB&gt;, strongly depends on the
frequency of type II burst f&lt;SUB&gt;i,j&lt;/SUB&gt; and monotonically changes
with time t&lt;SUB&gt;i&lt;/SUB&gt; along the harmonics of type II bursts. &lt;P /&gt;As a
result, the relationship between the maximum values of the SCR proton
flux intensity I&lt;SUB&gt;p&lt;/SUB&gt; and the calculated values of the frequency
drift velocity V&lt;SUB&gt;i,j&lt;/SUB&gt; and intensity of type II bursts
I&lt;SUB&gt;i,j&lt;/SUB&gt; was investigated. A comparative analysis showed that the
relationship between the intensity of the SCR proton flux I&lt;SUB&gt;p&lt;/SUB&gt;
and the intensity of type II bursts I&lt;SUB&gt;i,j&lt;/SUB&gt; is much stronger
than with the frequency drift velocity V&lt;SUB&gt;i,j&lt;/SUB&gt;, where the
correlation coefficient r is 0.82 and 0.71, respectively, for protons
with energies E&lt;SUB&gt;p&lt;/SUB&gt; &gt; 30 MeV. The relationship between the
proton flux intensity I&lt;SUB&gt;p&lt;/SUB&gt; and the frequency drift velocity
V&lt;SUB&gt;i,j&lt;/SUB&gt; and the intensity of type II bursts I&lt;SUB&gt;i,j&lt;/SUB&gt; was
also studied as a function of the proton energy E&lt;SUB&gt;p&lt;/SUB&gt; and the
frequency f&lt;SUB&gt;i,j&lt;/SUB&gt; of type II radio bursts. It was shown that the
strongest relationship between the intensity of the SCR proton flux
I&lt;SUB&gt;p&lt;/SUB&gt; with the frequency drift velocity V&lt;SUB&gt;i&lt;/SUB&gt; and with
the intensity of type II bursts I&lt;SUB&gt;i,j&lt;/SUB&gt; is observed with
subrelativistic SCR protons with energies E&lt;SUB&gt;p&lt;/SUB&gt; in the range &gt;
30-100 MeV and for type II radio bursts at a frequency f&lt;SUB&gt;i,j&lt;/SUB&gt;
in the range 40-160 MHz.</description>
</item>
<item>
<title> Interferometric Observations of the Quiet Sun at Decameter Wavelengths Under Strong Radio Frequency Interference</title>
<link>https://ui.adsabs.harvard.edu/abs/2023OAP....36..131S</link>
<description>Studies of the quiet Sun radio emission were carried out in a wide range
of wavelengths from extremely short up to decameter ones. At the longest
wavelengths, the measurements of angular sizes of the solar corona were
previously carried out using the UTR-2 radio telescope in the scanning
mode. We have developed a simple interferometric technique for measuring
the angular diameter of an extended radio source. It uses a set of
interferometers formed from the antenna sections of the north-south and
east-west arms of the UTR-2 radio telescope to measure the size of the
quiet Sun in the equatorial and polar directions. The first
interferometric observations with this approach were carried out using
the receivers and software of the URAN interferometers back in 2014.
That study allowed us to determine equatorial and polar solar sizes at
the fixed frequencies of 20 and 25 MHz. To expand the frequency range of
the studies in the following observations, we used broadband digital
DSPZ receivers in the correlation mode. However, in the daytime,
broadband observations are complicated by radio frequency interference
of various types, which often significantly exceed the level of wanted
signals. To limit the effect of RFI, software has been developed that
automatically detects and mitigates narrowband and impulse interference
in a recorded signal. The paper describes the methods of RFI mitigation
and criteria for the degree of signal clearing, which are used in this
software. We also present the measurement results of the angular
parameters of the quiet Sun radio emission, which were obtained by the
interferometric method in the frequency range of 10 - 30 MHz. The
observations were carried out during the minimum of solar activity in
2018 - 2020.</description>
</item>
<item>
<title> Self-organized criticality in solar GeV flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.518.3959P</link>
<description>The Sun emits significant flares in X-ray, ultraviolet, and radio
wavelengths. It is thought to originate from the magnetic reconnection
activity, which is capable of accelerating particles to high energies.
The magnetic process can be described by the avalanche model of self-
organized criticality (SOC), and it is evidenced by the observation.
Here, we study the frequency distribution of fluence, peak flux, and
duration time for solar GeV flares detected first by Fermi-Large Area
Telescope. Their cumulative distributions show a power-law behaviour.
The exponents are also consistent with those derived from the
observations at low-energy bands, and follow the predictions of the
fractal-diffuse SOC model. In the meantime, the waiting time shows
power-law distribution, and agrees a non-stationary Poission process. We
then explore the correlation between energy (fluence) and duration time
using a two-variable regression analysis. The correlation is found to be
$T_{\rm Duration} \propto F_{\rm GeV}^{0.38\pm 0.08}$ with the solar GeV
flare sample, which is comparable to that of the solar X-ray flares and
gamma-ray bursts (GRBs) and could be understood in an SOC model. These
facts suggest that, similar to the physical process accounting for the
X-ray emission of solar flares and prompt emission of GRBs, magnetic
reconnection may still dominate the energy-release process and particle
acceleration for solar flares at GeV energies.</description>
</item>
<item>
<title> Solar radio-frequency reflectivity and localization of FRB from solar reflection</title>
<link>https://ui.adsabs.harvard.edu/abs/2023MNRAS.518.2119W</link>
<description>The radiation of a fast radio burst (FRB) reflects from the Moon and
Sun. If a reflection is detected, the time interval between the direct
and reflected signals constrains the source to a narrow arc on the sky.
If both Lunar and Solar reflections are detected these two arcs
intersect, narrowly confining the location on the sky. A previous paper
calculated reflection by the Moon. Here, we calculate the reflectivity
of the Sun in the 'flat Sun' approximation as a function of angle of
incidence and frequency. The reflectivity is high at low frequencies
($\lessapprox 100\,$MHz) and grazing incidence (angles 60), but
exceeds 0.1 for frequencies $\lessapprox 80\,$ MHz at all angles.
However, the intense thermal emission of the Solar corona likely
precludes detection of the Solar reflection of even MJy Galactic bursts
like FRB 200428.</description>
</item>
<item>
<title> Rediscovering the observations of solar prominences from 1906 to 1957 recorded at the Madrid Astronomical Observatory</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JSWSC..13....5A</link>
<description>The Madrid Astronomical Observatory implemented a solar observation
program from 1876 to 1986. In addition to sunspots, the observers at
this observatory recorded other solar features such as prominences. In
this work, we have consulted the documentary sources of the Madrid
Astronomical Observatory (the information is not digitally available),
digitized the records of the observers on the annual number of
prominences, and constructed a homogeneous series of the total and
hemispheric annual number of prominences with heights of 25 and more
for the period 1906-1957. To evaluate the quality of the data and assess
their potential, we have compared the Madrid prominence series with the
number of prominences recorded by the Astronomical Observatory of the
University of Coimbra and other time series such as the sunspot number
index, solar radio flux at 10.7 cm, and sunspot areas. We have also
analyzed the hemispheric prominence numbers and the asymmetry index. We
obtained the strongest correlation between Madrid and Coimbra prominence
series (r = 0.7), whereas the correlations between the Madrid prominence
series and the other solar activity time series are similar (r  0.6).
In addition, we found that the correlation coefficient between the
Madrid prominence series and the sunspot number is lower than that from
the Coimbra prominence series and the sunspot number. We suggest that
these differences are a consequence of the way prominences were counted
in the Madrid Astronomical Observatory.</description>
</item>
<item>
<title> The effects of solar radio bursts on frequency bands utilised by the aviation industry in Sub-Saharan Africa</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JSWSC..13....4M</link>
<description>Solar radio bursts have been associated with a number of disruptions in
avionic systems. The objective of this work is to develop solar radio
burst interference thresholds which account for the technical
specifications of aviation-related instrumentation, instrument operating
frequencies as well as industry stipulated error tolerances. Solar radio
bursts are suggested to be potentially hazardous when exceeding these
calculated thresholds. Particular attention is paid to the radio
altimeter, an important component in aviation safety. The thresholds
suggested in this work for VHF communication, GPS navigation receivers
and radio altimeter frequencies are; 10&lt;SUP&gt;2&lt;/SUP&gt;, 10&lt;SUP&gt;3&lt;/SUP&gt;, and
10&lt;SUP&gt;4&lt;/SUP&gt; sfu respectively. Solar radio burst interference (for
solar radio bursts above 10&lt;SUP&gt;4&lt;/SUP&gt; sfu) is shown to result in large
errors (64-251 m) in the altitude estimates for the Frequency Modulated
Continuous Waves (FMCW) radio altimeter simulated in this work.</description>
</item>
<item>
<title> Ionospheric scintillation characteristics from GPS observations over Malaysian region after the 2011 Valentine's day solar flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2023JAGeo..17...79S</link>
<description>Ionospheric scintillations due to plasma irregularities can severely
affect the modern dynamic and technological systems whose operations
rely on satellite-based navigation systems. We investigate the
occurrence of ionospheric scintillation in the equatorial and low
latitude region over Malaysia after the 2011 Valentine's Day solar
flare. A network of three Global Ionospheric Scintillation and Total
Electron Content Monitor (GISTM) GSV4004B receivers with increasing
latitudes from the magnetic equator were used to monitor ionospheric
TEC, rate of change of TEC index (ROTI), and amplitude (S4) as well as
phase ( &lt;SUB&gt;&lt;/SUB&gt;) scintillation indices. The results show a
simultaneous sudden rise in S4 and  &lt;SUB&gt;&lt;/SUB&gt; along with a
significant depletion of TEC at all three locations. However, the
largest enhancement of scintillation indices accompanying a substantial
TEC depletion is observed at the farthest low latitude station (UNIMAS)
from the equator with values around 0.5, 0.3 rad, and 1 TECU,
respectively. The corresponding values at the near-equatorial station
(Langkawi; 0.4, 0.2 rad, and 3 TECU) and intermediate station (UKM;
0.45, 0.3 rad, and 5 TECU) are examined along with ROTI variations,
confirming the simultaneous occurrence of kilometer-scale and sub
kilometer scale irregularities during 17 and 18 February 2011. The
radiation effects of the solar flare on the ionosphere were prominently
recognized at the local nighttime hours (around 14:00 to 17:00 UT)
coinciding with the equatorial prereversal enhancement (PRE) time to
seed the equatorial plasma bubbles (EPBs) enhancement that resulted in
ionospheric irregularities over the low latitudes. The significant TEC
depletion seen in the signals from selected GPS satellites (PRNs 11, 19,
23, and 32) suggests plausible degradation in the performance of GPS-
based services over the Malaysian region. The study provides an
effective understanding of the post-flare ionospheric irregularities
during an episode of minor geomagnetic storm period and aligns with the
efforts for mitigating the scintillation effects in space-based radio
services over low latitudes.</description>
</item>
<item>
<title>The Sun Seen with the Atacama Large mm and sub-mm Array (ALMA) -First Results *</title>
<link>https://ui.adsabs.harvard.edu/abs/2023FrASS..1038626A</link>
<description>Not Available</description>
</item>
<item>
<title> Spatio-Temporal Comparisons of the Hydrogen-Alpha Line Width and ALMA 3 mm Brightness Temperature in the Weak Solar Network</title>
<link>https://ui.adsabs.harvard.edu/abs/2023FrASS...978405T</link>
<description>Comparisons between the Atacama Large Millimeter/sub-millimeter Array
(ALMA) 3mm emission and a range of optical and UV solar observations
have found the strongest correspondence between the width of the
hydrogen alpha line at 656.3nm and the 3mm brightness temperature.
Previous studies on the oscillatory power of \pmode{}s using ALMA Band 3
and Band 6 data in the 3 to 5 minute period bandpass have found a
confusing mix of results, with many reporting a complete lack of the
\pmode{} enhancement typically found in other chromospheric observables.
We study these issues using an extensive, publicly available coordinated
data set targeting a region of weak network flux near disk center at
time SOL2017-03-17T15:42-16:45. We focus on the Interferometric
Bidimensional Spectropolarimeter (IBIS) H-alpha and ALMA 3mm data
series. We confirm the strong correlation between the H-alpha line width
and the 3mm brightness temperature, but find a bimodal relation between
the two diagnostics, with a shallower slope of 7.4e-5\AA{}/K in cooler
regions and steeper slope of 1.2e-4\AA{}/K in hotter regions. The origin
of the bimodal distribution is unknown, but does hold for the duration
of the observations. Both slopes are steeper than a previously reported
value, but this is likely due to systematic differences in the analysis.
We then calculate the oscillatory power in the H-alpha and 3mm data. The
IBIS data clearly show the \pmode{} oscillations in spatially averaged
power spectra while the ALMA data do not. However, when we remove IBIS
data at times corresponding to the ALMA calibration windows, the
spatially averaged power spectra for the two data series are nearly
identical, with a Pearson correlation coefficient of 0.9895. Further,
the power in the two bands remains strongly correlated when the spatial
information is retained but the power is integrated over different
temporal frequency bands. We therefore argue that the lack of observed
\pmode{}s in the ALMA data may be predominantly due to spectral
windowing induced by the timing and duration of the calibration
observations. Finally, we find that spatial maps of oscillatory power at
3mm display the pattern of magnetic shadows and halos typically
displayed by other chromospheric diagnostics.</description>
</item>
<item>
<title> Effects of Solar Extreme Ultraviolet Radiation on Thermospheric Neutral Density.</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChJSS..43...87W</link>
<description>The Solar Extreme Ultraviolet (EUV) radiation is well known as the major
source of energy of driving the Earth atmospheric motion and
transformation. The 10.7 cm solar radio flux (F&lt;SUB&gt;10.7&lt;/SUB&gt;) instead
of EUV measurement is often used in the thermospheric neutral density
models, to calculate the thermosphere density and temperature. In this
paper, the continuous measurements of EUV from SEM instruments onboard
the SOHO satellite during 2001-2021 are directly compared with the
densities derived from accelerometers onboard the CHAMP, GRACE-A and
SWARM-C satellites, to reveal the essential relation between the solar
EUV radiation and the thermosphere density. It is found that the
correlation coefficients between the EUV data and the densities are
obviously greater than those between the F&lt;SUB&gt;10.7&lt;/SUB&gt; indexes and
the densities, which proves that the solar EUV radiation is the dominant
energy source of heating the thermosphere rather than the radio
radiation. From the liner regression slopes at different local time, it
is shown that the maximum value occurs at 15:00 LT (corresponding to
14:00-16:00 LT), while the minimum value at 01:00 LT (00:00-02:00 LT),
which confirms that the EUV radiation derives the diurnal variation of
the thermosphere. According to the statistical results from three
satellites with different orbital altitudes, it is indicated that in the
350~500 km altitude region, the heating effect of the EUV radiation at
lower altitude is more intense than that at higher altitude (considering
absolute variation). Because of the high spatial resolution of the
observation of three satellites, the difference in the effect of the EUV
radiation at various local time and geographic latitudes can be
concluded: the slope in sumer hemisphere, which is not described by the
thermosphere models such as DTM2000 and NRLMSISE00 yet. In order to
improve the modeling of the effect of the EUV radiation, the fitting
method of six-order spherical harmonics is proposed. Compared with the
formulas of the present models, the spherical harmonics are more
valuable in improving the model construction or correction of the EUV
effect and the thermosphere diurnal variation. At last, the physical
mechanism of statistical results is discussed by considering the energy
transmission and meridional circulation in the thermosphere.</description>
</item>
<item>
<title> High Dynamic Range Solar Radio Imaging Based on Deconvolution Using Prolate Spheroidal Wave Functions</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ChJSS..43...68Z</link>
<description>When the synthetic aperture radio telescope is used to observe the Sun,
faint sources can be revealed by accurately removing the bright extended
sources. Moreover, high dynamic range imaging can be achieved. The
inherent limitations of using image pixels as basis functions in the
CLEAN algorithm commonly used in radio astronomy lead to poor results
for modeling extended sources. In this paper, a deconvolution method
based on Prolate Spheroidal Wave Functions (PSWF) is applied to solar
radio imaging to overcome the limitations of the CLEAN algorithm. The
optimal PSWF orthogonal basis is determined by the Region of Interest
(ROI) in dirty images and UV coverage of the interferometric array. The
PSWF orthogonal basis is applied to the deconvolution of the solar radio
images observed by the uniform circular array to confirm its efficiency.
Moreover, the performance of the CLEAN algorithm and the method using
PSWF were quantitatively compared from two aspects including dynamic
range and fidelity. The faint sources in the residual dirty images
produced by deconvolution using PSWF orthogonal basis are closer to the
true model. A higher dynamic range imaging can also be obtained by using
PSWF.</description>
</item>
<item>
<title> Solar Coronal Density Turbulence and Magnetic Field Strength at the Source Regions of Two Successive Metric Type II Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...943...43R</link>
<description>We report spectral and polarimeter observations of two weak, low-
frequency (85-60 MHz) solar coronal type II radio bursts that occurred
on 2020 May 29 within a time interval 2 minutes. The bursts had fine
structures, and were due to harmonic plasma emission. Our analysis
indicates that the magnetohydrodynamic shocks responsible for the first
and second type II bursts were generated by the leading edge (LE) of an
extreme-ultraviolet flux rope/coronal mass ejection (CME) and
interaction of its flank with a neighboring coronal structure,
respectively. The CME deflected from the radial direction by 25 during
propagation in the near-Sun corona. The estimated power spectral density
and magnetic field strength (B) near the location of the first burst at
heliocentric distance r  1.35 R &lt;SUB&gt;&lt;/SUB&gt; are 2  10&lt;SUP&gt;-3&lt;/SUP&gt;
W&lt;SUP&gt;2&lt;/SUP&gt;m and 1.8 G, respectively. The corresponding values for
the second burst at the same r are 10&lt;SUP&gt;-3&lt;/SUP&gt; W&lt;SUP&gt;2&lt;/SUP&gt;m and
0.9 G. The significant spatial scales of the coronal turbulence at the
location of the two type II bursts are 62-1 Mm. Our conclusions from
the present work are that the turbulence and magnetic field strength in
the coronal region near the CME LE are higher compared to the
corresponding values close to its flank. The derived estimates of the
two parameters correspond to the same r for both the CME LE and its
flank, with a delay of 2 minutes for the latter.</description>
</item>
<item>
<title> The First Flare Observation with a New Solar Microwave Spectrometer Working in 35-40 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2023ApJ...942L..11Y</link>
<description>The microwave spectrum contains valuable information about solar flares.
Yet, the present spectral coverage is far from complete and broad data
gaps exist above 20 GHz. Here we report the first flare (the X2.2 flare
on 2022 April 20) observation of the newly built Chashan Broadband Solar
millimeter spectrometer (CBS) working from 35 to 40 GHz. We use the CBS
data of the new Moon to calibrate, and the simultaneous NoRP data at 35
GHz to cross-calibrate. The impulsive stage has three local peaks with
the middle one being the strongest and the maximum flux density reaches
~9300 solar flux unit at 35-40 GHz. The spectral index of the CBS data
( &lt;SUB&gt;C&lt;/SUB&gt;) for the major peak is mostly positive, indicating the
gyrosynchrotron turnover frequency ( &lt;SUB&gt; t &lt;/SUB&gt;) goes beyond 35-40
GHz. The frequency  &lt;SUB&gt; t &lt;/SUB&gt; is smaller yet still larger than 20
GHz for most of the other two peaks according to the spectral fittings
with NoRP-CBS data. The CBS index manifests the general rapid-hardening-
then-softening trend for each peak and gradual hardening during the
decay stage, agreeing with the fitted optically thin spectral index (
&lt;SUB&gt;tn&lt;/SUB&gt;) for  &lt;SUB&gt; t &lt;/SUB&gt; &lt; 35 GHz. In addition, the obtained
turnover frequency ( &lt;SUB&gt; t &lt;/SUB&gt;) during the whole impulsive stage
correlates well with the corresponding intensity (I &lt;SUB&gt; t &lt;/SUB&gt;)
according to a power-law dependence ( ${I}_{t}\propto {\nu }_{t}^{4.8}$
) with a correlation coefficient of 0.82. This agrees with earlier
studies on flares with low turnover frequency (17 GHz), yet it is being
reported for the first time for events with a high turnover frequency
(20 GHz).</description>
</item>
<item>
<title> The 18-19 March 2022 series of &lt;SUP&gt;3&lt;/SUP&gt;He-rich events observed by Solar Orbiter at 0.36 au compared with EUV, X-ray, and radio observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669L..16M</link>
<description>Context. During the first close perihelion pass of Solar Orbiter, a
series of impulsive &lt;SUP&gt;3&lt;/SUP&gt;He-rich solar particle events was
observed on 18-19 March 2022 from a distance of 0.36 au. In addition to
the energetic particle, radio, and X-ray data from Solar Orbiter, the
events were observed in radio and/or extreme ultraviolet by STEREO-A,
SDO, Wind, and Parker Solar Probe. &lt;BR /&gt; Aims: Observations of the
event series along with remote sensing of flaring and radio emission
with only small timing delays due to the close distance allow the
association with energetic particles to be determined with much higher
accuracy than previously possible from 1 au. &lt;BR /&gt; Methods: By
comparing the onsets of type-III bursts with the arrival of electrons of
tens of keV at Solar Orbiter only a few minutes later, it can be seen
that, overall, each of the more intense type-III bursts was associated
with an electron and ion injection. Extreme ultraviolet data show that
the times of the type-III bursts coincide with emission from a small
(approximately Earth-sized) loop to the west of a nearby active region.
&lt;BR /&gt; Results: The energetic particle spectra and abundances show
typical properties of impulsive &lt;SUP&gt;3&lt;/SUP&gt;He-rich flares and, when
combined with the remote sensing observations, establish that the
particle-accelerating mechanism in this series of events operates near
the solar surface in association with magnetic loops, and in the absence
of other phenomena such as jets and small coronal mass ejections. &lt;P
/&gt;Movie associated to Fig. 4 is available at &lt;A href="https://www.aanda.
org/10.1051/0004-6361/202245576/olm"&gt;https://www.aanda.org&lt;/A&gt;.</description>
</item>
<item>
<title> Flares detected in ALMA single-dish images of the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A.156S</link>
<description>Context. The millimeter and submillimeter radiation of solar flares is
poorly understood. Without spatial resolution, millimeter emission
cannot be easily compared to flare emission in other wavelengths. Though
the Atacama Large Millimeter-submillimeter Array (ALMA) offers
sufficient resolution for the first time, ALMA cannot be used on demand
to observe when a flare occurs, and when used as an interferometer, its
field of view is smaller than an active region. &lt;BR /&gt; Aims: We used
readily available large-scale single-dish ALMA observations of solar
millimeter flares and compared them to well-known features observed in
other wavelengths. The properties of these other flare emissions,
correlating in space and time, could then be used to interpret the
millimeter brightenings and vice versa. The aim is to obtain reliable
associations limited by the time and space resolution of single-dish
observations. &lt;BR /&gt; Methods: Ordinary interferometric ALMA observations
require single-dish images of the full Sun for calibration. We collected
such observations at 3 mm and 1 mm and searched for millimeter
brightenings during times listed in a flare catalog. &lt;BR /&gt; Results: All
of the flares left a signature in millimeter waves. We found five events
with nine or more images that could be used for comparison in time and
space. The millimeter brightenings are associated with a variety of
flare features in cool (H, 304 ), intermediate (171 ), and hot (94 )
lines. In several cases, the millimeter brightening peaked at the
footpoint of a hot flare loop. In other cases the peak of the millimeter
brightening coincided with the top or footpoint of an active H
filament. We also found correlations with post-flare loops and the tops
of a hot loop. In some images, the millimeter radiation peaked at
locations where no feature in the selected lines was found. &lt;BR /&gt;
Conclusions: The wide field of view provided by the single-dish ALMA
observations allowed for a complete overview of the flare activity in
millimeter waves for the first time. The associated phenomena often
changed in type and location during the flare. The variety of phenomena
detected in these millimeter observations may explain the sometimes
bewildering behavior of millimeter flare emissions previously observed
without spatial resolution.</description>
</item>
<item>
<title> Deep solar ALMA neural network estimator for image refinement and estimates of small-scale dynamics</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A.106E</link>
<description>Context. The solar atmosphere is highly dynamic, and observing the
small-scale features is valuable for interpretations of the underlying
physical processes. The contrasts and magnitude of the observable
signatures of small-scale features degrade as angular resolution
decreases. &lt;BR /&gt; Aims: The estimates of the degradation associated with
the observational angular resolution allows a more accurate analysis of
the data. &lt;BR /&gt; Methods: High-cadence time-series of synthetic
observable maps at  = 1.25 mm were produced from three-dimensional
magnetohydrodynamic Bifrost simulations of the solar atmosphere and
degraded to the angular resolution corresponding to observational data
with the Atacama Large Millimeter/sub-millimeter Array (ALMA). The deep
solar ALMA neural network estimator (Deep-SANNE) is an artificial neural
network trained to improve the resolution and contrast of solar
observations. This is done by recognizing dynamic patterns in both the
spatial and temporal domains of small-scale features at an angular
resolution corresponding to observational data and correlated them to
highly resolved nondegraded data from the magnetohydrodynamic
simulations. A second simulation, previously never seen by Deep-SANNE,
was used to validate the performance. &lt;BR /&gt; Results: Deep-SANNE
provides maps of the estimated degradation of the brightness temperature
across the field of view, which can be used to filter for locations that
most probably show a high accuracy and as correction factors in order to
construct refined images that show higher contrast and more accurate
brightness temperatures than at the observational resolution. Deep-SANNE
reveals more small-scale features in the data and achieves a good
performance in estimating the excess temperature of brightening events
with an average of 94.0% relative to the highly resolved data, compared
to 43.7% at the observational resolution. By using the additional
information of the temporal domain, Deep-SANNE can restore high
contrasts better than a standard two-dimensional deconvolver technique.
In addition, Deep-SANNE is applied on observational solar ALMA data, for
which it also reveals eventual artifacts that were introduced during the
image reconstruction process, in addition to improving the contrast. It
is important to account for eventual artifacts in the analysis. &lt;BR /&gt;
Conclusions: The Deep-SANNE estimates and refined images are useful for
an analysis of small-scale and dynamic features. They can identify
locations in the data with high accuracy for an in-depth analysis and
allow a more meaningful interpretation of solar observations.</description>
</item>
<item>
<title> Using the slope of the brightness temperature continuum as a diagnostic tool for solar ALMA observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A.105E</link>
<description>Context. The intensity of radiation from the solar atmosphere at
millimetre wavelengths is closely related to the plasma temperature, and
the formation height of the radiation is wavelength dependent. It
follows from this that the slope of the intensity continuum, or the
brightness temperature continuum, samples the local gradient of the gas
temperature of the sampled layers in the solar atmosphere. &lt;BR /&gt; Aims:
We aim to show the added information and diagnostics potential of the
solar atmosphere that comes with measuring the slope of the brightness
temperature continuum. &lt;BR /&gt; Methods: We used solar observations from
the Atacama Large Millimeter/sub-millimeter Array (ALMA) and estimated
and predicted the slope using a numerical three-dimensional radiation-
magnetohydrodynamic simulation. The slope was estimated by the
differences between observables at wavelengths corresponding to
different sub-bands at opposite sides of the ALMA receiver band 3
(2.8-3.2 mm) and band 6 (1.20-1.31 mm). &lt;BR /&gt; Results: The sign of the
brightness temperature slope indicates temperature changes with
increasing height at the sampled layers. A positive sign implies an
increase in temperature, while a negative sign implies a temperature
decrease. The differences in brightness temperature between the sub-
bands across the field of view of the simulation typically span from
0.4 kK to 0.75 kK for band 3 and 0.2 kK to 0.3 kK at band 6. The
network patches are dominated by large positive slopes, while the quiet-
Sun region shows a mixture of positive and negative slopes. As the slope
of the continuum is coupled to the small-scale dynamics, a negative
slope is seen typically under quiet-Sun conditions as a result of
propagating shock waves and the corresponding post-shock regions. The
temporal evolution of the slopes can therefore be used to identify
shocks. The observability of the slope of the brightness temperatures is
estimated at bands 3 and 6 for different angular resolutions
corresponding to ALMA observations. The simulations also show that the
intensity of the radiation at bands 3 and 6 can simultaneously originate
from several major components at different heights, which is strongly
dependent on the small-scale dynamics and is seen in both quiet-Sun and
network patches. Our in-depth analysis of selected shock waves that
propagating upward in the atmosphere shows that the delay of shock
signatures between two wavelengths (e.g., bands 6 and 3) does not
necessarily reflect the propagation speed of the shock front, but might
be cause by the rate of change in opacity of higher layers at these
wavelengths. &lt;BR /&gt; Conclusions: The slope of the brightness temperature
continuum sampled at different ALMA receiver sub-bands serves as an
indicator of the slope of the local plasma temperature at the sampled
heights in the atmosphere. This offers new diagnostic possibilities for
measuring the underlying physical properties of small-scale dynamic
features and thus contributes to the understanding of these features and
the related transport of energy and heat in the chromosphere.</description>
</item>
<item>
<title> Interferometric imaging of the type IIIb and U radio bursts observed with LOFAR on 22 August 2017</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A..52D</link>
<description>Context. The Sun is the source of different types of radio bursts that
are associated with solar flares, for example. Among the most frequently
observed phenomena are type III solar bursts. Their radio images at low
frequencies (below 100 MHz) are relatively poorly studied due to the
limitations of legacy radio telescopes. &lt;BR /&gt; Aims: We study the
general characteristics of types IIIb and U with stria structure solar
radio bursts in the frequency range of 20-80 MHz, in particular the
source size and evolution in different altitudes, as well as the
velocity and energy of electron beams responsible for their generation.
&lt;BR /&gt; Methods: In this work types IIIb and U with stria structure radio
bursts are analyzed using data from the LOFAR telescope including
dynamic spectra and imaging observations, as well as data taken in the
X-ray range (GOES and RHESSI satellites) and in the extreme ultraviolet
(SDO satellite). &lt;BR /&gt; Results: In this study we determined the source
size limited by the actual shape of the contour at particular
frequencies of type IIIb and U solar bursts in a relatively wide
frequency band from 20 to 80 MHz. Two of the bursts seem to appear at
roughly the same place in the studied active region and their source
sizes are similar. It is different in the case of another burst, which
seems to be related to another part of the magnetic field structure in
this active region. The velocities of the electron beams responsible for
the generation of the three bursts studied here were also found to be
different.</description>
</item>
<item>
<title> a novel remote sensing approach for coronal loops</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A..28M</link>
<description>Type U radio bursts are impulsive coherent radio emissions produced by
the Sun that indicate the presence of subrelativistic electron beams
propagating along magnetic loops in the solar corona. In this work, we
present the analysis of a type U radio burst that was exceptionally
imaged on 2011 March 22 by the Nanay Radioheliograph (NRH) at three
different frequencies (298.7, 327.0, and 360.8 MHz). Using a novel
modelling approach, we show for the first time that the use of high-
resolution radio heliograph images of type U radio bursts can be
sufficient to both accurately reconstruct the 3D morphology of coronal
loops (without recurring to triangulation techniques) and to fully
constrain their physical parameters. At the same time, we can obtain
unique information on the dynamics of the accelerated electron beams,
which provides important clues as to the plasma mechanisms involved in
their acceleration and as to why type U radio bursts are not observed as
frequently as type III radio bursts. We finally present plausible
explanations for a problematic aspect related to the apparent lack of
association between the modeled loop as inferred from radio images and
the extreme-ultraviolet (EUV) structures observed from space in the same
coronal region.</description>
</item>
<item>
<title> The first gradual solar energetic particle event with an enhanced &lt;SUP&gt;3&lt;/SUP&gt;He abundance on Solar Orbiter</title>
<link>https://ui.adsabs.harvard.edu/abs/2023A&amp;A...669A..13B</link>
<description>The origin of &lt;SUP&gt;3&lt;/SUP&gt;He abundance enhancements in gradual solar
energetic particle (SEP) events remains largely unexplained. Two
mechanisms have been suggested: the reacceleration of remnant flare
material by coronal mass ejection (CME)-driven shocks in interplanetary
space, and concomitant activity in the corona. We explore the first
gradual SEP event with enhanced &lt;SUP&gt;3&lt;/SUP&gt;He abundance that was
observed by Solar Orbiter. The event started on 2020 November 24 and was
associated with a relatively fast halo CME. During the event, the
spacecraft was at 0.9 au from the Sun. The event-averaged
&lt;SUP&gt;3&lt;/SUP&gt;He/&lt;SUP&gt;4&lt;/SUP&gt;He abundance ratio is 24 times higher than
the coronal or solar wind value, and the timing of the &lt;SUP&gt;3&lt;/SUP&gt;He
intensity was similar to that of other species. We inspected available
imaging, radio observations, and the spacecraft magnetic connection to
the CME source. The most probable cause of the enhanced &lt;SUP&gt;3&lt;/SUP&gt;He
abundance apparently are residual &lt;SUP&gt;3&lt;/SUP&gt;He ions remaining from a
preceding long period of &lt;SUP&gt;3&lt;/SUP&gt;He-rich SEPs on 2020 November
17-23.</description>
</item>
<item>
<title> Classification of Solar Radio Spectrum Based on Swin Transformer</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....9....9C</link>
<description>Solar radio observation is a method used to study the Sun. It is very
important for space weather early warning and solar physics research to
automatically classify solar radio spectrums in real time and judge
whether there is a solar radio burst. As the number of solar radio burst
spectrums is small and uneven, this paper proposes a classification
method for solar radio spectrums based on the Swin transformer. First,
the method transfers the parameters of the pretrained model to the Swin
transformer model. Then, the hidden layer weights of the Swin
transformer are frozen, and the fully connected layer of the Swin
transformer is trained on the target dataset. Finally, parameter tuning
is performed. The experimental results show that the method can achieve
a true positive rate of 100%, which is more accurate than previous
methods. Moreover, the number of our model parameters is only 20
million, which is 80% lower than that of the traditional VGG16
convolutional neural network with more than 130 million parameters.</description>
</item>
<item>
<title> Self-Supervised Learning for Solar Radio Spectrum Classification</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....8..656L</link>
<description>Solar radio observation is an important way to study the Sun. Solar
radio bursts contain important information about solar activity.
Therefore, real-time automatic detection and classification of solar
radio bursts are of great value for subsequent solar physics research
and space weather warnings. Traditional image classification methods
based on deep learning often require considerable training data. To
address insufficient solar radio spectrum images, transfer learning is
generally used. However, the large difference between natural images and
solar spectrum images has a large impact on the transfer learning
effect. In this paper, we propose a self-supervised learning method for
solar radio spectrum classification. Our method uses self-supervised
training with a self-masking approach in natural language processing.
Self-supervised learning is more conducive to learning the essential
information about images compared with supervised methods, and it is
more suitable for transfer learning. First, the method pre-trains using
a large amount of other existing data. Then, the trained model is fine-
tuned on the solar radio spectrum dataset. Experiments show that the
method achieves a classification accuracy similar to that of
convolutional neural networks and Transformer networks with supervised
training.</description>
</item>
<item>
<title> Common Origin of Quasi-Periodic Pulsations in Microwave and Decimetric Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297..152K</link>
<description>Not Available</description>
</item>
<item>
<title> Storm-Time Relative Total Electron Content Modelling Using Machine Learning Techniques</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RemS...14.6155A</link>
<description>Accurately predicting total electron content (TEC) during geomagnetic
storms is still a challenging task for ionospheric models. In this work,
a neural-network (NN)-based model is proposed which predicts relative
TEC with respect to the preceding 27-day median TEC, during storm time
for the European region (with longitudes 30W-50E and latitudes
32.5N-70N). The 27-day median TEC (referred to as median TEC),
latitude, longitude, universal time, storm time, solar radio flux index
F10.7, global storm index SYM-H and geomagnetic activity index Hp30 are
used as inputs and the output of the network is the relative TEC. The
relative TEC can be converted to the actual TEC knowing the median TEC.
The median TEC is calculated at each grid point over the European region
considering data from the last 27 days before the storm using global
ionosphere maps (GIMs) from international GNSS service (IGS) sources. A
storm event is defined when the storm time disturbance index Dst drops
below 50 nanotesla. The model was trained with storm-time relative TEC
data from the time period of 1998 until 2019 (2015 is excluded) and
contains 365 storms. Unseen storm data from 33 storm events during 2015
and 2020 were used to test the model. The UQRG GIMs were used because of
their high temporal resolution (15 min) compared to other products from
different analysis centers. The NN-based model predictions show the
seasonal behavior of the storms including positive and negative storm
phases during winter and summer, respectively, and show a mixture of
both phases during equinoxes. The model's performance was also compared
with the Neustrelitz TEC model (NTCM) and the NN-based quiet-time TEC
model, both developed at the German Aerospace Agency (DLR). The storm
model has a root mean squared error (RMSE) of 3.38 TEC units (TECU),
which is an improvement by 1.87 TECU compared to the NTCM, where an RMSE
of 5.25 TECU was found. This improvement corresponds to a performance
increase by 35.6%. The storm-time model outperforms the quiet-time model
by 1.34 TECU, which corresponds to a performance increase by 28.4% from
4.72 to 3.38 TECU. The quiet-time model was trained with Carrington
averaged TEC and, therefore, is ideal to be used as an input instead of
the GIM derived 27-day median. We found an improvement by 0.8 TECU which
corresponds to a performance increase by 17% from 4.72 to 3.92 TECU for
the storm-time model using the quiet-time-model predicted TEC as an
input compared to solely using the quiet-time model.</description>
</item>
<item>
<title> On some features of the solar proton event on 2021 October 28 - GLE73</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.517.2709C</link>
<description>In addition to several recent articles devoted to the rare event of
ground-level enhancement of the solar relativistic proton flux observed
on 2021 October 28 - GLE73, we study the 10-100 MeV solar energetic
particle (SEP) component of this event. Based on the Geostationary
Operational Environmental Satellite data for 26 GLEs recorded since
1986, we have formed a scatter plot displaying the ratio of the peak
fluxes of the $ $10 MeV ($J_{10}$) and $ $100 MeV ($J_{100}$) protons
and their energy spectra. Two extreme characteristics of the prompt
component of the SEP-GLE73 event were revealed: (1) very small $J_{10}$
and $J_{100}$ proton fluxes and (2) a very hard energetic spectrum in
the 10-100 MeV range. There are only two events with these
characteristics similar to SEP-GLE73, namely GLE40 (1989 July 25) and
GLE46 (1989 November 15). A correspondence was demonstrated between the
hard frequency spectrum of microwave radio bursts of initiating flares
and the hard SEP energy spectrum of these two and other GLEs. These
results suggest that the flare magnetic reconnection both in the
impulsive and post-eruption phases plays an important role in the
acceleration of the SEP-GLE protons.</description>
</item>
<item>
<title> Complex Type II Solar Radio Event on 4 July 2022</title>
<link>https://ui.adsabs.harvard.edu/abs/2022LatJP..59f..22K</link>
<description>On 4 July 2022, a complex low-frequency solar radio burst was observed
in Metshovi Radio Observatory of Aalto University. The radio burst was
observed at a frequency range between 20 and 80 MHz. In GOES
(Geostationary Operational Environmental Satellite) class, the event was
classified as C5.1. However, coronal mass ejection (CME) was not
associated to this event. The observed radio burst was a long-lasting
(~10 minutes) event, and it could be mainly classified as type II solar
radio event. Also type III solar events were observed before long-
lasting type II event. The event includes common frequency drifting
emission structures, both fundamental and harmonic structures, but also
rarely observed continuum-like or stationary structure. It is assumed
that the continuum-like radio emission structure is originated from the
stationary flare (coronal) loop, which was visible over the whole event.
The drifting emission structure means accelerated electrons, which are
produced by the shock related phenomena. The paper provides the
observations from this event on radio wavelength, and also soft-X-ray
regime and optical wavelength (AIA 171). In addition, a possible,
simplified scenario is presented for forming the drifting and continuum
solar radio emissions in type II solar burst.</description>
</item>
<item>
<title> Characterization and Climatological Modeling of Equatorial Ionization Anomaly (EIA) Crest Position</title>
<link>https://ui.adsabs.harvard.edu/abs/2022JGRA..12730798N</link>
<description>The Equatorial Ionization Anomaly (EIA) is characterized by strong
ionospheric gradients that complicate ionospheric modeling and
mitigation of ionospheric impact on Global Navigation Satellite System
applications. In this study, the variation of EIA crest locations as a
function of longitude and solar radio flux index F10.7 has been derived
and modeled. Seven years (2013-2019) of ionospheric NmF2 and in-situ ion
density data from Constellation Observing System for Meteorology
Ionosphere and Climate and Swarm-A satellites have been used. We find
that the distance between the northern and southern crest of EIA grows
slightly with increase of solar flux. The position of the crests of EIA
follows a wave number 4 structure with peak values at around 130, 0,
and 100E. At the altitude of Swarm-A (460 km), the equatorial crests
are found closer to the geomagnetic dip equator than they are at the
peak density height hmF2 (310 km) which may be due to the spatial
variations of geomagnetic field strength. Accordingly, two Crest
Position climatological Models have been developed, one for the F2 Peak
height (CPM_F2P) and the other one for Swarm-A height (CPM_SAH).</description>
</item>
<item>
<title> India's first radio telescope</title>
<link>https://ui.adsabs.harvard.edu/abs/2022JAHH...25..773O</link>
<description>India's first radio telescope was the Kalyan Array, a T-configuration
solar grating array erected near Bombay (Mumbai) in 1965. This was then
used until 1968 to monitor solar radio emission at 612 MHz. The antennas
from this radio telescope originally formed the E-W solar grating
interferometer invented by the Australian radio astronomer W.N. (Chris)
Christiansen, and were sited at Potts Hill in Sydney, a field station
Keywords: Govind Swarup, Potts Hill, W.N Christiansen, solar grating
arrays, Kalyan Array, coronal emission, radio plages, Ooty Radio
Telescope maintained by the CSIRO's Division of Radiophysics. In early
1953 Govind Swarup (along with R. Parthasarathy) went to Sydney on a
2-year Colombo Plan Fellowship, and was involved in reducing
observations made by this array and a companion N-S grating array. Then,
in 1954, Govind and Parthasarathy altered the array so that it could
operate at 500 MHz, and they used it to examine the extent of limb-
brightening at this frequency. When both arrays became surplus to
requirements in March 1955 Govind convinced the Division of Radiophysics
to donate the E-W array antennas to the Physical Research Laboratory in
New Delhi. This eventually occurred, and after some delay and the
transfer of the antennas to the Tata Institute of Fundamental Research
in Bombay they were erected nearby at Kalyan. In this paper I review
Govind Swarup's Sydney 'apprenticeship' and his substantial involvement
with the Potts Hill E-W solar grating array; his subsequent return to
India and intervals he then spent in the USA at Fort Davis (Harvard
University) and Stanford University (where he completed a solar radio
astronomy PhD); his return to India to found the Tata Institute's radio
astronomy group; erection of the solar grating array at Kalyan, and the
solar research that was carried out with it; and - finally - how the
Kalyan Array was always perceived as a training facility and forerunner
to the much more ambitious Ooty Radio Telescope.</description>
</item>
<item>
<title> Sunspot periodicity</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Gerb...18...92V</link>
<description>The Schwabe (~11 yr) value for the annual sunspot number is sometimes
uncritically applied to other measures of solar activity, direct and
indirect, including the 10.7 cm radio flux, the inflow of galactic
cosmic rays, solar flare frequency, terrestrial weather, and components
of space climate, with the risk of a resulting loss of information. The
ruling (Babcock) hypothesis and its derivatives link the sunspot cycle
to dynamo processes mediated by differential solar rotation, but despite
60 years of observation and analysis the ~11 yr periodicity remains
difficult to model; the possible contribution of planetary dynamics is
undergoing a revival. The various solar sequences that genuinely display
an~11 yr cycle stand to benefit from an understanding of its periodicity
that goes beyond statistical kinship. The outcome could ironically
prompt the demotion of sunspots from their dominant historical role in
favour of other possible indicators of solar cyclicity, such as the
solar wind flux and its isotopic signatures, even if they are less
accessible.</description>
</item>
<item>
<title> Aeronomic and Dynamic Correction of the Global Model GTEC for Disturbed Conditions</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62S..74S</link>
<description>An aeronomic and dynamic correction of the GTEC median global model of
the total electron content for disturbed conditions (Ap  15 nT) is
proposed. The GTEC global median model is developed for quiet conditions
(Ap &lt; 15 nT) as a function of the geographic coordinates, universal time
UT, day of the year, and solar activity level (the solar radio emission
flux F10.7). The model is based on a spherical harmonic analysis of the
GIM-TEC Global Ionospheric Maps (19962019) provided by the Jet
Propulsion Laboratory (NASA). The proposed GDMTEC global dynamic model
(Global Dynamic Model of TEC) consists of the GTEC median model updated
with several dynamic and aeronomic corrections related to formation of
the main ionospheric trough, position of the auroral ionization maximum
and changes of the thermospheric temperature and composition. The
advantage of the proposed corrections of the median model is the
independence of forecast of the data in real time from assimilation of
the current observational data. Testing of the model for disturbed
conditions shows an improvement of the forecast compared to the IRI-Plas
ionospheric reference model.</description>
</item>
<item>
<title> Assessment of long-term impact of solar activity on the ionosphere over an African equatorial GNSS station</title>
<link>https://ui.adsabs.harvard.edu/abs/2022EScIn..15.2109M</link>
<description>The level of solar activity and its influence on ionospheric variability
has received a focal interest among the ionospheric community. This
paper examines the impact of long-term solar activity on the ionosphere
over an African equatorial global navigation satellite system (GNSS)
station based on a large database of solar and ionospheric datasets. The
ionospheric total electron content (TEC) periodic variations,
climatology and its relation to solar activity are investigated through
wavelet analyses. It is observed that the magnitude and intensity of TEC
fluctuations measured by GNSS receivers vary substantially with solar
radiation intensity. To probe the processes accountable for the TEC
periodicities in the region, the wavelet analysis is undertaken by
considering solar indices (solar radio flux and sunspot number) and
observed TEC values. The results show a clear strong periodicity of 27
days in the ionospheric TEC, sunspots and F10.7 solar flux power
spectra, associated with the sun's 27 days rotation period. The
ultraviolet ray intensity and solar ionization were lower during the
solar maximum period (2013 to 2014) of solar cycle 24 compared to the
solar maximum period (2001 to 2002) of solar cycle 23, which is the key
factor for driving the decreasing trend in TEC between 1999 and 2017.
The ionospheric and solar climatology analysis indicates that
ionospheric TEC behaviour could be a good indicator of long-term solar
activity trend. A large mass of Africa lies within the equatorial and
low latitudes making the ionosphere over the region being highly
susceptible to low latitude electrodynamics. Results from this study
would support the concerted efforts towards developing a reliable
regional ionospheric forecasting model for technological applications
relying on spaced-based navigation and satellite services.</description>
</item>
<item>
<title> Monitoring solar activity during 23/24 solar cycle minimum through VLF radio signals</title>
<link>https://ui.adsabs.harvard.edu/abs/2022CoSka..52c.105K</link>
<description>Solar activity during solar minimum between 23&lt;SUP&gt;rd&lt;/SUP&gt; and
24&lt;SUP&gt;th&lt;/SUP&gt; solar cycle was inspected, based on solar X-ray
radiation listings from Geostationary Operational Environmental
Satellite (GOES) database. Periods of quiet solar conditions with low
background X radiation are particularly favourable for analysis and
exploration of low intensity solar flare events and their effects on
lower ionosphere. Low intensity solar flare events were monitored and
examined through Very Low Frequency (VLF) radio signals (3-30 kHz),
recorded by the use of Absolute Phase and Amplitude Logger system
(AbsPAL) operating at the Institute of Physics Belgrade, Serbia. For the
purposes of numerical modeling of low ionospheric response to low class
solar flare events, the Long Wave Propagation Capability (LWPC)
software, based on Wait's theory, was applied. Main results are
presented in this paper.</description>
</item>
<item>
<title> Connecting Loop-top and Footpoint Hard X-Ray Sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...941L..22K</link>
<description>The acceleration and transport of energetic electrons during solar
flares is one of the outstanding topics in solar physics. Recent X-ray
and radio imaging and spectroscopy observations have provided
diagnostics of the distribution of nonthermal electrons and suggested
that, in certain flare events, electrons are primarily accelerated in
the loop top and likely experience trapping and/or scattering effects.
By combining the focused particle transport equation with
magnetohydrodynamic (MHD) simulations of solar flares, we present a
macroscopic particle model that naturally incorporates electron
acceleration and transport. Our simulation results indicate that
physical processes such as turbulent pitch-angle scattering can have
important impacts on both electron acceleration in the loop top and
transport in the flare loop, and their influences are highly energy-
dependent. A spatial-dependent turbulent scattering with enhancement in
the loop top can enable both efficient electron acceleration to high
energies and transport of abundant electrons to the footpoints. We
further generate spatially resolved synthetic hard X-ray (HXR) emission
images and spectra, revealing both the loop-top and footpoint HXR
sources. Similar to the observations, we show that the footpoint HXR
sources are brighter and harder than the loop-top HXR source. We suggest
that the macroscopic particle model provides new insights into
understanding the connection between the observed loop-top and footpoint
nonthermal emission sources by combining the particle model with
dynamically evolving MHD simulations of solar flares.</description>
</item>
<item>
<title> Multiple Regions of Nonthermal Quasiperiodic Pulsations during the Impulsive Phase of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...940..137L</link>
<description>Flare-associated quasiperiodic pulsations (QPPs) in radio and X-ray
wavelengths, particularly those related to nonthermal electrons, contain
important information about the energy release and transport processes
during flares. However, the paucity of spatially resolved observations
of such QPPs with a fast time cadence has been an obstacle for us to
further understand their physical nature. Here, we report observations
of such a QPP event that occurred during the impulsive phase of a
C1.8-class eruptive solar flare using radio imaging spectroscopy data
from the Karl G. Jansky Very Large Array (VLA) and complementary X-ray
imaging and spectroscopy data. The radio QPPs, observed by the VLA in
the 1-2 GHz with a subsecond cadence, are shown as three spatially
distinct sources with different physical characteristics. Two radio
sources are located near the conjugate footpoints of the erupting
magnetic flux rope with opposite senses of polarization. One of the
sources displays a QPP behavior with a ~5 s period. The third radio
source, located at the top of the postflare arcade, coincides with the
location of an X-ray source and shares a similar period of ~25-45 s. We
show that the two oppositely polarized radio sources are likely due to
coherent electron cyclotron maser emission. On the other hand, the
looptop QPP source, observed in both radio and X-rays, is consistent
with incoherent gyrosynchrotron and bremsstrahlung emission,
respectively. We conclude that the concurrent, but spatially distinct
QPP sources must involve multiple mechanisms which operate in different
magnetic loop systems and at different periods.</description>
</item>
<item>
<title> Determination of the correlation coefficient of selected short-periodic comets of the Jupiter family and solar activity</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AASP...12....3S</link>
<description>The paper presents the study of the dependence between photometric
parameters of selected short-period comets of the Jupiter family and the
activity of the Sun. As a quantity of solar activity, we used the
sunspot area, the Wolf number, the annual mean solar radio flux, the
solar flare index (full disk), and the annual mean AA-index solar
activity. To study the correlation between cometary and solar activity
the Dobrovolsky method was used. It has been found no direct correlation
between the absolute stellar magnitude and the photometric parameter of
comets with individual parameters of solar activity. Moreover, the
correlation coefficients show that some comets are not associated with
solar activity.</description>
</item>
<item>
<title> Shock-accelerated electrons during the fast expansion of a coronal mass ejection</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...668A..15M</link>
<description>Context. Some of of the most prominent sources for energetic particles
in our Solar System are huge eruptions of magnetised plasma from the Sun
called coronal mass ejections (CMEs), which usually drive shocks that
accelerate charged particles up to relativistic energies. In particular,
energetic electron beams can generate radio bursts through the plasma
emission mechanism. The main types of bursts associated with CME shocks
are type II and herringbone bursts. However, it is currently unknown
where early accelerated electrons that produce metric type II bursts and
herringbones propagate and when they escape the solar atmosphere. &lt;BR /&gt;
Aims: Here, we investigate the acceleration location, escape, and
propagation directions of electron beams during the early evolution of a
strongly expanding CME-driven shock wave associated with herrinbgone
bursts. &lt;BR /&gt; Methods: We used ground-based radio observations from the
Nanay Radioheliograph combined with space-based extreme-ultraviolet and
white-light observations from the Solar Dynamics Observatory and and the
Solar Terrestrial Relations Observatory. We produced a three-dimensional
(3D) representation of the electron acceleration locations which,
combined with results from magneto-hydrodynamic (MHD) models of the
solar corona, was used to investigate the origin of the herringbone
bursts observed. &lt;BR /&gt; Results: Multiple herringbone bursts are found
close to the CME flank in plane-of-sky images. Some of these herringbone
bursts have unusual inverted J shapes and opposite drifting herringbones
also show opposite senses of circular polarisation. By using a 3D
approach combined with the radio properties of the observed bursts, we
find evidence that the first radio emission in the CME eruption most
likely originates from electrons that initially propagate in regions of
low Alfvn speeds and along closed magnetic field lines forming a
coronal streamer. The radio emission appears to propagate in the same
direction as a coronal wave in three dimensions. &lt;BR /&gt; Conclusions: The
CME appears to inevitably expand into a coronal streamer where it meets
ideal conditions to generate a fast shock which, in turn, can accelerate
electrons. However, at low coronal heights, the streamer consists of
exclusively closed field lines indicating that the early accelerated
electron beams do not escape. This is in contrast with electrons which,
in later stages, escape the corona so that they are detected by
spacecraft. &lt;P /&gt;Movies are available at &lt;A href="https://www.aanda.org/
10.1051/0004-6361/202244432/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> A Machine Learning-Based Method for Modeling TEC Regional Temporal-Spatial Map</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RemS...14.5579L</link>
<description>In order to achieve the high-accuracy prediction of the total electron
content (TEC) of the regional ionosphere for supporting the application
of satellite navigation, positioning, measurement, and controlling, we
proposed a modeling method based on machine learning (ML) and use this
method to establish an empirical prediction model of TEC for parts of
Europe. The model has three main characteristics: (1) The principal
component analysis (PCA) is used to separate TEC's temporal and spatial
variation characteristics and to establish its corresponding map, (2)
the solar activity parameters of the 12-month mean flux of the solar
radio waves at 10.7 cm (F10.712) and the 12-month mean sunspot number
(R12) are introduced into the temporal map as independent variables to
reflect the temporal variation characteristics of TEC, and (3) The
modified Kriging spatial interpolation method is used to achieve the
spatial reconstruction of TEC. Finally, the regression learning method
is used to determine the coefficients and harmonic numbers of the model
by using the root mean square error (RMSE) and its relative value
(RRMSE) as the evaluation standard. Specially, the modeling process is
easy to understand, and the determined model parameters are
interpretable. The statistical results show that the monthly mean values
of TEC predicted by the proposed model in this paper are highly
consistent with the observed values curve of TEC, and the RRMSE of the
predicted results is 12.76%. Furthermore, comparing the proposed model
with the IRI model, it can be found that the prediction accuracy of TEC
by the proposed model is much higher than that of the IRI model either
with CCIR or URSI coefficients, and the improvement is 38.63% and
35.79%, respectively.</description>
</item>
<item>
<title> Long-Term Relationship Between foF2 From China Ionospheric Stations and Solar Activity During the 24th Solar Activity Cycle</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RaSc...5707539C</link>
<description>This paper employs the complete data of six ionospheric observation
stations in China in the 24th solar activity cycle and researches the
variation of frequency of the F2 layer (foF2) and the relationship with
the solar activity indices. We discover that the dependence of foF2 on
the sunspot number (R) and the solar radio flux of 10.7 cm wavelength
(F10.7) is strongest in mid-solar years, and weakest in high solar
years. At the same time, the long-term variation trends of foF2, R and
F10.7 in the complete 24th solar activity cycle are analyzed using the
mutual information method in information theory. We utilize the linear
and nonlinear methods to compare the effects of long term change
relationship between foF2 and R during the rising and falling phases of
solar activity. The findings reveal that the sunspot number is more
suitable to depict the long-term trend of foF2 in China, and the
relationship between them is better described by nonlinear quasi-
polynomial. This result has important implications for improving foF2
forecasts and the prediction accuracy of some ionospheric models.</description>
</item>
<item>
<title> Prospects and challenges of numerical modelling of the Sun at millimetre wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...967878W</link>
<description>The Atacama Large Millimeter/submillimeter Array (ALMA) offers new
diagnostic possibilities that complement other commonly used diagnostics
for the study of our Sun. In particular, ALMA's ability to serve as an
essentially linear thermometer of the chromospheric gas at unprecedented
spatial resolution at millimetre wavelengths and future polarisation
measurements have great diagnostic potential. Solar ALMA observations
are therefore expected to contribute significantly to answering long-
standing questions about the structure, dynamics and energy balance of
the outer layers of the solar atmosphere. In this regard, current and
future ALMA data are also important for constraining and further
developing numerical models of the solar atmosphere, which in turn are
often vital for the interpretation of observations. The latter is
particularly important given the Sun's highly intermittent and dynamic
nature that involves a plethora of processes occurring over extended
ranges in spatial and temporal scales. Realistic forward modelling of
the Sun therefore requires time-dependent three-dimensional radiation
magnetohydrodynamics that account for non-equilibrium effects and,
typically as a separate step, detailed radiative transfer calculations,
resulting in synthetic observables that can be compared to observations.
Such artificial observations sometimes also account for instrumental and
seeing effects, which, in addition to aiding the interpretation of
observations, provide instructive tools for designing and optimising
ALMA's solar observing modes. In the other direction, ALMA data in
combination with other simultaneous observations enables the
reconstruction of the solar atmospheric structure via data inversion
techniques. This article highlights central aspects of the impact of
ALMA for numerical modelling for the Sun, their potential and
challenges, together with selected examples.</description>
</item>
<item>
<title> Rapid variations of Si IV spectra in a flare observed by interface region imaging spectrograph at a sub-second cadence</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...940945L</link>
<description>We report on observations of highly-varying Si IV 1402.77  line
profiles observed with the Interface Region Imaging Spectrograph (IRIS)
during the M-class flare from 2022 January 18 at an unprecedented 0.8 s
cadence. Moment analysis of this line observed in flare ribbon kernels
showed that the intensity, Doppler velocity, and non-thermal broadening
exhibited variations with periods below 10 s. These variations were
found to be correlated with properties of the Gaussian fit to a well-
resolved secondary component of the line redshifted by up to 70 km/s,
while the primary component was consistently observed near the rest
wavelength of the line. A particularly high correlation was found
between the non-thermal broadening of the line resulting from the moment
analysis and the redshift of the secondary component. This means that
the oscillatory enhancements in the line broadening were due to plasma
flows (away from the observer) with varying properties. A simple de-
projection of the Doppler velocities of the secondary component based on
a three-dimensional reconstruction of flare loops rooted in the kernel
suggests that the observed flows were caused by downflows and compatible
with strong condensation flows recently predicted by numerical
simulations. Furthermore, peaks of the intensity and the trends of
Doppler velocity of the Gaussian fit to the secondary component
(averaged in the ribbon) were found to correspond to one of the quasi-
periodic pulsations (QPPs) detected during the event in the soft X-ray
flux (as measured by the Geostationary Operational Environmental
Satellite, GOES) and the microwave radio flux (as measured by the
Expanded Owens Valley Solar Array, EOVSA). This result supports a
scenario in which the QPPs were driven by repeated magnetic
reconnection.</description>
</item>
<item>
<title> The "SPectrogram Analysis and Cataloguing Environment" (SPACE) Labelling Tool</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...901166L</link>
<description>The SPectrogram Analysis and Cataloguing Environment (SPACE) tool is an
interactive python tool designed to label radio emission features of
interest in a time-frequency map (called "dynamic spectrum"). The
program uses Matplotlib's Polygon Selector widget to allow a user to
select and edit an undefined number of vertices on top of the dynamic
spectrum before closing the shape (polygon). Multiple polygons may be
drawn on any spectrum, and the feature name along with the coordinates
for each polygon vertex are saved into a ".json" file as per the "Time-
Frequency Catalogue" (TFCat) format along with other data such as the
feature id, observer name, and data units. This paper describes the
first official stable release (version 2.0) of the tool.</description>
</item>
<item>
<title> Polarization Observations of a Split-band Type II Radio Burst from the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...940...80R</link>
<description>Using temporal observations of circular polarized harmonic plasma
emission from a split-band type II solar radio burst at 80 MHz, we
separately estimated the coronal magnetic field strengths (B) associated
with the lower (L) and upper (U) frequency bands of the burst. The
corresponding Stokes I and V data were obtained with the polarimeter
operating at the above frequency in the Gauribidanur observatory. The
burst was associated with a flare/coronal mass ejection on the solar
disk. Simultaneous spectral observations with the spectrograph there in
the frequency range 80-35 MHz helped to establish that the observed
polarized emission was from the harmonic component of the burst. The B
values corresponding to the polarized emission from the L and U bands at
80 MHz are B &lt;SUB&gt; L &lt;/SUB&gt;  1.2 G and B &lt;SUB&gt; U &lt;/SUB&gt;  2.4 G,
respectively. The different values of B for the observed harmonic
emission at the same frequency (80 MHz) from the two bands imply
unambiguously that the corresponding fundamental emission at 40 MHz must
have originated at different spatial locations. Two-dimensional radio
imaging observations of the burst with the radioheliograph in the same
observatory at 80 MHz indicate the same. As comparatively higher B is
expected behind a propagating shock due to compression as well as the
corresponding coronal regions being closer to the Sun, our results
indicate that the sources of L- and U-band emission should be located
ahead of and behind the associated coronal shock, respectively. These
are useful to understand the pre- and postshock corona as well as
locations of electron acceleration in a propagating shock.</description>
</item>
<item>
<title> First Millimeter Flares Detected from  Eridani with the Atacama Large Millimeter/submillimeter Array</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...939L...6B</link>
<description>We report the detection of three large millimeter flaring events from
the nearby Sun-like,  Eridani, found in archival Atacama Large
Millimeter/submillimeter Array (ALMA) 12 m and Atacama Compact Array
observations at 1.33 mm taken from 2015 January 17 to 18 and 2016
October 24 to November 23, respectively. This is the first time that
flares have been detected from a Sun-like star at millimeter
wavelengths. The largest flare among our data was detected in the ALMA
observations on 2015 January 17 from 20:09:10.4-21:02:49.3 UT with a
peak flux density of 28  7 mJy and a duration of 9 s. The peak
brightness of the largest flare is 3.4  0.9  10&lt;SUP&gt;14&lt;/SUP&gt; erg
s&lt;SUP&gt;-1 &lt;/SUP&gt;Hz&lt;SUP&gt;-1&lt;/SUP&gt;, a factor of &gt;50 times brighter than the
star's quiescent luminosity and &gt;10 brighter than solar flares observed
at comparable wavelengths. We find changes in the spectral index (F&lt;SUB&gt;
 &lt;/SUB&gt;   &lt;SUP&gt;  &lt;/SUP&gt;) at the flare peak, with  = 1.81  1.94 and
a lower limit on the fractional linear polarization Q/I = 0.08  0.12.
This positive spectral index is more similar to millimeter solar flares,
differing from M-dwarf flares also detected at millimeter wavelengths
that exhibit steeply negative spectral indices.</description>
</item>
<item>
<title> Radio Emission Variability of Supernova Remnants and a Possible Explanation of the Phenomenon</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ARep...66..953I</link>
<description>The flux densities and current spectra of plerions and combined
supernova remnants (SNRs): 3C58, 3C144, G11.2-0.3, G21.5-0.9, and 3C396
are determined on an artificial moon (AM) flux scale. The radio emission
variability of the objects on different time scales is studied by
multiple measurements using the RT-32 radio telescope at the Svetloe
Observatory, Institute of Applied Astronomy, Russian Academy of Sciences
and by mutual comparisons of the published measurement data, which have
been brought to a common system using the AM flux scale. The radio
emission from the SNRs displays both slow evolutionary variations and
rapid ones, nonstationary in time. The rapid variability of the SNRs has
features that are similar to those observed during solar flares. This
fact may testify to the identity of the physical mechanisms underlying
the rapid variability of the radio emission from plerions and from the
Sun. Field line reconnections are considered as such a common mechanism.</description>
</item>
<item>
<title> Magnetic Field and Density Models in the Zebra Source Region</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297..133Y</link>
<description>Using the double-plasma resonance model of solar radio zebras, we
analyze five models of the magnetic field and density in the zebra
source region. We present analytical relations of zebra-stripe
frequencies depending on the gyro-harmonic number. By fitting of
observed zebra-stripe frequencies using model frequencies, we find that
the determined gyro-harmonic number and corresponding magnetic field
depend on the model used. We show that all previously analyzed zebras,
where the absolute value of the difference between neighboring zebra-
stripe frequencies increases with respect to increasing frequency, can
be well fitted by the model with exponential dependencies of the
magnetic field and density or by the model with smaller gradients of
both of these variables. Although these models give different results,
their more sophisticated versions give more similar results. We also
present the models that can fit the zebras, if observed, where the
absolute value of the difference between neighboring zebra-stripe
frequencies decreases with respect to increasing frequency. We check all
these models by a fitting of the zebra-stripe frequencies observed in
the 21 June 2011 zebra event. In one model, although it reasonably
describes the conditions in the atmosphere above the active region, the
fit of the observed zebra-stripe frequencies could not be made.</description>
</item>
<item>
<title> Solar Radio-Burst Forecast Based on a Convolutional Neural Network</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297..130M</link>
<description>A solar radio burst is the enhancement of radio emission during the
release of solar magnetic energy. It is an important indicator of the
level of solar activity. In this paper, we propose a solar radio-burst
forecast model that takes the Solar and Heliospheric Observatory
(SOHO)/Michelson Doppler Imager (MDI) full-disk solar magnetograms as
inputs. The model takes advantage of a Convolutional Neural Network
(CNN) to automatically extract the effective feature information from
the input images. Through multiple trainings, the relationship between
the magnetic-field characteristics of the full-disk solar magnetograms
and the solar radio bursts is established, so it is possible to predict
the presence or absence of a solar radio burst on that day. The
experimental results demonstrate that the forecast Accuracy of the
proposed model is 0.875  0.007. The True Skill Statistic (TSS) is 0.723
 0.026, and the Heidke Skill Score (HSS) is 0.713  0.019. These
results indicate the strong reliability and wide applicability of the
forecast model proposed in this paper. The proposed model is also used
to predict solar type-II and type-III bursts, respectively. It is found
that the prediction performance for type-III bursts is better than that
of type-II bursts. The result is well explained from the differences of
their formation mechanisms.</description>
</item>
<item>
<title> Solar Flare and Radio Burst Effects on GNSS Signals and the Ionosphere During September 2017</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RaSc...5707418D</link>
<description>Strong solar flare events can occur even during the decay phase of the
solar cycle. During these events concurrent increases in the X-ray and
Enhanced UV (EUV) fluxes and solar radio bursts (SRBs) can be observed.
The SRBs cover a large range of frequencies including the L band, giving
rise to signal fades in the GNSS carrier-to-noise ratio and fluctuations
in its amplitude and phase. The increases in the X-ray, UV, and EUV
fluxes cause increase in the ionospheric D, E, and F region electron
densities. The aim of this work is to analyze the effects in the GNSS
signal, in the ionosphere and in the magnetic field H component of the
X9.3 and X1.3 solar flares that occurred on 06 and 07 September 2017,
respectively. Data from a network of six GNSS receivers, two
magnetometers, and four Digisondes are used in the analysis. Fades of
about 5 and 10 dB were observed in the signals of GNSS L1 and L2/L5
frequencies, respectively. Significant positioning errors, were observed
for the strongest X9.3 flare. A sudden increase in Total Electron
Content with the rates of 2.5-5.0 TECU/min was observed. An increase in
the E layer density gave origin to an increase in the Equatorial
Electrojet intensity, whose signatures were observed in the H component
of two magnetometers. Another observed effect was the ionospheric D
region density increase that caused disruption in the Digisonde signal.
As a consequence of the described effects, GNSS receivers may fail to
produce accurate navigation solution.</description>
</item>
<item>
<title> A New Position Calibration Method for MUSER Images</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RAA....22j5019Z</link>
<description>The Mingantu Spectral Radioheliograph (MUSER), a new generation of solar
dedicated radio imaging-spectroscopic telescope, has realized high-time,
high-angular, and high-frequency resolution imaging of the Sun over an
ultra-broadband frequency range. Each pair of MUSER antennas measures
the complex visibility in the aperture plane for each integration time
and frequency channel. The corresponding radio image for each
integration time and frequency channel is then obtained by inverse
Fourier transformation of the visibility data. However, the phase of the
complex visibility is severely corrupted by instrumental and propagation
effects. Therefore, robust calibration procedures are vital in order to
obtain high-fidelity radio images. While there are many calibration
techniques available-e.g., using redundant baselines, observing standard
cosmic sources, or fitting the solar disk-to correct the visibility data
for the above-mentioned phase errors, MUSER is configured with non-
redundant baselines and the solar disk structure cannot always be
exploited. Therefore it is desirable to develop alternative calibration
methods in addition to these available techniques whenever appropriate
for MUSER to obtain reliable radio images. In the case where a point-
like calibration source contains an unknown position error, we have for
the first time derived a mathematical model to describe the problem and
proposed an optimization method to calibrate this unknown error by
studying the offset of the positions of radio images over a certain
period of the time interval. Simulation experiments and actual
observational data analyses indicate that this method is valid and
feasible. For MUSER's practical data the calibrated position errors are
within the spatial angular resolution of the instrument. This
calibration method can also be used in other situations for radio
aperture synthesis observations.</description>
</item>
<item>
<title> A Study on Non-coplanar Baseline Effects for Mingantu Spectral Radioheliograph</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RAA....22j5010Y</link>
<description>As a dedicated solar radioheliograph, the MingantU SpEctral
RadioHeliograph (MUSER) has a maximum baseline of more than 3000 m and a
frequency range of 400 MHz-15 GHz. According to the classical radio
interferometry theory, the non-coplanar baseline effect (i.e., w-term
effect) would be considered and calibrated for such a radio instrument.
However, little previous literature made the qualitative or quantitative
analyses on w-term effects of solar radioheliograph in-depth. This study
proposes a complete quantitative analysis of w-term effects for the
MUSER. After a brief introduction of the MUSER, we systematically
investigate the baseline variations over a year and analyze the
corresponding variations of w-term. We further studied the effects of
the w-term in the imaging for the specified extended source, i.e., the
Sun. We discussed the possible effects of the w-term, such as image
distortion and so on. The simulated results show that the w-term is an
essential and unavoidable issue for solar radio imaging with high
spatial resolution.</description>
</item>
<item>
<title> Modulation of the solar microwave emission by sausage oscillations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.516.2292K</link>
<description>The modulation of the microwave emission intensity from a flaring loop
by a standing linear sausage fast magnetoacoustic wave is considered in
terms of a straight plasma slab with the perpendicular Epstein profile
of the plasma density, penetrated by a magnetic field. The emission is
of the gyrosynchrotron (GS) nature, and is caused by mildly relativistic
electrons that occupy a layer in the oscillating slab, i.e. the emitting
and oscillating volumes do not coincide. It is shown that the microwave
response to the linear sausage wave is highly non-linear. The degree of
the non-linearity, defined as a ratio of the Fourier power of the second
harmonic to the Fourier power of the principal harmonic, is found to
depend on the combination of the width of the GS source and the viewing
angle, and is different in the optically thick and optically thin parts
of the microwave spectrum. This effect could be considered as a
potential tool for diagnostics of the transverse scales of the regions
filled in by the accelerated electrons.</description>
</item>
<item>
<title> Searching for stellar flares from low-mass stars using ASKAP and TESS</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.516..540R</link>
<description>Solar radio emission at low frequencies (&lt;1 GHz) can provide valuable
information on processes driving flares and coronal mass ejections
(CMEs). Radio emission has been detected from active M dwarf stars,
suggestive of much higher levels of activity than previously thought.
Observations of active M dwarfs at low frequencies can provide
information on the emission mechanism for high energy flares and
possible stellar CMEs. Here, we conducted two observations with the
Australian Square Kilometre Array Pathfinder Telescope totalling 26 h
and scheduled to overlap with the Transiting Exoplanet Survey Satellite
Sector 36 field, utilizing the wide fields of view of both telescopes to
search for multiple M dwarfs. We detected variable radio emission in
Stokes I centred at 888 MHz from four known active M dwarfs. Two of
these sources were also detected with Stokes V circular polarization.
When examining the detected radio emission characteristics, we were not
able to distinguish between the models for either electron cyclotron
maser or gyrosynchrotron emission. These detections add to the growing
number of M dwarfs observed with variable low-frequency emission.</description>
</item>
<item>
<title> Characteristic Features of the Magnetic and Ionospheric Storms on December 2124, 2016</title>
<link>https://ui.adsabs.harvard.edu/abs/2022KPCB...38..262L</link>
<description>Solar storms accompanied by solar flares, coronal mass ejections, and
high-speed flows result in considerable disturbances in the
Suninterplanetary mediummagnetosphereionosphereatmosphereEarth
(internal geospheres) system. As a result, geospace storms with
synergistically interacting magnetic, ionospheric, atmospheric, and
electrical storms arise in our planet. Magnetic and ionospheric storms
have been studied for a long time, but atmospheric storms and electrical
storms have been studied considerably to a less extent. Geospace storms
and their components exhibit significant variability. It may be asserted
that no identical two storms exist. Therefore, a comprehensive study of
each new geospace storm and its manifestations and features is an urgent
scientific issue. This will contribute to a process of their adequate
simulation and, in the long term, forecasting. The purpose of this
article is to describe the observed features of the ionospheric and
magnetic storms accompanying the geospace storm on December 2124, 2016.
The state of the geomagnetic field has been observed via the fluxgate
magnetometer located at the Magnetometer Observatory of the Karazin
Kharkiv National University (4938' N, 3656' E). The dynamics of the
ionospheric plasma has been monitored by a vertical incidence Doppler
radar and a digisonde located at the Radio Physics Observatory of the
Karazin Kharkiv National University (4938' N, 3620' E). The Doppler
radar operate at 3.2 and 4.2 MHz; however, only measurements performed
at 3.2 MHz are given below, since a frequency of 4.2 MHz turned out to
be inefficient at nighttime when F2 layer critical frequency median
f&lt;SUB&gt;0 F2&lt;/SUB&gt;  2 MHz, which prevented signal reflection from the
ionosphere even at 3.2 MHz. Prior to the beginning of the magnetic storm
on December 20, 2016, the level of the H and D components rarely
exceeded 0.20.7 nT. The sudden commencement of a storm between 06:00
and 10:00 UTC virtually did not affect this level. During the second
half of the day on December 21, 2016, the level of exhibited sporadic
fluctuations increased from approximately 1 to 34 nT. During the next
few days, up to December 25, 2016, their level showed variations mostly
from approximately 1 nT to approximately 2 nT. Increases in the level
were predominantly observed in the period from 05:00 to 15:00 UTC for
the H component and from 10:00 to 20:00 UTC for the D component. The
weak (power 20 GJ/s and energy approximately 0.45 PJ) geospace storm in
the period of December 2124, 2016, was accompanied by a moderate
positive ionospheric storm, as well as by three negative ionospheric
storms, one of which was very strong, and the other two were strong and
moderate. The geospace storm was accompanied by a moderate magnetic
storm with an energy of approximately 2 PJ and a power of approximately
56 GW. The positive ionospheric storm barely affects the level of the
signal reflected from the ionosphere, whereas the reflected signal may
be very weak or totally absent during the negative ionospheric storms.
The positive ionospheric storm has a substantial effect on the Doppler
shift when the wave activity enhanced in the ionosphere. The relative
amplitude of disturbances in the electron density increases from a few
percent to approximately 50%, and their period increases from 612 to 40
min. It is impossible to follow wave activity during the negative
ionospheric storms. In the course of a long magnetic storm, the level of
D and H components in a subrange of 2001000 s of the period increased
from 0.20.3 and 0.30.5 nT to 1.02.0 and 1.01.8 nT, respectively. In
a subrange of 50200 s of the period, the corresponding levels increased
from 0.30.5 and 0.30.5 nT to 0.51.0 and 1.52.0 nT, respectively.
Within a subrange of 1050 s the period, the corresponding levels
increased from 0.050.06 and 0.100.15 nT to 0.200.30 and 0.51.0 nT,
respectively. Comparative studies of two geospace storms that occurred
on December 2124, 2016, and March 2123, 2017, show that their
ionospheric and magnetic effects are comparable, even if the storms are
different.</description>
</item>
<item>
<title> The Solar Activity Index for the Critical Frequency of the E-Layer at Subauroral Latitudes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62..582D</link>
<description>Based on the analysis of data from subauroral ionospheric stations
during daytime hours with low geomagnetic activity, it was found that
the index P = 0.5(F&lt;SUB&gt;1&lt;/SUB&gt; + F&lt;SUB&gt;81&lt;/SUB&gt;) is the optimal solar
activity index for the daily values of the E-layer critical frequency
foE, where F&lt;SUB&gt;1&lt;/SUB&gt; and F&lt;SUB&gt;81&lt;/SUB&gt; are the solar radio flux at
a wavelength of 10.7 cm on a given day and the average of this flux over
81 days. The standard deviations  of the foE dependence on P are at
their maximum for winter. The  value in this season for the Salekhard
and Lycksele stations, which are located at the Arctic Circle and near
it, is significantly greater than for the Leningrad station.
Substituting the P index into the IPG, IRI, or NeQuick models allows
these models to be used for the calculation of daily foE values. Based
on the preliminary analysis, it was found that the NeQuick model is more
accurate than the IPG and IRI models for winter and equinoxes. For
summer, these models have approximately the same accuracy with a slight
advantage of the IPG model. For the Salekhard and Lycksele stations in
winter at foE &lt; 2 MHz, even the NeQuick model underestimates the foE
values by approximately 0.2 MHz on average. The search for the causes of
this property of the ionosphere requires special consideration.</description>
</item>
<item>
<title> Medium-Term Forecast of Solar Activity From Daily Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62..539G</link>
<description>Empirical ionospheric models reflect the dependence of key ionospheric
characteristics on 12-month smoothed solar activity indices. These
indices are determined with a delay of 6 months relative to the current
time so the model implementation in real time is made with a forecast of
solar activity, whose errors affect the accuracy of the ionospheric
prediction. The 81-day smoothed proxy indices of solar activity can be
used for driving the ionospheric model in real time including daily
indices for the previous 40 days, an observation or forecast for the
current day, and a forecast for the subsequent 40 days. In this paper, a
method for predicting solar activity for 45 days (MSA45) is proposed,
which is equally suitable for use with F10.7 solar radio emission flux
indices and the SSN2 sunspot number. The model is based on the
similarity of data in the current phase of the solar cycle with indices
of solar activity in a relevant phase of the previous solar cycle. The
model input parameters are the daily indices of solar activity F10.7 or
SSN2 for the previous 45 days (d&lt;SUB&gt;45&lt;/SUB&gt;, , d&lt;SUB&gt;1&lt;/SUB&gt;), the
solar cycle phase (d) for the current day, and the daily indices of
solar activity for the subsequent 45 days (d&lt;SUB&gt;1&lt;/SUB&gt;, ,
d&lt;SUB&gt;45&lt;/SUB&gt;) in the corresponding phase  of the previous solar
cycle. The forecast of the sunspot number SSN2 for 45 days is made for
the first time with an accuracy from 5.1 units for low solar activity to
23.1 units for high solar activity. A comparison of the forecast of
F10.7 index of the MSA45 model with USAF-45DF forecast of this parameter
and observational data show an improvement in the forecast accuracy from
15% at the solar activity maximum to 50% at the minimum solar activity.</description>
</item>
<item>
<title> DLITEAn inexpensive, deployable interferometer for solar radio burst observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...926455C</link>
<description>Solar radio bursts (SRBs) are brief periods of enhanced radio emission
from the Sun. SRBs can provide unique insights into the plasma structure
where emission occurs. SRBs can also provide critical information
concerning space weather events such as coronal mass ejections or solar
energetic particle events. Providing continuous monitoring of SRBs
requires a full network of detectors continuously monitoring the Sun. A
promising new network is being developed, employing a four-element
interferometer called the Deployable Low-band Ionosphere and Transient
Experiment (DLITE) array. DLITE, which operates in a 3040 MHz band, was
specifically designed to probe the Earth's ionosphere using high
resolution measurements (1.024-s temporal resolution, 16.276-kHz
frequency resolution); however, this also makes DLITE a powerful new
tool for providing detailed observations of SRBs at these frequencies.
DLITE is particularly adept at detecting long-duration SRBs like Type II
and Type IV bursts. DLITE provides high resolution SRB data that can
complement ground-based networks like e-Callisto or space-based
observations, e.g., from Wind/WAVES. As an inexpensive interferometer,
DLITE has strong potential as an educational tool: DLITE can be used to
study the ionosphere, SRBs, and even Jovian radio bursts. Future DLITE
arrays could be enhanced by using the full 2080 MHz band accessible by
the antennas and employing its millisecond time-resolution capability;
this would improve DLITE's ability to track long-duration bursts, create
the opportunity to study short-duration Type III bursts in detail, and,
in particular, make the study of Type I bursts practical.</description>
</item>
<item>
<title> The Sun and Space Weather</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Atmos..13.1781G</link>
<description>The explosion of space weather research since the early 1990s has been
partly fueled by the unprecedented, uniform, and extended observations
of solar disturbances from space- and ground-based instruments. Coronal
mass ejections (CMEs) from closed magnetic field regions and high-speed
streams (HSS) from open-field regions on the Sun account for most of the
disturbances relevant to space weather. The main consequences of CMEs
and HSS are their ability to cause geomagnetic storms and accelerate
particles. Particles accelerated by CME-driven shocks can pose danger to
humans and their technological structures in space. Geomagnetic storms
produced by CMEs and HSS-related stream interaction regions also result
in particle energization inside the magnetosphere that can have severe
impact on satellites operating in the magnetosphere. Solar flares are
another aspect of solar magnetic energy release, mostly characterized by
the sudden enhancement in electromagnetic emission at various
wavelengthsfrom radio waves to gamma-rays. Flares are responsible for
the sudden ionospheric disturbances and prompt perturbation of Earth's
magnetic field known as magnetic crochet. Nonthermal electrons
accelerated during flares can emit intense microwave radiation that can
drown spacecraft and radar signals. This review article summarizes major
milestones in understanding the connection between solar variability and
space weather.</description>
</item>
<item>
<title> A Small Flare from Proxima Cen Observed in the Millimeter, Optical, and Soft X-Ray with Chandra and ALMA</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...938..103H</link>
<description>We present millimeter, optical, and soft X-ray observations of a stellar
flare with an energy squarely in the regime of typical X1 solar flares.
The flare was observed from Proxima Cen on 2019 May 6 as part of a
larger multi-wavelength flare monitoring campaign and was captured by
Chandra, the Las Cumbres Observatory Global Telescope, the Irn du Pont
Telescope at Las Campanas Observatory, and the Atacama Large Millimeter
Array. Millimeter emission appears to be a common occurrence in small
stellar flares that had gone undetected until recently, making it
difficult to interpret these events within the current multi-wavelength
picture of the flaring process. The May 6 event is the smallest stellar
millimeter flare detected to date. We compare the relationship between
the soft X-ray and millimeter emission to that observed in solar flares.
The X-ray and optical flare energies of 10&lt;SUP&gt;30.3  0.2&lt;/SUP&gt; and
10&lt;SUP&gt;28.9  0.1&lt;/SUP&gt; erg, respectively, the coronal temperature of T
= 11.0  2.1 MK, and the emission measure of 9.5  2.2  10&lt;SUP&gt;49&lt;/SUP&gt;
cm&lt;SUP&gt;-3&lt;/SUP&gt; are consistent with M-X class solar flares. We find the
soft X-ray and millimeter emission during quiescence are consistent with
the Gdel-Benz relation, but not during the flare. The millimeter
luminosity is &gt;100 higher than that of an equivalent X1 solar flare and
lasts only seconds instead of minutes as seen for solar flares.</description>
</item>
<item>
<title> Tracking a Beam of Electrons from the Low Solar Corona into Interplanetary Space with the Low Frequency Array, Parker Solar Probe, and 1 au Spacecraft</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...938...95B</link>
<description>Type III radio bursts are the result of plasma emission from mildly
relativistic electron beams propagating from the low solar corona into
the heliosphere where they can eventually be detected in situ if they
align with the location of a heliospheric spacecraft. Here we observe a
type III radio burst from 0.1 to 16 MHz using the Parker Solar Probe
(PSP) FIELDS Radio Frequency Spectrometer (RFS) and from 20 to 80 MHz
using the Low Frequency Array (LOFAR). This event was not associated
with any detectable flare activity but was part of an ongoing type III
and noise storm that occurred during PSP encounter 2. A deprojection of
the LOFAR radio sources into 3D space shows that the type III radio
burst sources were located on open magnetic field from 1.6 to 3 R
&lt;SUB&gt;&lt;/SUB&gt; and originated from a near-equatorial active region around
longitude E48. Combining PSP/RFS observations with WIND/WAVES and Solar
Terrestrial Relations Observatory (STEREO) WAVES, we reconstruct the
type III radio source trajectory in the heliosphere interior to PSP's
position, assuming ecliptic confinement. An energetic electron
enhancement is subsequently detected in situ at the STEREO A spacecraft
at compatible times, although the onset and duration suggests the
individual burst contributes a subset of the enhancement. This work
shows relatively small-scale flux emergence in the corona can cause the
injection of electron beams from the low corona into the heliosphere,
without needing a strong solar flare. The complementary nature of
combined ground and space-based radio observations, especially in the
era of PSP, is also clearly highlighted by this study.</description>
</item>
<item>
<title> Influence of Fine Structures on Gyrosynchrotron Emission of Flare Loops Modulated by Sausage Modes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...937L..25S</link>
<description>Sausage modes are a leading mechanism for interpreting short-period
quasi-periodic pulsations (QPPs) of solar flares. Forward modeling their
radio emission is crucial for identifying sausage modes observationally
and for understanding their connections with QPPs. Using the numerical
outputs from three-dimensional magnetohydrodynamic simulations, we
forward model the gyrosynchrotron emission of flare loops modulated by
sausage modes and examine the influence of fine structures of loops. The
temporal evolution of the emission intensity is analyzed for an oblique
line of sight crossing the loop center. We find that the low- and high-
frequency intensities oscillate in phase in the periods of sausage modes
for models with or without fine structures. For low-frequency emissions
where the optically thick regime arises, the modulation magnitude of the
intensity is dramatically reduced by the fine structures at some viewing
angles. On the contrary, for high-frequency emissions where the
optically thin regime holds, the effects of fine structures or the
viewing angle are marginal. Our results show that the periodic intensity
variations of sausage modes are not wiped out by fine structures, and
that sausage modes remain a promising candidate mechanism for QPPs, even
when the flare loops are fine-structured.</description>
</item>
<item>
<title> First Detection of Transverse Vertical Oscillation during the Expansion of Coronal Loops</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...937L..21Z</link>
<description>In this Letter, we perform a detailed analysis of the M5.5 class
eruptive flare occurring in active region 12,929 on 2022 January 20. The
eruption of a hot channel generates a fast coronal mass ejection (CME)
and a dome-shaped extreme-ultraviolet (EUV) wave at speeds of 740-860 km
s&lt;SUP&gt;-1&lt;/SUP&gt;. The CME is associated with a type II radio burst,
implying that the EUV wave is a fast-mode shock wave. During the
impulsive phase, the flare shows quasi-periodic pulsations (QPPs) in
EUV, hard X-ray, and radio wavelengths. The periods of QPPs range from
18 to 113 s, indicating that flare energy is released and nonthermal
electrons are accelerated intermittently with multiple timescales. The
interaction between the EUV wave and low-lying adjacent coronal loops
(ACLs) results in contraction, expansion, and transverse vertical
oscillation of ACLs. The speed of contraction in 171, 193, and 211  is
higher than that in 304 . The periods of oscillation are 253 s and 275
s in 304  and 171 , respectively. A new scenario is proposed to
explain the interaction. The equation that interprets the contraction
and oscillation of the overlying coronal loops above a flare core can
also interpret the expansion and oscillation of ACLs, suggesting that
the two phenomena are the same in essence.</description>
</item>
<item>
<title> Long-term temperature and ozone response to natural drivers in the mesospheric region using 16 years (2005-2020) of TIMED/SABER observation data at 5-15N</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AdSpR..70.2095B</link>
<description>The long-term mesospheric (60-100 km) temperature and ozone volume
mixing ratio variability during the period of January 2005 to December
2020 were analyzed to obtain trends and their response to natural
influences using the SABER, an instrument onboard the TIMED satellite to
obtain observation data in the latitude range of 5N-15N. A wavelet
analysis technique has been used to identify the dominant periodic
oscillations in mesospheric temperature and ozone. Using the proxy data
of F10.7, Nino 3.4, and zonal wind index (QBO at 30 hPa), the
mesospheric response to natural drivers was investigated using a
multiple linear regression technique. Among the three natural drivers,
solar radio flux (F10.7) is the dominant contributor to mesospheric
variability rather than ENSO and QBO. It influences negatively the lower
mesosphere (60-80 km), and above 80 km, it responds positively in
temperature (2.6 K), whereas ozone responds with a constant negative
value (0.12ppmv) up to 80 km, and after it influences by a maximum
positive value of 0.7 ppmv. At 80 km, the temperature and ozone respond
in phase to all natural influences (F10.7, ENSO, and QBO), and are out
of phase below and above 80 km. Both the temperature and the ozone
reveal cooling trends (-0.85 K/decade and -0.12 ppmv/decade) of the the
lower mesosphere (60-80 km) and are followed by the upper mesospheric
(85-100 km) warming trends (1.25 K/decade and 0.27 ppmv/ decade) over
the low latitudes. In general, natural influences affected the
mesospheric temperature more strongly than the ozone volume mixing
ratio. Our results are expected to be an updated and reliable estimation
of the mesospheric temperature and ozone variability for the equatorial
mesosphere.</description>
</item>
<item>
<title> Stochastic approach to Markovian interrelationship assessment of solar activity indices</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;C....4100637I</link>
<description>This paper employs a discrete-time Markov chain (DTMC) stochastic
process to investigate a state/event based Markovian interrelationship
between various solar activity indices (SAI) (including 10.7 cm solar
radio flux (SF&lt;SUB&gt;10.7&lt;/SUB&gt;), coronal index (CI), solar flare index
(SFI) and total solar irradiance (TSI)) in relation to sunspot number
(SSN). First, we applied the first order DTMC model as a first
approximation to the total number of transitions between different
states of SAI in order to estimate the probability of occurrence
corresponding with each transition. Next, several DTMC descriptors like
persistency, state dependency, stationarity, mean first passage time and
entropy are derived from estimated transition probability matrices.
These descriptors are very useful as they related to time series
characteristics (like randomness, nature of cycles and predictability)
within a stochastic dynamical system as well as crucial for checking the
applicability of Markov chain method. Therefore, via the DTMC analysis
and derived descriptors, this study found remarkable similarities in the
formation of transition matrices and diagrams, significant 2-dimensional
correlation values, robust self-communication behaviour among states,
existence of dependent successive transitions and stationary nature of
data throughout the space. Further, the resemblance in the average
transit time from one state to another, probabilistically disordered
symmetrical time series and existence of randomness in transition states
has been observed. Therefore, results obtained in this paper provide a
new insight to increase the level of knowledge of the possible linkage
between underlying SAI that could be helpful in enhanced understanding
of the potential future climate changes and other solar energy-related
objectives.</description>
</item>
<item>
<title> Overexpansion-dominated coronal mass ejection formation and induced radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...666A.166W</link>
<description>&lt;BR /&gt; Aims: Coronal mass ejections (CMEs) are the most fascinating
explosions in the Solar System. Their formation is still not fully
understood, however. &lt;BR /&gt; Methods: We investigated a well-observed CME
on 2021 May 7 that showed a typical three-component structure and was
continuously observed from 0 to 3 R&lt;SUB&gt;&lt;/SUB&gt; by a combination of
SDO/AIA (0-1.3 R&lt;SUB&gt;&lt;/SUB&gt;), PROBA2/SWAP (0-1.7 R&lt;SUB&gt;&lt;/SUB&gt;), and
MLSO/K-Cor (1.05-3 R&lt;SUB&gt;&lt;/SUB&gt;). Furthermore, we compared the
morphological discrepancy between the CME white-light bright core and
the extreme-UV (EUV) blob. We finally explored the origin of various
radio bursts that are closely related to the interaction of the CME
overexpansion with a nearby streamer. &lt;BR /&gt; Results: An interesting
finding is that the height increases of the CME leading front and of the
bright core are dominated by the overexpansion during the CME formation.
The aspect ratios of the CME bubble and bright core, quantifying the
overexpansion, are found to decrease as the SO/STIX 4-10 keV and GOES
1-8  soft X-ray flux of the associated flare increases near the peaks.
This indicates that the flare reconnection plays an important role in
the first overexpansion. The CME bubble even undergoes a second
overexpansion, although it is relatively weak, which is closely related
to the compression with a nearby streamer and likely arises from an
ideal magnetohydrodynamics process. Moreover, the CME EUV blob is found
to be relatively lower and wider than the CME white-light bright core,
which may correspond to the bottom part of the growing CME flux rope.
The interaction between the CME and the streamer leads to two type II
radio bursts, one that is drifting normally and another that is
stationary, which are speculated to be induced by two different sources
of the CME-driven shock front. The bidirectional electrons shown in
series of C-shaped type III bursts suggest that the interchange
reconnection is also involved during the interaction of the CME and
streamer. &lt;P /&gt;Movies associated to Figs. 1 and 2 are available at &lt;A hr
ef="https://www.aanda.org/10.1051/0004-6361/202244275/olm"&gt;https://www.a
anda.org&lt;/A&gt;</description>
</item>
<item>
<title> A Mini-Review</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ITPS...50.2558O</link>
<description>Plasma spectroscopy, employing the shapes of spectral lines of atoms and
ions, historically started from astrophysical plasmas (thus, it was the
crossing of the macro- and micro-worlds)-before finding broad
applications to all kinds of laboratory plasmas intended for various
important practical purposes. The present mini-review covers advances in
understanding a variety of selected astrophysical plasmas achieved by
the analysis of their emission or absorption in the visible, microwave,
and radio ranges. It discusses the observational data and also touches
upon the relevant advances in the theory of line shapes. The
presentation is organized in order of the decreasing electron density
$N_{e}$ of the astrophysical objects: from white dwarfs ($N_{e} ~\sim
~10^{17}$ cm$^{-3}$ ) to flare stars ($N_{e} ~\sim ~10^{15}$ cm$^{-3}$
), solar flares ($N_{e} ~\sim ~10^{13}$ cm$^{-3}$ ), the quiet Sun
($N_{e} ~ \sim ~10^{11}$ cm$^{-3}$ ), the H II regions ($N_{e} ~\sim
~10^{4}$ cm$^{-3}$ ), and the recombination epoch of the early universe
($N_{e} ~\sim ~10^{4}$ cm$^{-3}$ ).</description>
</item>
<item>
<title> The Influence of Solar Activity on Snow Cover over the Qinghai-Tibet Plateau and Its Mechanism Analysis</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Atmos..13.1499S</link>
<description>Using global ocean vertical temperature anomaly data, we identified that
a significant response of the sea temperature anomaly (STA) to the solar
radio flux (SRF) exists. We found that the STA exhibited a significant
correlation with Asian summer and winter precipitation, among which the
response from the Qinghai-Tibet Plateau (the QTP) was particularly
noticeable. Based on NCEP/NCAR reanalysis data, the latent heat flux
(LHF) anomaly, which plays a key role in winter precipitation in China,
especially over the QTP, showed a significant response to the SRF in the
Pacific. The results demonstrated the bottom-up mechanism of impact of
solar activity (SA) on the plateau snow through sea-air interaction.
Meanwhile, a top-down mechanism was also present. When the SRF was high,
the stratospheric temperature in the low and mid-latitudes increased and
the temperature gradient pointed to the pole to strengthen the westerly
wind in the mid-latitudes. The EP flux showed that atmospheric long
waves in the high altitudes propagated downward from the stratosphere to
the troposphere. A westerly (easterly) wind anomaly occurred in the
south (north) of the QTP at 500 hPa and the snowfall rate over the QTP
tended to increase. When the SRF was low, the situation was the
opposite, and the snowfall rate tended to decrease. The model results
confirmed that when total solar irradiance (TSI) became stronger
(weaker), both of the solar radiation fluxes at the top of the
atmosphere and the surface temperature over the QTP increased
(decreased), the vertical updraft intensified (weakened), and the
snowfall rate tended to increase (decrease) accordingly. These
conclusions are helpful to deepen the understanding of SA's influence on
the snow cover over the QTP.</description>
</item>
<item>
<title> Searching for Quasi-periodic Oscillations in Astrophysical Transients Using Gaussian Processes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...936...17H</link>
<description>Analyses of quasi-periodic oscillations (QPOs) are important to
understanding the dynamic behavior in many astrophysical objects during
transient events like gamma-ray bursts, solar flares, magnetar flares,
and fast radio bursts. Astrophysicists often search for QPOs with
frequency-domain methods such as (Lomb-Scargle) periodograms, which
generally assume power-law models plus some excess around the QPO
frequency. Time-series data can alternatively be investigated directly
in the time domain using Gaussian process (GP) regression. While GP
regression is computationally expensive in the general case, the
properties of astrophysical data and models allow fast likelihood
strategies. Heteroscedasticity and nonstationarity in data have been
shown to cause bias in periodogram-based analyses. GPs can take account
of these properties. Using GPs, we model QPOs as a stochastic process on
top of a deterministic flare shape. Using Bayesian inference, we
demonstrate how to infer GP hyperparameters and assign them physical
meaning, such as the QPO frequency. We also perform model selection
between QPOs and alternative models such as red noise and show that this
can be used to reliably find QPOs. This method is easily applicable to a
variety of different astrophysical data sets. We demonstrate the use of
this method on a range of short transients: a gamma-ray burst, a
magnetar flare, a magnetar giant flare, and simulated solar flare data.</description>
</item>
<item>
<title> Comparative analysis of type III solar radio bursts associated with solar particle events and its impact on space weather for solar cycle 23 &amp; 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ap&amp;SS.367...91P</link>
<description>We have analyzed type III-l radio bursts associated with SEP events (&gt;10
MeV) during solar cycles 23 and 24 respectively. We have studied the
properties of type III radio bursts and SEP events. We have also
analyzed the correlation between the properties of type III-l bursts and
SEPs. We found that the mean duration of type III-l bursts and their
deviation for solar cycle 24 is higher. The log peak intensity of SEP
and its deviation is higher for solar cycle 23, which suggests that the
SEP events for solar cycle 23 are faster and long-duration events. From
the correlations, we conclude that the type III-l radio burst properties
for solar cycle 23 contribute more towards the SEP events as compared to
solar cycle 24.</description>
</item>
<item>
<title> Propagation of transverse waves in the solar chromosphere probed at different heights with ALMA sub-bands</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...665L...2G</link>
<description>The Atacama Large Millimeter/sub-millimeter Array (ALMA) has provided us
with an excellent diagnostic tool for studies of the dynamics of the
Solar chromosphere, albeit through a single receiver band at one time
presently. Each ALMA band consists of four sub-bands that are comprised
of several spectral channels. To date, however, the spectral domain has
been neglected in favour of ensuring optimal imaging, so that time-
series observations have been mostly limited to full-band data products,
thereby limiting studies to a single chromospheric layer. Here, we
report the first observations of a dynamical event (i.e., wave
propagation) for which the ALMA Band 3 data (centred at 3 mm; 100 GHz)
is split into a lower and an upper sideband. In principle, this approach
is aimed at mapping slightly different layers in the Solar atmosphere.
The side-band data were reduced together with the Solar ALMA Pipeline
(SoAP), resulting in time series of brightness-temperature maps for each
side-band. Through a phase analysis of a magnetically quiet region,
where purely acoustic waves are expected to dominate, the average height
difference between the two side-bands is estimated as 73  16 km.
Furthermore, we examined the propagation of transverse waves in small-
scale bright structures by means of wavelet phase analysis between
oscillations at the two atmospheric heights. We find 6% of the waves to
be standing, while 54% and 46% of the remaining waves are propagating
upwards and downwards, respectively, with absolute propagating speeds on
the order of 96 km s&lt;SUP&gt;1&lt;/SUP&gt;, resulting in a mean energy flux of
3800 W m&lt;SUP&gt;2&lt;/SUP&gt;.</description>
</item>
<item>
<title> Diagnostics of the dynamics of the Langmuir spectrum based on radio emission during the 12 March 2015 solar radio burst</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...665A..98K</link>
<description>&lt;BR /&gt; Aims: We investigate the dynamics of spectra of Langmuir waves in
the plasma radiation of solar radio bursts. &lt;BR /&gt; Methods: We simulated
the radio emission that is formed during the merging of Langmuir waves.
The observed frequency spectra of radio bursts were fitted by the model
spectrum of Langmuir waves. &lt;BR /&gt; Results: We determined shapes of the
Langmuir wave spectra, consistent with the solar burst observed in the
0.8-2.0 GHz range on 12 March 2015 by the Ondejov radiospectrograph. We
estimated the sizes of the corresponding radio source for different
values of the energy density of Langmuir waves. We present the time
evolution of the model Langmuir wave spectra at four instants. Finally,
we explain a role of the induced scattering of Langmuir waves in the
formation of their spectra.</description>
</item>
<item>
<title> Zebra Stripes with High Gyro-Harmonic Numbers</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297..103B</link>
<description>Solar radio zebras are used in the determination of the plasma density
and magnetic field in solar flare plasmas. Analyzing observed zebra
stripes and assuming their generation by the double-plasma resonance
(DPR) instability, high values of the gyro-harmonic number are found. In
some cases they exceed one hundred, in disagreement with the DPR growth
rates computed up to now, which decrease with increasing gyro-harmonic
number. We address the question of how zebras with high values of the
gyro-harmonic numbers s are generated. For this purpose, we compute the
growth rates of the DPR instability in a very broad range of s ,
considering a loss-cone  -distribution of superthermal electrons and
varying the loss-cone angle, electron energies, and background plasma
temperature. We have numerically calculated the dispersion relations and
the growth rates of the upper-hybrid waves and found that the growth
rates increase with increasing gyro-harmonic numbers if the loss-cone
angles are 80&lt;SUP&gt;&lt;/SUP&gt;. The highest growth rates for these loss-cone
angles are obtained for velocity v&lt;SUB&gt;&lt;/SUB&gt;=0.15 c . The growth rates
as a function of the gyro-harmonic number still show well distinct
peaks, which correspond to zebra-stripe frequencies. The contrast
between peak growth rates and surrounding growth rate levels increases
as the  index increases and the background temperature decreases.
Zebras with high values of s can be generated in regions where loss-cone
distributions of superthermal electrons with large loss-cone angles
(80&lt;SUP&gt;&lt;/SUP&gt;) are present. Furthermore, owing to the high values of
s , the magnetic field is relatively weak and has a small spatial
gradient in such regions.</description>
</item>
<item>
<title> Analysis of the Radio Solar Telescope Network's Noon Flux Observations Over Three Solar Cycles (1988-2020)</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RaSc...5707456G</link>
<description>The Sun is a readily accessible source of wideband noise that can be
used for the calibration of a wide variety of radio systems. Since 1979
the United States Air Force Radio Solar Telescope Network (RSTN) has
performed solar flux observations around noon on eight frequencies
between 245 and 15,400 MHz. These fluxes are disseminated by the
National Ocean and Atmospheric Administration (NOAA) and are used by
many radio and radar system operators to perform system calibration.
Little analysis has been performed on the RSTN noon flux values. Here we
review the calibration procedures of RSTN and perform statistical tests
between the four sites comprising RSTN. For system operators who require
precise system calibration the noted variations may be large enough to
cast doubt on RSTN flux values for such calibration. However, for many
communication systems a calibration within one or two dB is adequate. We
discuss the reported variation both in linear and logarithmic terms.
When it is possible to used smoothed data the inter-site variation
becomes less of a problem, although the correlation between sites at Ku
band (15,400 MHz) still appears excessively large. We update some simple
empirical models for wideband solar flux based purely on the 10 cm flux
at any time, as these have also been used in solar radio calibration
procedures. We give practical advice on the use of solar flux for radio
system calibration and make some recommendations that we believe could
improve the accuracy and utility of solar radio flux reports.</description>
</item>
<item>
<title> A 3 Giga Sample Per Second 14-bit Digital Receiver with 9 GHz Input Bandwidth for Solar Radio Observation</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RAA....22h5012Z</link>
<description>A new digital receiver with excellent performances has been designed and
developed for solar radio observation, which can receive the radio
signal from direct current (DC) to 9 GHz in the direct acquisition way.
On the digital receiver, the analog-to-digital converter (ADC) with
14-bit, two input channels and 3 Giga Samples per second (Gsps) are used
to acquire observed signal, and the field-programmable-gate-array chip
XCKU115 acts as the processing module. The new digital receiver can be
used to directly sample the solar radio signals of frequency under 9
GHz. When receiving the solar radio signal above 9 GHz, the new digital
receiver can save 1-2 stages of frequency down-conversion, and
effectively improve many indexes of the solar radio observation system,
i.e., the time resolution, analog front-end circuit, weight and volume
of the analog circuit system. Compared with the digital receiver with
sampling rate below 1 Gsps used in existing solar radio telescope, the
new digital receiver reduces the frequency switching times of large
bandwidth, which is beneficial to improving the frequency and time
resolutions. The ADC sampling resolution of 14 bits, providing a large
dynamic range, is very beneficial to observing smaller solar eruptions.
This receiver, which would be used in the solar radio observation
system, well meets the latest requirements with the resolutions of time
(1 ms) and frequency (0.5 MHz) for fine observation of radio signals.</description>
</item>
<item>
<title> Diagnostics of energy release in solar flares with radio dynamic imaging spectroscopy</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PhDT........18L</link>
<description>Not Available</description>
</item>
<item>
<title> Design of a high-resolution antenna array solar observing system for radio frequencies of 25-110 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PASA...39...30W</link>
<description>Spectral observations with high temporal and frequency resolution are of
great significance for studying the fine structures of solar radio
bursts. In addition, it is helpful to understand the physical processes
of solar eruptions. In this paper, we present the design of a system to
observe solar radio bursts with high temporal and frequency resolutions
at frequencies of 25-110 MHz. To reduce the impact of analog devices and
improve the system flexibility, we employ various digital signal
processing methods to achieve the function of analog devices, such as
polarisation synthesis and beamforming. The resourceful field
programmable gate array is used to process radio signals. The system has
a frequency resolution of $$ 30 kHz and a temporal resolution of up to
0.2 ms. The left/right circular polarisation signals can be
simultaneously observed. At present, the system has been installed at
Chashan Solar Observatory operated by the Institute of Space Science,
Shandong University. The system is running well, multiple bursts have
been observed, and relevant data have been obtained.</description>
</item>
<item>
<title> Characteristics of stripes-pattern radio-emission sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.514.2135A</link>
<description>An investigation of the generation mechanism for stripes-pattern radio
spectra is important for an understanding of the dynamics of non-thermal
electrons in several astronomical objects, including the Sun, Jupiter,
and the Crab Pulsar. A new analytical study is carried out to identify
the plasma characteristics of fiber- and zebra-pattern emission sources
without an underlying density or magnetic model. The analysis
demonstrates that the source region of the stripes emission is located
underneath the reconnection point, where the ratio s of the instability
growth rate to the electron gyrofrequency &lt;SUB&gt;c&lt;/SUB&gt; does not equal
unity; that is, s = k&lt;SUB&gt;&lt;/SUB&gt;v&lt;SUB&gt;&lt;/SUB&gt;/&lt;SUB&gt;c&lt;/SUB&gt;  1. When
|s| &lt; 1, the plasma condition of the source region becomes
k&lt;SUB&gt;&lt;/SUB&gt;v&lt;SUB&gt;&lt;/SUB&gt; &lt; &lt;SUB&gt;p&lt;/SUB&gt; &lt; &lt;SUB&gt;c&lt;/SUB&gt;, where
&lt;SUB&gt;p&lt;/SUB&gt; is the plasma frequency, and the emission source is likely
to produce a fiber radio burst. For |s| &gt; 1, the plasma condition of the
source region is &lt;SUB&gt;c&lt;/SUB&gt; &lt; &lt;SUB&gt;p&lt;/SUB&gt; &lt;
k&lt;SUB&gt;&lt;/SUB&gt;v&lt;SUB&gt;&lt;/SUB&gt;, and the emission source is likely to produce
zebra-pattern emission. This indicates that the magnetic field in the
source region of zebra-pattern radio emission is weak and it is
relatively high in the source region of fiber-pattern emission. An
approach is applied to estimate the plasma parameters of a zebra-pattern
emission source observed on 2011 June 21. The behaviour of the blasted
medium, which is produced by magnetic reconnection, is investigated. The
results show that the blasted medium propagates isothermally as a
sausage-like wave for a short time during the emission. The study
discusses the conditions for producing different types of striped radio
emission and provides a simple computational approach that could be
useful in a number of astronomical contexts.</description>
</item>
<item>
<title> Self-powered wearable sensors design considerations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022JMiMi..32h3002H</link>
<description>Wearable sensors have been implemented widely to provide comfortable and
continuous long-term monitoring in many applications. Minimal
requirements on maintenance is a main characteristic of wearable
sensors, but unfortunately, many of them are still powered by battery
with limited capacity which need to be charged or replaced regularly.
Energy harvesting technologies are applied to provide a reliable
solution to this issue. This paper presents several design
considerations for self-powered wearable sensors. Suitable energy
sources are discussed, such as ambient energy sources (solar, radio
frequency, and ultrasonic energy), human body energy (mechanical,
piezoelectric, triboelectric, electromagnetic, electrostatic, and
thermal energy). Moreover, power management integrated circuits, energy
storage options, and the material selection and conditioning circuit of
triboelectric nanogenerator are discussed. Five case studies utilizing
different energy harvesting techniques are discussed and evaluated in
terms of their system implementation and performance to provide some
deeper understandings of wearable sensors.</description>
</item>
<item>
<title> The Relationship of the IG and T Ionospheric Indices to the Solar and Geomagnetic Activity Indices</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62..382D</link>
<description>An analysis of the relationship between the monthly mean ionospheric
indices IG and T and the indices of solar (F107) and geomagnetic (Ap)
activity based on the massif of these data within 19542020 interval is
presented. F107 and Ap are the monthly mean flux of the solar radio
emission at a wavelength of 10.7 cm and the planetary index of
geomagnetic activity Ap, respectively. It is found that the index F =
(F107&lt;SUB&gt;0&lt;/SUB&gt; + F107&lt;SUB&gt;1&lt;/SUB&gt;)/2 provides a higher correlation
to the ionospheric indices than the indices F107 over the given
(F107&lt;SUB&gt;0&lt;/SUB&gt;) or previous (F107&lt;SUB&gt;1&lt;/SUB&gt;) months. The IG and T
dependencies on F in the form of a second-degree polynomials make it
possible to reproduce 96% of variations in IG and 98% of variations in T
for the analyzed time interval. That is the reason that the additional
contribution of Ap into IG and T is weak. Nevertheless, the contribution
of Ap into T and IG depends on the time of the year: it is not
significant for January and is significant for July. This property of
the annual anomaly in the ionospheric parameters by the IG index,
apparently, is discovered for the first time. In all considered cases,
an increase in Ap leads to a decrease in T and IG, that is, to a mean
(global) decrease in the median of the F2-layer maximum concentration
and, under equal other conditions, such a decrease is more significant
in July than in January. The properties of the dependencies of the IG
and T indices on F and Ap are in many aspects similar, but the accuracy
of these dependencies is higher for T than for IG.</description>
</item>
<item>
<title> A Publicly Available Multiobservatory Data Set of an Enhanced Network Patch from the Photosphere to the Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJS..261...15K</link>
<description>New instruments sensitive to chromospheric radiation at X-ray, UV,
visible, IR, and submillimeter wavelengths have become available that
significantly enhance our ability to understand the bidirectional flow
of energy through the chromosphere. We describe the calibration,
coalignment, initial results, and public release of a new data set
combining a large number of these instruments to obtain multiwavelength
photospheric, chromospheric, and coronal observations capable of
improving our understanding of the connectivity between the photosphere
and the corona via transient brightenings and wave signatures. The
observations center on a bipolar region of enhanced-network magnetic
flux near disk center on SOL2017-03-17T14:00-17:00. The comprehensive
data set provides one of the most complete views to date of
chromospheric activity related to small-scale brightenings in the corona
and chromosphere. Our initial analysis shows a strong spatial
correspondence between the areas of broadest width of the hydrogen-
spectral line and the hottest temperatures observed in Atacama Large
Millimeter/submillimeter Array (ALMA) Band 3 radio data, with a linear
coefficient of 6.12  10&lt;SUP&gt;-5&lt;/SUP&gt;/K. The correspondence persists
for the duration of cotemporal observations (60 m). Numerous transient
brightenings were observed in multiple data series. We highlight a
single, well-observed transient brightening in a set of thin filamentary
features with a duration of 20 minutes. The timing of the peak intensity
transitions from the cooler (ALMA, 7000 K) to the hotter (XRT, 3 MK)
data series.</description>
</item>
<item>
<title> Third and Fourth Harmonics of Electromagnetic Emissions by a Weak Beam in a Solar Wind Plasma with Random Density Fluctuations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...934L..28K</link>
<description>Electromagnetic emissions ${{ \mathcal H }}_{3}$ and ${{ \mathcal H
}}_{4}$ at the third and fourth harmonics of the plasma frequency 
&lt;SUB&gt; p &lt;/SUB&gt; were observed during the occurrence of type II and type
III solar radio bursts. Two-dimensional particle-in-cell simulations are
performed using a weak beam, high space and time resolutions, and a
plasma with density fluctuations of a few percent, for parameters
relevant to regions of type III bursts. For the first time, a detailed
study of the different wave coalescence processes involved in the
generation of ${{ \mathcal H }}_{3}$ and ${{ \mathcal H }}_{4}$ waves is
presented and the impact of density fluctuations on the wave interaction
mechanisms is demonstrated. Energy ratios between the second, third, and
fourth harmonics ${{ \mathcal H }}_{2}$ , ${{ \mathcal H }}_{3}$ , and
${{ \mathcal H }}_{4}$ are consistent with space observations. It is
shown that, in both homogeneous and inhomogeneous plasmas, the dominant
processes generating ${{ \mathcal H }}_{3}$ ( ${{ \mathcal H }}_{4}$ )
are the coalescence of ${{ \mathcal H }}_{2}$ ( ${{ \mathcal H }}_{3}$ )
with a Langmuir wave, in spite of the random density fluctuations
modifying the waves' resonance conditions by energy transport in the
wavevector space and of the damping of Langmuir waves. The role of the
backscattered (forward-propagating) Langmuir waves coming from the first
(second) cascade of the electrostatic decay of beam-driven Langmuir
waves is determinant in these processes. Understanding such wave
coalescence mechanisms can provide indirect information on Langmuir and
ion acoustic wave turbulence, the average level of density
inhomogeneities, and suprathermal electron fluxes generated in solar
wind regions where the harmonics manifest. Causes for the rarity of
their observations are discussed.</description>
</item>
<item>
<title> A Comparative Statistical Study on Their Characteristics and Geoeffectiveness</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...97H</link>
<description>Interplanetary sheaths and corotating interaction regions (CIRs), while
having different solar sources, represent turbulent solar-wind plasma
and magnetic field that can perturb the Earth's magnetosphere. We
explore long-term solar-wind measurements upstream of the Earth during
Solar Cycle 24, from January 2008 to December 2019, to compare their
solar-cycle variation, characteristic features, and geoeffectiveness.
Earth is found to be encountered by  2.6 times more CIRs (290) than
sheaths (110) during this period. The sheath occurrence follows the
F&lt;SUB&gt;10.7&lt;/SUB&gt; solar radio-flux variation, with a cross-correlation
coefficient (r&lt;SUB&gt;cc&lt;/SUB&gt;) of +0.71 at zero-year time lag. However,
the CIR occurrence is more prominent during the solar cycle descending
to minimum phases, reflected in r&lt;SUB&gt;cc&lt;/SUB&gt; values of 0.53 and +0.50
at time lags of 2 and +4 years, respectively, between the CIR
occurrence and the F&lt;SUB&gt;10.7&lt;/SUB&gt; solar flux. Both sheath and CIR are
characterized by identical average plasma density and interplanetary
magnetic-field (IMF) magnitude, and their fluctuations characterized by
enhanced variance, and periodic variations of a few minutes to an hour.
However, on average, the CIR has  12% higher plasma speed,  33% higher
temperature,  20% stronger southward IMF component,  131% longer
duration, and  158% longer radial extent than the sheath. The
intensities of the auroral electrojet index [AE] and the symmetric ring-
current index [SYM-H] are, respectively,  38% and  55% stronger during
the CIR than the sheath, on average. The geoeffectiveness of the CIR is
found to be significantly higher than the sheath. Among all CIRs
(sheaths),  25% ( 14%) caused moderate storms (50 nT  SYM-H &gt;100
nT), and  5% ( 4%) caused intense storms (SYM-H 100 nT).</description>
</item>
<item>
<title> Continuum Imaging in the 18 - 26 GHz Range</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...86P</link>
<description>We present a new solar radio imaging system implemented through the
upgrade of the large single-dish telescopes of the Italian National
Institute for Astrophysics (INAF), not originally conceived for solar
observations.</description>
</item>
<item>
<title> Study of Fine Radio-Burst Structures (FRBS) Observed by the Mexican Array Radio Telescope (MEXART)</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...84C</link>
<description>Solar events occur in several energy ranges and durations, with
emissions involving a wide range of the electromagnetic spectrum. The
present work reveals the instrumental capacity of the Mexican Array
Radio Telescope (MEXART) to detect solar radio emissions in the VHF
band. Particular attention is focused on intense, short-duration solar
transient emissions in the form of fine radio-burst structures (FRBS),
observed by MEXART at around 140 MHz. A Type-I noise storm event with
metric FRBS corresponding to observations on 6 May 2019 is reported. The
FRBS exhibited distinct durations within the range of 0.47 - 8.07 s, a
mean value of 2.48 s, and intensities between  1.0 - 8.0 sfu, with the
initial FRBS having a longer duration and greater peak intensity levels
than the subsequent radio bursts. The time profile of the FRBS has an
asymmetric structure consisting of an abrupt rise, a short-term maximum
peak, and a slow decay phase with mean values of 1.90 and 2.50 s for the
rise and decay times, respectively. Compared with other fast radio
transients observed at higher frequencies, the longer duration of the
FRBS suggests lack of interaction of an electron beam with its
surrounding parcelled low-density plasma environment. The properties of
the FRBS structures are discussed.</description>
</item>
<item>
<title> Diagnostic Functions of Solar Coronal Magnetic Fields from Radio Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RAA....22g2001T</link>
<description>In solar physics, it is a big challenge to measure the magnetic fields
directly from observations in the upper solar atmosphere, including the
chromosphere and corona. Radio observations are regarded as the most
feasible approach to diagnose the magnetic field in solar chromosphere
and corona. However, because of the complexity and diversity of the
emission mechanisms, the previous studies have only presented the
implicit diagnostic functions of the magnetic field for specific
mechanism from solar radio observations. This work collected and sorted
out all methods for diagnosing coronal magnetic field from solar radio
observations, which are expressed as a set of explicit diagnostic
functions. In particular, this work supplemented some important
diagnostic methods missed in other reviews. This set of diagnostic
functions can completely cover all regions of the solar chromosphere and
corona, including the quiet region, active region and flaring source
regions. At the same time, it also includes incoherent radiation such as
bremsstrahlung emission of thermal plasma above the quiet region,
cyclotron and gyro-synchrotron emissions of magnetized hot plasma and
mildly relativistic nonthermal electrons above the active regions, as
well as coherently plasma emission around flaring source regions. Using
this set of diagnostic functions and the related broadband spectral
solar radio imaging observations, we can derive the magnetic fields of
almost all regions in the solar atmosphere, which may help us to make
full use of the spectral imaging observations of the new generation
solar radio telescopes (such as MUSER, EVOSA and the future FASR, etc.)
to study the solar activities, and provide a reliable basis for the
prediction of disastrous space weather events.</description>
</item>
<item>
<title> Wave Emission of Nonthermal Electron Beams Generated by Magnetic Reconnection</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...933..219Y</link>
<description>Magnetic reconnection in solar flares can efficiently generate
nonthermal electron beams. The energetic electrons can, in turn, cause
radio waves through microscopic plasma instabilities as they propagate
through the ambient plasma along the magnetic field lines. We aim at
investigating the wave emission caused by fast-moving electron beams
with characteristic nonthermal electron velocity distribution functions
(EVDFs) generated by kinetic magnetic reconnection: two-stream EVDFs
along the separatrices and in the diffusion region, and perpendicular
crescent-shaped EVDFs closer to the diffusion region. For this purpose,
we utilized 2.5D fully kinetic Particle-In-Cell code simulations in this
study. We found the following: (1) the two-stream EVDFs plus the
background ions are unstable to electron/ion (streaming) instabilities,
which cause ion-acoustic waves and Langmuir waves due to the net
current. This can lead to multiple-harmonic plasma emission in the
diffusion region and the separatrices of reconnection. (2) The
perpendicular crescent-shaped EVDFs can cause multiple-harmonic
electromagnetic electron cyclotron waves through the electron cyclotron
maser instabilities in the diffusion region of reconnection. Our results
are applicable to diagnose the plasma parameters, which are associated
to magnetic reconnection in solar flares by means of radio wave
observations.</description>
</item>
<item>
<title> Study of Time Evolution of Thermal and Nonthermal Emission from an M-class Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...933..173N</link>
<description>We conduct a wide-band X-ray spectral analysis in the energy range of
1.5-100 keV to study the time evolution of the M7.6-class flare of 2016
July 23, with the Miniature X-ray Solar Spectrometer (MinXSS) CubeSat
and the Reuven Ramaty High Energy Solar Spectroscopic Imager (RHESSI)
spacecraft. With the combination of MinXSS for soft X-rays and RHESSI
for hard X-rays, a nonthermal component and three-temperature
multithermal component-"cool" (T  3 MK), "hot" (T  15 MK), and
"superhot" (T  30 MK)-were measured simultaneously. In addition, we
successfully obtained the spectral evolution of the multithermal and
nonthermal components with a 10 s cadence, which corresponds to the
Alfvn timescale in the solar corona. We find that the emission measures
of the cool and hot thermal components are drastically increasing more
than hundreds of times and the superhot thermal component is gradually
appearing after the peak of the nonthermal emission. We also study the
microwave spectra obtained by the Nobeyama Radio Polarimeters, and we
find that there is continuous gyrosynchrotron emission from mildly
relativistic nonthermal electrons. In addition, we conducted a
differential emission measure (DEM) analysis by using Atmospheric
Imaging Assembly on board the Solar Dynamics Observatory and determined
that the DEM of cool plasma increases within the flaring loop. We find
that the cool and hot plasma components are associated with
chromospheric evaporation. The superhot plasma component could be
explained by the thermalization of the nonthermal electrons trapped in
the flaring loop.</description>
</item>
<item>
<title> A case study of the M&lt;SUB&gt;w&lt;/SUB&gt; 7.8 Nepal earthquake</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AdSpR..70..440S</link>
<description>We propose a Multi-Network-based Hybrid Long Short Term Memory (N-LSTM)
model for ionospheric anomaly detection to forecast highly irregular
data of the ionospheric Total Electron Content (TEC). Previously
purposed models were suffering from the problems of vanishing gradient,
exploding gradient, uncertainty, and parameter bias. LSTM is used to
overcome the vanishing and exploding gradient problems and the remaining
two (uncertainty and parameter bias) are subjugated by N-LSTM. We have
also discussed the implementation of the model by using the Mw 7.8 Nepal
Earthquake (EQ) that occurred on April 25, 2015. The proposed model
detects a significant negative anomaly about 14 days before the
impending EQ. Furthermore, we find gradual increments in the TEC time-
series, where the TEC values gradually increased, in terms of positive
anomalies, for four continuous days (April 21-24, 2015) till the
mainshock. Further analysis revealed that the nighttime TEC enhancements
are more dominant than the daytimes, which persisted for 10 h
(22:00-08:00 LT) in the absence of the solar flux, we named them the
absolute seismic precursors. These gradual enhancements establish a
perfect correlation with several atmospheric anomalies, reported in the
previous studies, where the variations in different atmospheric
parameters like Outgoing Longwave Radiation (OLR), air temperature,
Ozone, and sub-ionospheric Very-Low Frequency (VLF), were reported for 4
consistent days till the EQ day. The N-LSTM result was compatible with a
30-day running median, which is the classical method of ionospheric
anomaly detection. We also examined the planetary K-index (Kp),
disturbance storm-time (Dst), solar radio flux (F10.7), and solar wind
speed (V&lt;SUB&gt;SW&lt;/SUB&gt;) indices to check the possible attribution of
space weather on the ionosphere during the analysis. The results showed
that the anomalies of the ionospheric TEC were more dominantly caused by
the EQ phenomenon than the space weather during the nighttime hours.
Also, N-LSTM provided sufficient short-term prediction performance of
the ionospheric TEC and anomaly detection.</description>
</item>
<item>
<title> Evidence of particle acceleration within and escape from the solar corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...663A.173K</link>
<description>&lt;BR /&gt; Aims: We analyse particle, radio, and X-ray observations during
the first relativistic proton event of solar cycle 25 detected on Earth.
The aim is to gain insight into the relationship between relativistic
solar particles detected in space and the processes of acceleration and
propagation in solar eruptive events. &lt;BR /&gt; Methods: To this end, we
used ground-based neutron monitor measurements of relativistic nucleons
and space-borne measurements of electrons with similar speed to
determine the arrival times of the first particles at 1 AU and to infer
their solar release times. We compared the release times with the time
histories of non-thermal electrons in the solar atmosphere and their
escape to interplanetary space, as traced by radio spectra and X-ray
light curves and images. &lt;BR /&gt; Results: Non-thermal electrons in the
corona are found to be accelerated in different regions. Some are
confined in closed magnetic structures expanding during the course of
the event. Three episodes of electron escape to the interplanetary space
are revealed by groups of decametric-to-kilometric type III bursts. The
first group appears on the low-frequency side of a type II burst
produced by a coronal shock wave. The two latter groups are accompanied
at higher frequencies by bursts with rapid drifts to both lower and
higher frequencies (forward- or reverse-drifting bursts). They are
produced by electron beams that propagate both sunward and anti-sunward.
The first relativistic electrons and nucleons observed near Earth are
released with the third group of type III bursts, more than ten minutes
after the first signatures of non-thermal electrons and of the formation
of the shock wave in the corona. Although the eruptive active region is
near the central meridian, several tens of degrees east of the footpoint
of the nominal Parker spiral to the Earth, the kilometric spectrum of
the type III bursts and the in situ detection of Langmuir waves
demonstrate a direct magnetic connection between the L1 Lagrange point
and the field lines onto which the electron beams are released at the
Sun. &lt;BR /&gt; Conclusions: We interpret the forward- and reverse-drifting
radio bursts as evidence of reconnection between the closed expanding
magnetic structures of an erupting flux rope and ambient open magnetic
field lines. We discuss the origin of relativistic particles near the
Earth across two scenarios: (1) acceleration at the CME-driven shock as
it intercepts interplanetary magnetic field lines rooted in the western
solar hemisphere and (2) an alternative where the relativistic particles
are initially confined in the erupting magnetic fields and get access to
the open field lines to the Earth through these reconnection events. &lt;P
/&gt;Movie is available at &lt;A href="https://www.aanda.org/10.1051/0004-6361
/202243903/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> Double peak quasi-periodic pulsations in a circular-ribbon flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...663A.149A</link>
<description>We study quasi-periodic pulsations (QPPs) during the impulsive phase of
the C8.3 flare SOL2002-08-06T01:43. The shape of an extended 5.7 GHz
source is similar to a tadpole with the head located above the region of
a negative magnetic polarity, surrounded by positive polarity patches
and with a remote tail source. The flare configuration includes bright
extreme ultraviolet (EUV) ropes with footpoints near the boundary of the
negative magnetic field region and it can be identified as a circular
ribbon flare. We use simultaneous observations carried out by the
Siberian Solar Radio Telescope at 5.7 GHz, the Nobeyama Radio Heliograph
(NoRH) at 17 and 34 GHz, the Reuven Ramaty High Energy Solar
Spectroscopic Imager (RHESSI)/HXR, and the Transition Region and Coronal
Explorer (TRACE) imaging in the extreme ultraviolet. The flare HXR
emission is produced by a compact source located at the south periphery
of the Negative Magnetic field Region (NMR). The QPPs are observed
during a one-minute interval after the start of the impulsive phase,
when this HXR source appeared. The remote source is detected on the
variation maps of the of the brightness temperature at 17 GHz and is
located at the end of tadpole tail about 60 arcsec eastward. More than a
dozen cotemporal HXR and microwave pulses with timescales from 1.5 s up
to about 8 s were observed in the flare kernel. At 5.7 GHz, the pulses
are more prominent near the remote source where they are highly
polarized and generated by the electron beams propagating from the flare
kernel. The main tone of the QPP periodicity corresponds to the
oscillations with a period of 8 s and is accompanied by the variations
in the hardness of nonthermal electrons, that is, in the efficiency of
the acceleration mechanism. The second intensity harmonic (about a 3-s
period) appears due to a double peak structure of the QPP event. Such
pulse shapes suggest oscillations of the current sheet during the loop
coalescence as a modulation mechanism of the flare energy release.</description>
</item>
<item>
<title> Clusters of Solar Radio Spikes Modulated by Quasi-Periodic Pulsations in a Confined Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....8..348H</link>
<description>Spikes are typical radio bursts in solar flares, which are proposed to
be the signal of energy release in the solar corona. The whole group of
spikes always shows different spectral patterns in the dynamic spectrum.
Here, we present a special new feature at 0.62 GHz in a confined flare.
Each group of spikes is composed of many quasi-periodic sub-clusters,
which are superposed on the broadband quasi-periodic pulsations (QPPs).
The quasi-periodic cluster of spikes (QPSs) have very intense emissions,
and each cluster includes tens of individual spikes. When the intensity
of background pulsation is increased, the intensity, duration and
bandwidth of the spike cluster are also enlarged. There are 21 groups of
QPSs throughout the confined flare. The central frequency of the whole
group shifts from 1.9 to 1.2 GHz, and the duration of each cluster shows
a negative exponential decay pattern. We propose that nonthermal
electron beams play a crucial role in emitting both pulsations and
spikes. The tearing-mode oscillations of a confined flux rope produce
periodic accelerated electron beams. These electron beams travel inside
the closed magnetic structure to produce frequency drifting pulsations
via plasma emission and scattered narrowband spikes by electron-
cyclotron maser emission (ECME). The slow rise of flux rope makes the
source region move upward, and thus, QPSs shift towards low frequency.
We propose that the confined flux rope may provide the essential
conditions for the formation of QPSs.</description>
</item>
<item>
<title> Duration and Fluence of Major Solar Energetic Particle (SEP) Events</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...71F</link>
<description>To understand solar energetic particle (SEP) events and their
acceleration processes, it is important to study the SEP properties,
e.g. duration and fluence. In this work, we analyzed the temporal
evolution of fluxes [cm&lt;SUP&gt;2&lt;/SUP&gt; sr&lt;SUP&gt;1&lt;/SUP&gt; s&lt;SUP&gt;1&lt;/SUP&gt;] of
&gt;10, &gt;30, and &gt;60 MeV protons and the temporal and spectral evolution of
electromagnetic-radiation components for 34 major SEP events that
include 13 ground-level enhancement (GLE)-SEP and 21 non-GLE-SEP events,
and then determined their possible onset and end times [UT], their
duration [hours], and fluence [cm&lt;SUP&gt;2&lt;/SUP&gt; sr&lt;SUP&gt;1&lt;/SUP&gt;]. It is
observed that the temporal fluxes of &gt;30 MeV protons can sometimes be
utilized for those of the fluxes of &gt;10 MeV protons. Correspondence
between SEP duration and fluence demonstrates the dependence of fluence
on duration that helps distinguish the typical and atypical SEP events.
For instance, for the &gt;10 MeV protons, correspondence between the
duration and fluence exhibited a weaker correlation (r  0.78; p &lt;0.002)
during the 13 GLE-SEPs than that (r  0.83; p &lt;0.0001) during the 21
non-GLE-SEPs, revealing a few GLE-SEPs with disproportionate
comparability. During the 13 GLE-SEPs, correspondence between the SEP
duration and fluence for &gt;30 MeV protons exhibited a stronger
correlation (r  0.82; p &lt;0.0006) than that (r  0.78; p &lt;0.002) for the
&gt;10 MeV protons, indicating that the temporal window of &gt;30 MeV protons
is sometimes more appropriate for obtaining a reasonable duration of
SEPs. Accordingly, when the temporal window of flux of &gt;30 MeV protons
is utilized for that of the &gt;10 MeV protons, the correlation increased
significantly (r  0.86; p &lt;0.0002) during the 13 GLE-SEPs.</description>
</item>
<item>
<title> Solar radio emission as a disturbance of radiomobile networks</title>
<link>https://ui.adsabs.harvard.edu/abs/2022NatSR..12.9324M</link>
<description>This paper analyses the effects of solar radio emissions in the
radiomobile context, for the first time leveraging massive European
Telecommunications Standards Institute (ETSI) 3rd Generation Partnership
Program (3GPP) Minimization of Drive Test (MDT) radio measures produced
by 4G LTE (Long Term Evolution) terminals and by 4G LTE Base Station
cells. A method to study solar noise effects starting from radiomobile
3GPP standard MDT measures is illustrated and correlated with the
excellent 10.7 cm (2800 MHz) indicator of solar activity (National
Research Council Canada). The effects of solar disturbance on the LTE
radio access network for mobile services are analysed, and possible
countermeasures are presented from the perspective of radiomobile
network evolution to 5G and 6G.</description>
</item>
<item>
<title> Relationship Between Solar Millimeter and Soft X-Ray Emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2022LatJP..59c..39K</link>
<description>The connection between solar radio and soft X-ray emission has earlier
been studied at various radio frequencies. For instance, the intensity
peak times during solar flares have been compared between these two
wavelength regimes. It has been reported that solar radio emission peaks
before soft X-ray emission during a flare. However, opposite results
have also been presented. In this study, we compare millimetre (8 mm)
solar and soft X-ray emissions (0.5-4  and 1-8 ). The radio
observations were made at Metshovi Radio Observatory of Aalto
University in Finland between 2015 and 2019. The soft X-ray data were
observed with GOES-15 (Geostationary Operational Environmental
Satellite). The data show that the solar millimetre emission can peak
either before or after soft X-ray peak emission. In this study, we
present two different scenarios, which could explain the peaking time
differences and behaviour. The first scenario proposes a tight
connection between the millimetre (8 mm) and soft X-ray emissions, the
second one is for cases where the emission mechanisms are more separate.</description>
</item>
<item>
<title> Driving Influences of the Doppler Flash Observed by SuperDARN HF Radars in Response to Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2022JGRA..12730342C</link>
<description>Sudden enhancement in high-frequency absorption is a well-known impact
of solar flare-driven Short-Wave Fadeout (SWF). Less understood, is a
perturbation of the radio wave frequency as it traverses the ionosphere
in the early stages of SWF, also known as the Doppler flash.
Investigations have suggested two possible sources that might contribute
to it's manifestation: first, enhancements of plasma density in the
D-and lower E-regions; second, the lowering of the F-region reflection
point. Our recent work investigated a solar flare event using first
principles modeling and Super Dual Auroral Radar Network (SuperDARN) HF
radar observations and found that change in the F-region refractive
index is the primary driver of the Doppler flash. This study analyzes
multiple solar flare events observed across different SuperDARN HF
radars to determine how flare characteristics, properties of the
traveling radio wave, and geophysical conditions impact the Doppler
flash. In addition, we use incoherent scatter radar data and first-
principles modeling to investigate physical mechanisms that drive the
lowering of the F-region reflection points. We found, (a) on average,
the change in E- and F-region refractive index is the primary driver of
the Doppler flash, (b) solar zenith angle, ray's elevation angle,
operating frequency, and location of the solar flare on the solar disk
can alter the ionospheric regions of maximum contribution to the Doppler
flash, (c) increased ionospheric Hall and Pedersen conductance causes a
reduction of the daytime eastward electric field, and consequently
reduces the vertical ion-drift in the lower and middle latitude
ionosphere, which results in lowering of the F-region ray reflection
point.</description>
</item>
<item>
<title> Similarities and Differences between Forbush Decreases Associated with Streams from Coronal Holes, Filament Ejections, and Ejections from Active Regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62..159M</link>
<description>The Forbush decreases for the period from 1997 to 2020 were studied
based on data from the database on Forbush effects and interplanetary
disturbances created and maintained at the Pushkov Institute of
Terrestrial Magnetism, Ionosphere, and Radio Wave Propagation (IZMIRAN).
Using statistical methods, we compared the Forbush decreases associated
with coronal mass ejections from active regions of the Sun accompanied
by solar flares; filament ejections outside active regions; high-speed
streams from coronal holes; and several sources. The difference between
Forbush decreases was related to coronal mass ejections when magnetic
clouds in the interplanetary disturbances near the Earth were observed
or not observed. It has been shown that the distributions of most of
parameters are asymmetric for the sporadic Forbush decreases; for the
recurrent Forbush decreases, they are nearly symmetric. The strongest
correlations between the parameters of Forbush decreases and
interplanetary disturbances are observed in the group of coronal
ejections from active regions that are accompanied by solar flares and
have a structure of magnetic cloud.</description>
</item>
<item>
<title> A Genetic Algorithm to Model Solar Radio Active Regions From 3D Magnetic Field Extrapolations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...9.1118D</link>
<description>In recent decades our understanding of solar active regions (ARs) has
improved substantially due to observations made with better angular
resolution and wider spectral coverage. While prior AR observations have
shown that these structures were always brighter than the quiet Sun at
centimeter wavelengths, recent observations at millimeter and
submillimeter wavelengths have shown ARs with well defined dark umbrae.
Given this new information, it is now necessary to update our
understanding and models of the solar atmosphere in active regions. In
this work, we present a data-constrained model of the AR solar
atmosphere, in which we use brightness temperature measurements of NOAA
12470 at three radio frequencies: 17, 100 and 230 GHz. The observations
at 17 GHz were made by the Nobeyama Radioheliograph (NoRH), while the
observations at 100 and 230 GHz were obtained by the Atacama Large
Millimeter/submillimeter Array (ALMA). Based on our model, which assumes
that the radio emission originates from thermal free-free and
gyroresonance processes, we calculate radio brightness temperature maps
that can be compared with the observations. The magnetic field at
distinct atmospheric heights was determined in our modelling process by
force-free field extrapolation using photospheric magnetograms taken by
the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics
Observatory (SDO). In order to determine the best plasma temperature and
density height profiles necessary to match the observations, the model
uses a genetic algorithm that modifies a standard quiet Sun atmospheric
model. Our results show that the height of the transition region (TR) of
the modelled atmosphere varies with the type of region being modelled:
for umbrae the TR is located at 1080  20 km above the solar surface;
for penumbrae, the TR is located at 1800  50 km; and for bright regions
outside sunspots, the TR is located at 2000  100 km. With these
results, we find good agreement with the observed AR brightness
temperature maps. Our modelled AR can be used to estimate the emission
at frequencies without observational coverage.</description>
</item>
<item>
<title> The Algorithm</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932..110K</link>
<description>Coronal magnetic fields are well known to be one of the crucial
parameters defining coronal physics and space weather. However,
measuring the global coronal magnetic fields remains challenging. The
polarization properties of coronal radio emissions are sensitive to
coronal magnetic fields. While they can prove to be useful probes of
coronal and heliospheric magnetic fields, their usage has been limited
by technical and algorithmic challenges. We present a robust algorithm
for precise polarization calibration and imaging of low-radio frequency
solar observations and demonstrate it on data from the Murchison
Widefield Array, a Square Kilometre Array (SKA) precursor. This
algorithm is based on the Measurement Equation framework, which forms
the basis of all modern radio interferometric calibration and imaging.
It delivers high-dynamic-range and high-fidelity full-Stokes solar radio
images with instrumental polarization leakages &lt;1%, on par with general
astronomical radio imaging, and represents the state of the art. Opening
up this rewarding, yet unexplored, phase space will enable multiple
novel science investigations and offer considerable discovery potential.
Examples include detection of low-level circular polarization from
thermal coronal emission to estimate large-scale quiescent coronal
fields; polarization of faint gyrosynchrotron emissions from coronal
mass ejections for robust estimation of plasma parameters; and detection
of the first-ever linear polarization at these frequencies. This method
has been developed with the SKA in mind and will enable a new era of
high-fidelity spectropolarimetric snapshot solar imaging at low radio
frequencies.</description>
</item>
<item>
<title> The Temporal and Spatial Behaviors of CME Occurrence Rate at Different Latitudes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932...62L</link>
<description>The statistical study of the coronal mass ejections (CMEs) is a hot
topic in solar physics. To further reveal the temporal and spatial
behaviors of the CMEs at different latitudes and heights, we analyzed
the correlation and phase relationships between the occurrence rate of
CMEs, the coronal brightness index (CBI), and the 10.7 cm solar radio
flux (F10.7). We found that the occurrence rate of the CMEs correlates
with the CBI relatively stronger at high latitudes (60) than at low
latitudes (50). At low latitudes, the occurrence rate of the CMEs
correlates relatively weaker with the CBI than the F10.7. There is a
relatively stronger correlation relationship between CMEs, the F10.7,
and the CBI during Solar Cycle 24 (SC24) than Solar Cycle 23 (SC23).
During SC23, the high-latitude CME occurrence rate lags behind the F10.7
by 3 months, and during SC24, the low-latitude CME occurrence rate leads
the low-latitude CBI by 1 month. The correlation coefficient values turn
out to be larger when the very faint CMEs are removed from the samples
of the CDAW catalog. Based on our results, we may speculate that the
source regions of the high/low-latitude CMEs may vary in height, and the
process of magnetic energy accumulation and dissipation is from the
lower to the upper atmosphere of the Sun. The temporal offsets between
different indicators could help us better understand the physical
processes responsible for the solar-terrestrial interactions.</description>
</item>
<item>
<title> Implications for Additional Plasma Heating Driving the Extreme-ultraviolet Late Phase of a Solar Flare with Microwave Imaging Spectroscopy</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932...53Z</link>
<description>Extreme-ultraviolet late phase (ELP) refers to the second extreme-
ultraviolet (EUV) radiation enhancement observed in certain solar
flares, which usually occurs tens of minutes to several hours after the
peak of soft X-ray emission. The coronal loop system that hosts the ELP
emission is often different from the main flaring arcade, and the
enhanced EUV emission therein may imply an additional heating process.
However, the origin of the ELP remains rather unclear. Here we present
the analysis of a C1.4 flare that features such an ELP, which is also
observed in microwave wavelengths by the Expanded Owens Valley Solar
Array. Similar to the case of the ELP, we find a gradual microwave
enhancement that occurs about 3 minutes after the main impulsive phase
microwave peaks. Radio sources coincide with both foot points of the ELP
loops and spectral fits on the time-varying microwave spectra
demonstrate a clear deviation of the electron distribution from the
Maxwellian case, which could result from injected nonthermal electrons
or nonuniform heating to the footpoint plasma. We further point out that
the delayed microwave enhancement suggests the presence of an additional
heating process, which could be responsible for the evaporation of
heated plasma that fills the ELP loops, producing the prolonged ELP
emission.</description>
</item>
<item>
<title> Circular Polarization Observations of Type II Solar Radio Bursts and the Coronal Magnetic Field</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932...48R</link>
<description>It is well known that magnetic field strength (B) in the solar corona
can be calculated using the Alfvn Mach number (M &lt;SUB&gt; A &lt;/SUB&gt;) and
Alfvn speed (v &lt;SUB&gt; A &lt;/SUB&gt;) of the magnetohydrodynamic shock waves
associated with coronal type II radio bursts. We show that observations
of weak circularly polarized emission associated with the harmonic
component of the type II bursts provide independent and consistent
estimates of B. For the coronal type II burst observed on 2021 October
9, we obtained B 1.5 G and 1.9 G at a heliocentric distance (r) of
1.8 R &lt;SUB&gt;&lt;/SUB&gt;, using the above two techniques, respectively.</description>
</item>
<item>
<title> Harmonic Electron Cyclotron Maser Emission along the Coronal Loop</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932...35Y</link>
<description>Efficient radiation at second and/or higher harmonics of &lt;SUB&gt;ce&lt;/SUB&gt;
has been suggested to circumvent the escaping difficulty of the electron
cyclotron maser emission mechanism when it is applied to solar radio
bursts, such as spikes. In our earlier study, we developed a three-step
numerical scheme to connect the dynamics of energetic electrons within a
large-scale coronal loop structure with the microscale kinetic
instability energized by the obtained nonthermal velocity distribution
and found that direct and efficient harmonic X-mode (X2 for short)
emission can be achieved due to the strip-like features of the
distribution. That study only considered the radiation from the loop top
at a specific time. Here we present the emission properties along the
loop at different locations and timings. We found that, in accordance
with our earlier results, few to several strip-like features can appear
in all cases, and the first two strips play the major role in exciting
X2 and Z (i.e., the slow extraordinary mode) that propagate quasi-
perpendicularly. For the four sections along the loop, significant
excitation of X2 is observed from the upper two sections, and the
strongest emission is from the top section. In addition, significant
excitation of Z is observed for all loop sections, while there is no
significant emission of the fundamental X mode. The study provides new
insight into coherent maser emission along the coronal loop structure
during solar flares.</description>
</item>
<item>
<title> Imaging of the Quiet Sun in the Frequency Range of 20-80 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...932...17Z</link>
<description>Radio emission of the quiet Sun is considered to be due to thermal
bremsstrahlung emission of the hot solar atmosphere. The properties of
the quiet Sun in the microwave band have been well studied, and they can
be well described by the spectrum of bremsstrahlung emission. In the
meter-wave and decameter-wave bands, properties of the quiet Sun have
rarely been studied due to the instrumental limitations. In this work,
we use the LOw Frequency ARray telescope to perform high quality
interferometric imaging spectroscopy observations of quiet Sun coronal
emission at frequencies below 90 MHz. We present the brightness
temperature spectrum and the size of the Sun in the frequency range of
20-80 MHz. We report on dark coronal regions with low brightness
temperatures that persist with frequency. The brightness temperature
spectrum of the quiet Sun is discussed and compared with the
bremsstrahlung emission of a coronal model and previous quiet Sun
observations.</description>
</item>
<item>
<title> Quasi-periodic Accelerations of Energetic Particles during a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...931L..28L</link>
<description>We report the observation of nonstationary quasi-periodic pulsations
(QPPs) in high-energy particles during the impulsive phase of an X4.8
flare on 2002 July 23 (SOL2002-07-23T00:35). The X4.8 flare was
simultaneously measured by the Reuven Ramaty High Energy Solar
Spectroscopic Imager, Nobeyama Radio Polarimeters, and Nobeyama
Radioheliograph. The quasi-period of ~50  15 s, determined by the
wavelet transform, is detected in the -ray line emission. Using the
same method, a quasi-period of ~90  20 s is found in the -ray
continuum, hard X-ray (HXR), and radio emissions during almost the same
time. Our observations suggest that the flare QPPs should be associated
with energetic ions and nonthermal electrons that are quasi-periodically
accelerated by the repetitive magnetic reconnection. The different
quasi-periods between the -ray line and continuum/HXR/radio emissions
indicate an apparent difference in acceleration or propagation between
energetic ions and nonthermal electrons of this solar flare.</description>
</item>
<item>
<title> Recombination Radio Lines of the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ARep...66..490D</link>
<description>The lines observed in the spectra of astronomical objects provide unique
information about them. Currently, only one radio line has been detected
in the spectrum of the Sun: a hydrogen fine structure line
2&lt;SUP&gt;2&lt;/SUP&gt;P&lt;SUB&gt;3/2&lt;/SUB&gt;-2&lt;SUP&gt;2&lt;/SUP&gt;S&lt;SUB&gt;1/2&lt;/SUB&gt; at the
frequency 9845 MHz (3.05 cm). It was also found that in the spectrum of
solar active formations above sunspots, two more hydrogen fine structure
lines are observed with high probability:
3&lt;SUP&gt;2&lt;/SUP&gt;P&lt;SUB&gt;3/2&lt;/SUB&gt;-3&lt;SUP&gt;2&lt;/SUP&gt;S&lt;SUB&gt;1/2&lt;/SUB&gt; and
3&lt;SUP&gt;2&lt;/SUP&gt;D&lt;SUB&gt;3/2&lt;/SUB&gt;-3&lt;SUP&gt;2&lt;/SUP&gt;P&lt;SUB&gt;1/2&lt;/SUB&gt; at the
frequencies 2917 and 3237 MHz (10.28 and 9.27 cm). The analysis of long-
term spectral observations of the Sun by the RATAN-600 radio telescope
has shown that numerous recombination radio lines of hydrogen and other
elements should be observed in the spectrum of solar active formations
above sunspots.</description>
</item>
<item>
<title> First detection of metric emission from a solar surge</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...662A..14A</link>
<description>We report the first detection of metric radio emission from a surge,
observed with the Nanay Radioheliograph (NRH), STEREO, and other
instruments. The emission was observed during the late phase of the M9
complex event SOL2010-02-012T11:25:00, described in a previous
publication. It was associated with a secondary energy release, also
observed in STEREO 304  images, and there was no detectable soft X-ray
emission. The triangulation of the STEREO images allowed for the
identification of the surge with NRH sources near the central meridian.
The radio emission of the surge occurred in two phases and consisted of
two sources, one located near the base of the surge, apparently at or
near the site of energy release, and another in the upper part of the
surge; these were best visible in the frequency range of 445.0 to about
300 MHz, whereas a spectral component of a different nature was observed
at lower frequencies. Sub-second time variations were detected in both
sources during both phases, with a 0.2-0.3 s delay of the upper source
with respect to the lower, suggesting superluminal velocities. This
effect can be explained if the emission of the upper source was due to
scattering of radiation from the source at the base of the surge. In
addition, the radio emission showed signs of pulsations and spikes. We
discuss possible emission mechanisms for the slow time variability
component of the lower radio source. Gyrosynchrotron emission reproduced
the characteristics of the observed total intensity spectrum at the
start of the second phase of the event fairly well, but failed to
reproduce the high degree of the observed circular polarization or the
spectra at other instances. On the other hand, type IV-like plasma
emission from the fundamental could explain the high polarization and
the fine structure in the dynamic spectrum; moreover, it gives projected
radio source positions on the plane of the sky, as seen from STEREO-A,
near the base of the surge. Taking all the properties into
consideration, we suggest that type IV-like plasma emission with a low-
intensity gyrosynchrotron component is the most plausible mechanism. &lt;P
/&gt;Movie associated to Fig. A.2 is available at &lt;A href="https://www.aand
a.org/10.1051/0004-6361/202243169/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> Solar Radio Bursts Associated with In Situ Detected Energetic Electrons in Solar Cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....8..275M</link>
<description>The first comprehensive analysis between the in situ detected solar
energetic electrons (SEEs) from ACE/EPAM satellite and remotely observed
radio signatures in solar cycles (SCs) 23 and 24 (19972019) is
presented. The identified solar origin of the SEEs (in terms of solar
flares, SFs, and coronal mass ejections, CMEs) is associated with solar
radio emission of types II, III and IV, where possible. Occurrence rates
are calculated as a function of the radio wavelength, from the low
corona to the interplanetary space near Earth. The tendencies of the
different burst appearances with respect to SC, helio-longitude, and SEE
intensity are also demonstrated. The corresponding trends of the driver
(in terms of median values of the SF class and CME projected speed) are
also shown. A comparison with the respective results when using solar
energetic protons is presented and discussed.</description>
</item>
<item>
<title> Kinematic Study of Radio-Loud CMEs Associated with Solar Flares and DH Type-II Radio Emissions During Solar Cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...57P</link>
<description>We have statistically analyzed 379 radio-loud (RL) CMEs and their
associated flares during the period 1996 - 2019 covering both Solar
Cycles (SC) 23 and 24. We classified them into two populations based on
the observation period: i ) 235 events that belong to SC 23 (August 1996
- December 2008) and ii ) 144 events that belong to SC 24 (January 2009
- December 2019). For both cycles, the mean sky-plane speed, projection
corrected speed (space speed), and initial acceleration of RL CMEs are
found to be similar. Moreover, the average residual acceleration of RL
CMEs in SC 24 (17.39 43.51 m s&lt;SUP&gt;2&lt;/SUP&gt;) is twice lower than that
of the RL CMEs in SC 23 (8.29 36.23 m s&lt;SUP&gt;2&lt;/SUP&gt;), which means
that the deceleration of RL CMEs in SC 24 is twice as fast as in SC 23.
RL CMEs reach their peak speed at higher altitudes in SC 23 (1443 504
km s&lt;SUP&gt;1&lt;/SUP&gt;; 13.82 7.40 R&lt;SUB&gt;&lt;/SUB&gt;) than SC 24 (1920 649 km
s&lt;SUP&gt;1&lt;/SUP&gt;; 12.51 7.41 R&lt;SUB&gt;&lt;/SUB&gt;). We also observed that the
mean apparent widths of RL CMEs in SC 23 are less than in SC 24, which
is statistically significant. SC 23 has a lower average CME nose height
(3.85 R&lt;SUB&gt;&lt;/SUB&gt;) at the start time of DH type-II bursts than that of
SC 24 (3.46 R&lt;SUB&gt;&lt;/SUB&gt;). The starting frequencies of DH type-II
bursts associated with RL CMEs for SC 24 are significantly larger
(formed at lower heights) than those of SC 23. We found that there is a
good correlation between the drift rates and the midfrequencies of DH
type-II radio bursts for both of these solar cycles (R&lt;SUP&gt;2&lt;/SUP&gt; =
0.80,  = 1.53). Most of the RL CMEs kinematics and their associated
solar-flare properties are found to be similar for SC 23 and SC 24. The
annual variations for the general population of CMEs are well consistent
with the mean sunspot number but small variations in halo and RL CMEs
are observed. We concluded that the reduced total pressure in the
heliosphere for SC 24 enables RL CMEs to expand wider and decelerate
faster, resulting in DH type-II radio emissions at lower heights than
for SC 23.</description>
</item>
<item>
<title> Spectroscopy of Electric-Field Oscillations in the Solar Wind During the Passage of a Type III Radio Burst Using Observations Compared with Self-Similar Theory</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...50F</link>
<description>We present a spectrum of electric-field oscillations observed in situ in
the solar wind by the WAVES experiment on the Wind spacecraft during the
passage of a type III solar radio burst. 19 frequencies of this spectrum
are compared with recent predictions of a self-similar nonlinear theory
of two-dimensional electron oscillations (Osherovich and Fainberg,
2018).</description>
</item>
<item>
<title> A novel solar radio spectrogram encryption algorithm based on parameter variable chaotic systems and DNA dynamic encoding</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PhyS...97e5210S</link>
<description>Considering that chaotic systems are highly sensitive to parameters, we
design two new parameter variable chaotic systems by constructing
parameter perturbation items. These systems are constructed using the
state variables of the Liu chaotic system to perturb the parameters of
the Lorenz and Chen chaotic systems and are called the Lorenz-Liu
chaotic system (LLCS) and Chen-Liu chaotic system (CLCS), respectively.
In particular, the parameter perturbation items constructed in this
study are not periodic but rather chaotic signals and change in real
time. Compared with the original systems, they exhibit more complex
randomness and dynamic behaviors. In the proposed cryptosystem, which
considers the concept of Deoxyribonucleic Acid (DNA), the solar radio
spectrogram is dynamically encoded through the LLCS, and then, the CLCS
is used to scramble and diffuse the decoding matrices. In addition, the
algorithm uses the 256-bit Secure Hash Algorithm (SHA-256) to generate
the initial keys, which enhances the algorithm's sensitivity to
plaintext. Simulation results and security analysis show that the
cryptosystem has a large key space and high key sensitivity, and can
resist various attacks, such as differential attacks and chosen-
plaintext attacks.</description>
</item>
<item>
<title> The Solar Cycle Clock</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrASS...9.6670L</link>
<description>The Sun's variability is controlled by the progression and interaction
of the magnetized systems that form the 22-year magnetic activity cycle
(the "Hale Cycle") as they march from their origin at 55 latitude to
the equator, over 19 years. We will discuss the end point of that
progression, dubbed "terminator" events, and our means of diagnosing
them. In this paper we expand on the Extended Solar Cycle framework to
construct a new solar activity "clock" which maps all solar magnetic
activity onto a single normalized epoch based on the terminations of
Hale Magnetic Cycles. Defining phase 0*2 on this clock as the
Terminators, then solar polar field reversals occur at  0.2*2, and the
geomagnetically quiet intervals centered around solar minimum start at 
0.6*2 and end at the terminator, thus lasting 40% of the cycle length.
At this onset of quiescence, dubbed a "pre-terminator," the Sun shows a
radical reduction in active region complexity and, like the terminator
events, is associated with the time when the solar radio flux crosses
F10.7 = 90 sfu. We use the terminator-based clock to illustrate a range
of phenomena that further emphasize the strong interaction of the
global-scale magnetic systems of the Hale Cycle: the vast majority, 96%,
of all X-flares happen between the Terminator and pre-Terminator. In
addition to the X-rays from violent flares, rapid changes in the number
of energetic photonsEUV spectral emission from a hot corona and the
F10.7 solar radio fluximpinging on the atmosphere are predictable from
the Terminator-normalized unit cycle, which has implications for
improving the fidelity of atmospheric modelling.</description>
</item>
<item>
<title> Statistical Analysis of Circular-ribbon Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJS..260...19Z</link>
<description>Circular-ribbon flares (CFs) are a special type of solar flares owing to
their particular magnetic topology. In this paper, we conducted a
comprehensive statistical analysis of 134 CFs from 2011 September to
2017 June, including 4 B-class, 82 C-class, 40 M-class, and 8 X-class
flares. The flares were observed by the Atmospheric Imaging Assembly on
board the Solar Dynamics Observatory spacecraft. The physical properties
of CFs are derived, including the location, area (A &lt;SUB&gt;CF&lt;/SUB&gt;),
equivalent radius (r &lt;SUB&gt;CF&lt;/SUB&gt;) assuming a semispherical fan dome,
lifetime ( &lt;SUB&gt;CF&lt;/SUB&gt;), and peak soft X-ray (SXR) flux in 1-8 . It
is found that all CFs are located in active regions, with the latitudes
between -30 and 30. The distributions of areas and lifetimes could be
fitted with a lognormal function. There is a positive correlation
between the lifetime and area. The peak SXR flux in 1-8  is well in
accord with a power-law distribution with an index of -1.42. For the 134
CFs, 57% of them are accompanied by remote brightenings or ribbons. A
positive correlation exists between the total length (L &lt;SUB&gt;RB&lt;/SUB&gt;)
and average distance (D &lt;SUB&gt;RB&lt;/SUB&gt;) of remote brightenings. About 47%
and 51% of the 134 CFs are related to type III radio bursts and jets,
respectively. The association rates are independent of flare energies.
About 38% of CFs are related to minifilament eruptions, and the
association rates increase with flare classes. Only 28% of CFs are
related to coronal mass ejections (CMEs), meaning that a majority of
them are confined rather than eruptive events. There is a positive
correlation between the CME speed and peak SXR flux in 1-8 , and faster
CMEs tend to be wider.</description>
</item>
<item>
<title> Multi-instrument Comparative Study of Temperature, Number Density, and Emission Measure during the Precursor Phase of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...930..154L</link>
<description>We present a multi-instrument study of the two precursor brightenings
prior to the M6.5 flare (SOL2015-06-22T18:23) in the NOAA Active Region
12371, with a focus on the temperature (T), electron number density (n),
and emission measure (EM). The data used in this study were obtained
from four instruments with a variety of wavelengths, i.e., the Solar
Dynamics Observatory's Atmospheric Imaging Assembly (AIA), in six
extreme ultraviolet (EUV) passbands; the Expanded Owens Valley Solar
Array (EOVSA) in microwave (MW); the Reuven Ramaty High Energy Solar
Spectroscopic Imager (RHESSI) in hard X-rays (HXR); and the
Geostationary Operational Environmental Satellite (GOES) in soft X-rays
(SXR). We compare the temporal variations of T, n, and EM derived from
the different data sets. Here are the key results. (1) GOES SXR and AIA
EUV have almost identical EM variations (1.5-3  10&lt;SUP&gt;48&lt;/SUP&gt;
cm&lt;SUP&gt;-3&lt;/SUP&gt;) and very similar T variations, from 8 to 15 million
Kelvin (MK). (2) Listed from highest to lowest, EOVSA MW provides the
highest temperature variations (15-60 MK), followed by RHESSI HXR (10-24
MK), then GOES SXR and AIA EUV (8-15 MK). (3) The EM variation from the
RHESSI HXR measurements is always less than the values from AIA EUV and
GOES SXR by at most 20 times. The number density variation from EOVSA MW
is greater than the value from AIA EUV by at most 100 times. The results
quantitatively describe the differences in the thermal parameters at the
precursor phase, as measured by different instruments operating at
different wavelength regimes and for different emission mechanisms.</description>
</item>
<item>
<title> A first look at the submillimeter Sun with ALMA</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...661L...4A</link>
<description>We present the first full-disk solar images obtained with the Atacama
Large Millimeter/submillimeter Array (ALMA) in Band 7 (0.86 mm; 347
GHz). In spite of the low spatial resolution (21), several interesting
results were obtained. During our observation, the sun was practically
devoid of active regions. Quiet Sun structures on the disk are similar
to those in Atmospheric Imaging Assembly images at 1600  and 304 ,
after the latter are smoothed to the ALMA resolution, as noted
previously for Band 6 (1.26 mm) and Band 3 (3 mm) images; they are also
similar to negative H images of equivalent resolution. Polar coronal
holes, which are clearly seen in the 304  band and small H filaments,
are not detectable at 0.86 mm. We computed the center-to-limb variation
of the brightness temperature, T&lt;SUB&gt;b&lt;/SUB&gt;, in Band 7, as well as in
Bands 6 and 3, which were obtained during the same campaign, and we
combined them to a unique curve of T&lt;SUB&gt;b&lt;/SUB&gt;(log &lt;SUB&gt;100&lt;/SUB&gt;),
where &lt;SUB&gt;100&lt;/SUB&gt; is the cosine of the heliocentric angle reduced to
100 GHz. Assuming that the absolute calibration of the Band 3
commissioning observations is accurate, we deduced a brightness
temperature at the center of the disk of 6085 K for Band 7, instead of
the value of 5500 K, extrapolated from the recommended values for Bands
3 and 6. More importantly, the T&lt;SUB&gt;b&lt;/SUB&gt;(log &lt;SUB&gt;100&lt;/SUB&gt;) curve
flattens at large values of &lt;SUB&gt;100&lt;/SUB&gt;, and so does the
corresponding T&lt;SUB&gt;e&lt;/SUB&gt;(log &lt;SUB&gt;100&lt;/SUB&gt;) at large
&lt;SUB&gt;100&lt;/SUB&gt;. This is probably an indication that we are approaching
the temperature minimum.</description>
</item>
<item>
<title> Power distribution of oscillations in the atmosphere of a plage region. Joint observations with ALMA, IRIS, and SDO</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...661A..95N</link>
<description>Context. Joint observations of the Atacama Large
Millimeter/Submillimeter Array (ALMA) with other solar observatories can
provide a wealth of opportunities for understanding the coupling between
different layers of the solar atmosphere. &lt;BR /&gt; Aims: We present a
statistical analysis of the power distribution of oscillations in a
plage region in active region NOAA AR12651, which was observed jointly
with ALMA, the Interface Region Imaging Spectrograph (IRIS), and the
Solar Dynamics Observatory (SDO). &lt;BR /&gt; Methods: We employ coordinated
ALMA Band 6 (1.25 mm) brightness temperature maps, IRIS slit-jaw images
in the 2796  passband, and observations in six passbands (1600 , 304
, 131 , 171 , 193 , and 211 ) from the Atmospheric Imaging Assembly
(AIA) on board SDO. We perform Lomb-Scargle transforms to study the
distribution of oscillation power by means of dominant period maps and
power maps. We study the spatial association of oscillations through the
atmosphere, with a focus on the correlation of the power distribution of
ALMA oscillations with others. &lt;BR /&gt; Results: We do not observe any
significant association of ALMA oscillations with IRIS and AIA
oscillations. While the global behavior of the dominant ALMA
oscillations shows a similarity with that of the transition region and
coronal passbands of AIA, the ALMA dominant period maps and power maps
do not show any correlation with those from the other passbands. The
spatial distribution of dominant periods and power in different period
intervals of ALMA oscillations is uncorrelated with those of any other
passbands. &lt;BR /&gt; Conclusions: We speculate that the non-association of
ALMA oscillations with those of IRIS and AIA is due to significant
variations in the height of formation of the millimeter continuum
observed by ALMA. Additionally, the fact that ALMA directly maps the
brightness temperature, in contrast to the intensity observations by
IRIS and AIA, can result in the very different intrinsic nature of the
ALMA oscillations compared to the IRIS and AIA oscillations.</description>
</item>
<item>
<title> Heating of the solar chromosphere through current dissipation</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...661A..59D</link>
<description>Context. The solar chromosphere is heated to temperatures higher than
predicted by radiative equilibrium. This excess heating is greater in
active regions where the magnetic field is stronger. &lt;BR /&gt; Aims: We aim
to investigate the magnetic topology associated with an area of enhanced
millimeter (mm) brightness temperatures in a solar active region mapped
by the Atacama Large Millimeter/submillimeter Array (ALMA) using
spectropolarimetric co-observations with the 1-m Swedish Solar Telescope
(SST). &lt;BR /&gt; Methods: We used Milne-Eddington inversions, nonlocal
thermodynamic equilibrium (non-LTE) inversions, and a magnetohydrostatic
extrapolation to obtain constraints on the three-dimensional (3D)
stratification of temperature, magnetic field, and radiative energy
losses. We compared the observations to a snapshot of a
magnetohydrodynamics simulation and investigate the formation of the
thermal continuum at 3 mm using contribution functions. &lt;BR /&gt; Results:
We find enhanced heating rates in the upper chromosphere of up to 5 kW
m&lt;SUP&gt;2&lt;/SUP&gt;, where small-scale emerging loops interact with the
overlying magnetic canopy leading to current sheets as shown by the
magnetic field extrapolation. Our estimates are about a factor of two
higher than canonical values, but they are limited by the ALMA spatial
resolution (1.2). Band 3 brightness temperatures reach about
10&lt;SUP&gt;4&lt;/SUP&gt; K in the region, and the transverse magnetic field
strength inferred from the non-LTE inversions is on the order of 500 G
in the chromosphere. &lt;BR /&gt; Conclusions: We are able to quantitatively
reproduce many of the observed features including the integrated
radiative losses in our numerical simulation. We conclude that the
heating is caused by dissipation in current sheets. However, the
simulation shows a complex stratification in the flux emergence region
where distinct layers may contribute significantly to the emission in
the mm continuum. &lt;P /&gt;The movie is available at &lt;A href="https://www.aa
nda.org/10.1051/0004-6361/202243191/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> Simulations of solar radio zebras</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...661A..56K</link>
<description>Context. Solar radio zebras are used in diagnostics of solar flare
plasmas and it is of great importance to construct accurate models to
correctly characterize them. &lt;BR /&gt; Aims: We simulated two zebras to
verify their double-plasma resonance (DPR) model. &lt;BR /&gt; Methods: In our
zebra simulations, we used the DPR model in an expanding and compressing
part of the loop as well as with the wave propagating along the loop.
&lt;BR /&gt; Results: Using the DPR model in such a loop, we successfully
simulated zebras from the 1 August 2010 and 21 June 2011 flares. We
found that increasing the density or decreasing the magnetic field in
the part of the loop, where zebra-stripe sources are located, the zebra
stripes are shifted to higher frequencies and vice versa. In the case of
the 21 June 2011 flare, we confirm that small deviations of zebra-stripe
frequencies from their mean values can be explained by waves propagating
along the loop. We also confirm high values for the gyro-harmonic number
of zebra stripes. We explain an inconsistency in the wave velocities
derived from the plasma parameters and from the frequency drift in
combination with the density model of the solar atmosphere. Finally, we
discuss the high values of the gyro-harmonic number found in the studied
zebras.</description>
</item>
<item>
<title> Exploring the Circular Polarisation of Low-Frequency Solar Radio Bursts with LOFAR</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...47M</link>
<description>The Sun is an active star that often produces numerous bursts of
electromagnetic radiation at radio wavelengths. Low frequency radio
bursts have recently been brought back to light with the advancement of
novel radio interferometers. However, their polarisation properties have
not yet been explored in detail, especially with the Low Frequency Array
(LOFAR), due to difficulties in calibrating the data and accounting for
instrumental leakage. Here, using a unique method to correct the
polarisation observations, we explore the circular polarisation of
different sub-types of solar type III radio bursts and a type I noise
storm observed with LOFAR, which occurred during March-April 2019. We
analysed six individual radio bursts from two different dates. We
present the first Stokes V low frequency images of the Sun with LOFAR in
tied-array mode observations. We find that the degree of circular
polarisation for each of the selected bursts increases with frequency
for fundamental emission, while this trend is either not clear or absent
for harmonic emission. The type III bursts studied, that are part of a
long-lasting type III storm, can have different senses of circular
polarisation, occur at different locations and have different
propagation directions. This indicates that the type III bursts forming
a classical type III storm do not necessarily have a common origin, but
instead they indicate the existence of multiple, possibly unrelated
acceleration processes originating from solar minimum active regions.</description>
</item>
<item>
<title> Mitigation of Radio Frequency Interference in the Solar Radio Spectrum Based on Deep Learning</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...46C</link>
<description>Radio frequency interference (RFI) may contaminate the signal received
by solar radio telescopes. The existence of RFI in the solar radio
spectrum affects the accuracy and efficiency of the extraction of burst
parameters, which is related to the quality of scientific results and
even the authenticity of conclusions. Therefore, it is necessary to
carry out research on RFI recognition algorithms for solar radio data.
This article aims to compare the recognition performance of six
different deep-learning networks (FCN, Deconvnet, Segnet, Unet, Dual-
Resunet, and DSC Based Dual-Resunet) on the RFI in solar radio spectra
observed by the Chinese Solar Broadband Radio Spectrometer (SBRS). The
accuracy and convergence speed in the training process, as well as
various performance metrics in the test, indicate that the proposed DSC
Based Dual-Resunet is the most suitable neural-network for this task and
can achieve both performance and light weight. The RFI recognition
accuracy of the DSC Based Dual-Resunet is close to Unet when there is no
burst in the spectrum, but in the case of a burst DSC Based Dual-Resunet
is obviously better than Unet in terms of RFI recognition. Moreover the
model size and number of parameters are approximately 12.5% of those of
Unet, and the amount of computation is 38% of that of Unet, which
greatly improves the computation efficiency and is of great significance
for the realization of the network on mobile hardware. It is promising
for the large-scale application of RFI recognition for solar radio
telescopes.</description>
</item>
<item>
<title> Detection of Solar Flares from the Analysis of Signal-to-Noise Ratio Recorded by Digisonde at Mid-Latitudes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RemS...14.1898D</link>
<description>This work proposes a new indirect method to detect the impact of solar
flares on ionospheric sounding measurements, i.e., on the signal-to-
noise ratio of ionospheric reflected radio signals. The method allows us
to detect and characterize the ionospheric absorption of high-frequency
radio waves as a product of these energetic events. The detection is
based on the estimation of the quiet conditions signal-to-noise ratio
(SNR) pattern of the month and the subsequent comparison of this pattern
with the SNR for the analyzed day. The method has been tested by using
data from Ebro Observatory ionospheric station (DPS4D, EB040), but it
can be applied to any other ionospheric station. At EB040, it can
provide observational data to the international Service of Rapid
Magnetic Variations (SRMV) to help confirm Sfe (Solar Flare Effects). To
set up the method, we considered a data set of 262 solar flares that
occurred during 2011-2014 and were observed during daylight hours at
EB040 (17 X-class, 124 M-class, and 121 C-class). This led to impose a
threshold of -20 dB in the SNR for at least four consecutive frequencies
to confirm that a solar flare took place. The method is particularly
sensitive for the detection of X-class solar flares, performs quite well
with M-class events, and is even able to detect some C-class flares with
high solar altitude angles. Furthermore, we studied some constraints
that affect the detection of solar flares from the analysis of GOES-15
hard X-ray flux data about the considered events. For each flare, we
computed its solar altitude angle at the time of the ionospheric
sounding to get an estimation of its geoeffective irradiance, which had
an effect on the local ionosphere. We can confirm that the method of
detection is more effective with flares that present a solar elevation
angle higher than 18.94, a geoeffective hard X-ray irradiance above
3.30  10&lt;SUP&gt;-6&lt;/SUP&gt; W/m&lt;SUP&gt;2&lt;/SUP&gt;, and a geoeffective hard X-ray
radiant exposure higher than 1.61  10&lt;SUP&gt;-3&lt;/SUP&gt; J/m&lt;SUP&gt;2&lt;/SUP&gt;,
computed during the 5 min preceding the ionospheric sounding.</description>
</item>
<item>
<title> Probing the Solar Corona at High Temporal and Spatial Resolution with the Low Frequency Array</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PhDT.........2M</link>
<description>The solar corona is the outermost layer of the Sun's atmosphere.
Advancements in radio astronomy over the last 50 years have revealed a
number of radio phenomena which occur in the corona each with different
temporal and spectral characteristics. Current generation
interferometers such as the LOw Frequency ARray (LOFAR) give an
unprecedented insight into the fine spatial, spectral and temporal
structure of these radio bursts. Of particular interest are what are
known as type III radio bursts, which are indicative of electrons
propagating along open magnetic field lines in the solar corona.
Observations of type III bursts allow for the remote sensing of the
plasma at various heights in the corona due to the relation between
emission at the plasma frequency and electron density. High spatial
resolution observations of radio bursts give insight into the role of
radio wave scattering on the observed source sizes while high temporal
and spectral resolution observations can be used to determine the power
density of electron density fluctuations in the corona. Key results of
this thesis come from observations of solar radio emission at the
highest temporal, spectral and spatial resolutions to date. Firstly, the
REAL-time Transient Acquisition backend (REALTA) was developed and
installed at the Irish LOFAR station (I-LOFAR) to record the raw
voltages from the station at $5.12 \mu$s temporal resolution. This is
among the most advanced data acquisition clusters installed at an
international LOFAR station to date. First light observations from
REALTA are shown, including a variety of solar radio bursts showcasing
fine temporal and spectral structure. The installation of REALTA allows
for observations of solar radio bursts at some of the highest temporal
resolutions to date and is a key resource in investigating the fine
temporal structure of solar radio emission. Secondly, a new technique
was implemented to directly measure the size of radio bursts from their
interferometric visibilities. This is the first time that such a
technique has been used to study a type IIIb radio burst. Spectroscopic
analysis of the fine frequency structure of a type IIIb burst is used to
calculate an expected a source size of $3.18$~arcsec. The full width at
half maximum height (FWHM) along the major and minor axes of the burst
at 34.76~MHz is found to be $18.8$~$\pm~0.1$~arcmin and
$10.2$~$\pm~0.1$~arcmin respectively. % at a plane of sky heliocentric
distance of 1.75~R$_\odot$. The new fitting technique used in this
analysis removes the need for interferometric imaging and as such, these
results indicate that the large size observed for the type IIIb radio
burst is due to radio wave scattering in the corona. It is also
determined that this effect may be over estimated by previous tied array
imaging observations.% These results suggest that the level of density
fluctuations in the solar corona is the major cause of the scattering of
radio waves, resulting in large source sizes. Finally, this technique
was utilised to determine the size and shape of 29 type III bursts and
compare them to predictions from state-of-the-art radio wave scattering
simulations. It is found that these bursts have a mean size along the
major and minor axis of FWHM\textsubscript{x} = 16.27~arcmin and
FWHM\textsubscript{y} = 11.96~arcmin respectively. No trend of source
size with respect to helioprojective longitude is found, which is in
contrast to predictions from modelling of anisotropic scattering from a
point source. I attribute this discrepancy to an intrinsic source size
of type III bursts. These results underscore the necessity for thorough
comparison between radio observations and radio wave scattering
simulations before one can be used to infer information from the other.
I highlight some future work that could be built upon the research
presented in this thesis to further advance the knowledge of radio wave
generation and propagation in the solar corona.</description>
</item>
<item>
<title> Geoneutrino Detection and Other Non-Solar Neutrino Physics Achievements of Borexino</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MUPB...77..431Z</link>
<description>The cosmic silence of the underground Gran Sasso laboratory together
with the exceptional radio purity of the liquid scintillator, has
allowed Borexino to investigate the radiogenic heating of the Earth's
interior and to contribute to various fields of experimental neutrino
astronomy. This contribution is aimed to summarize the results obtained
by Borexino on geo-neutrinos and on possible extra-terrestrial sources
of antineutrinos such as supernovae explosions and solar flares.</description>
</item>
<item>
<title> Pulsations of microwave emission from a solar flare in a twisted loop caused by intrinsic magnetohydrodynamic oscillations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.511.2880S</link>
<description>We present results revealing microwave pulsations produced in a model of
a flaring twisted solar coronal loop, without any external oscillatory
driver. Two types of oscillations are identified: slowly decaying
oscillations with a period of about 70-75 s and amplitude of about 5-10
per cent seen in loops both with and without energetic electrons, and
oscillations with a period of about 40 s and amplitude of a few tens of
per cent observed only in loops with energetic electrons for about 100 s
after the onset of fast energy release. We interpret the longer-period
oscillations as the result of a standing kink mode modulating the
average magnetic field strength in the loop, whilst the short-period
intermittent oscillations associated with energetic electrons are likely
to be produced by fast variations of the electric field, which produces
energetic electrons in this scenario. The slowly decaying oscillations
can explain the quasi-periodic pulsations often observed in the flaring
corona.</description>
</item>
<item>
<title> The Coupling of an EUV Coronal Wave and Ion Acceleration in a Fermi-LAT Behind-the-Limb Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...929..172P</link>
<description>We present the Fermi-LAT observations of the behind-the-limb (BTL) flare
of 2021 July 17 and the joint detection of this flare by STIX on board
the Solar Orbiter. The separation between Earth and the Solar Orbiter
was 99.2 at 05:00 UT, allowing STIX to have a front view of the flare.
The location of the flare was S20E140 in Stonyhurst heliographic
coordinates, making this the most distant behind-the-limb flare ever
detected in &gt;100 MeV gamma-rays. The LAT detection lasted for ~16
minutes, the peak flux was 3.6  0.8 (10&lt;SUP&gt;-5&lt;/SUP&gt;) ph
cm&lt;SUP&gt;-2&lt;/SUP&gt; s&lt;SUP&gt;-1&lt;/SUP&gt; with a significance &gt;15. A coronal wave
was observed from both STEREO-A and SDO in extreme ultraviolet (EUV),
with an onset on the visible disk in coincidence with the LAT onset. A
complex type II radio burst was observed by GLOSS also in coincidence
with the onset of the LAT emission, indicating the presence of a shock
wave. We discuss the relation between the time derivative of the EUV
wave intensity profile at 193  as observed by STEREO-A and the LAT flux
to show that the appearance of the coronal wave at the visible disk and
the acceleration of protons as traced by the observed &gt;100 MeV gamma-ray
emission are coupled. We also report how this coupling is present in the
data from three other BTL flares detected by Fermi-LAT, suggesting that
the protons driving the gamma-ray emission of BTL solar flares and the
coronal wave share a common origin.</description>
</item>
<item>
<title> Density Turbulence and the Angular Broadening of Outer Heliospheric Radio Sources at High Latitudes and in the Ecliptic Plane</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...928..125T</link>
<description>Density irregularities are responsible for the scattering of radio waves
in the solar wind and astrophysical plasmas. These irregularities
significantly affect the inferred physical properties of radio sources,
such as size, direction, and intensity. We present here a theory of
angular broadening due to the scattering of radio waves by density
irregularities that improves the existing formalism used to investigate
radio wave scattering in the outer heliosphere and the very local
interstellar medium. The model includes an inner scale and both
latitudinal and radial dependencies for the density fluctuation spectra
and propagation paths for the radiation both near and out of the
ecliptic plane. Based on the pickup-ion-mediated solar wind model (PUI
model) of Zank et al., we estimate the turbulence and solar wind
quantities for the high-latitude fast solar wind. The predictions
include the density variance, inner/dissipation scale, velocity
correlation length, mean magnetic field, and proton temperature. The
density turbulence amplitude is estimated in two ways. First, a simple
scaling technique is used to extend the theoretical predictions of the
PUI model for the high-latitude wind beyond the heliospheric termination
shock. Second, the solar wind and turbulence quantities are calculated
near the ecliptic plane using plasma and magnetometer data from the
Voyager 2 spacecraft over the period 1977-2018. Based on the turbulence
models and observations, we calculate the scattering angle of the radio
sources in the high-latitude and near-ecliptic wind. Finally, we compare
the numerical results with the analytic predictions from Cairns and
Armstrong et al. and the observed source sizes.</description>
</item>
<item>
<title> Plasma Emission versus Electron Cyclotron Maser Emission due to Power-law Energetic Electrons in Differently Magnetized Coronal Plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...928..115Z</link>
<description>By using self-consistent 2.5-dimensional particle-in-cell simulations,
we study the excitation efficiency of electromagnetic waves by power-law
energetic electrons with an anisotropic pitch-angle velocity
distribution, which can simultaneously trigger the Langmuir and electron
cyclotron maser instabilities, in differently magnetized coronal
plasmas. It is found that the (transverse) electromagnetic waves can be
excited much more efficiently in the case of strongly magnetized plasmas
with  &lt;SUB&gt;ce&lt;/SUB&gt; &gt;  &lt;SUB&gt;pe&lt;/SUB&gt; than that of weakly magnetized
plasmas with  &lt;SUB&gt;ce&lt;/SUB&gt; &lt;  &lt;SUB&gt;pe&lt;/SUB&gt;, where  &lt;SUB&gt;ce&lt;/SUB&gt;
and  &lt;SUB&gt;pe&lt;/SUB&gt; are the electron cyclotron frequency and the
electron plasma frequency, respectively. In particular, in a weakly
magnetized plasma the electromagnetic wave is hardly excited effectively
via the nonlinear coupling of Langmuir waves; although the Langmuir
waves can be generated by the power-law energetic electrons, implying
that the so-called plasma emission does not effectively work. These
results can be helpful for us to better understand the physical
mechanism of solar radio bursts.</description>
</item>
<item>
<title> a multi-wavelength analysis</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ap&amp;SS.367...40S</link>
<description>In this paper, we present the evolution and speed expansion of a shock
driven by a Coronal Mass Ejection (CME) that triggered a type II radio.
We combine radio analysis with a broad range of observations taken by
other ground-based and space borne observatories to track the evolution
of this CME/shock from Sun to 1 AU. The Halo CME studied here occurred
on 22 August 2015 at 07:12 UT with a linear speed of 547 km/s derived
from white-light observations obtained by the SoHO/LASCO spacecraft. The
CME and its associated flare (M1 Class at 06:39 UT) originated at active
region 12403 located at S14E09 on the visible solar disk. Type II radio
bursts drift with the shock propagation up from the solar surface and
produce emissions at the fundamental and higher harmonic frequencies
which can be seen in radio dynamic spectrograms. The speed of the shock
derived from radio observations was consistent with white-light
observations. We combined different models to estimate the evolution of
the ambient coronal magnetic field at lower corona. We present evidence
that this halo CME has been detected in interplanetary space near 1 AU
as a smooth rotation in the interplanetary magnetic field suggesting the
passage of a magnetic cloud but no shock detected in situ. We compared
the CME arrival time with the arrival time obtained from the Empirical
shock arrival model and drag-based model. We discuss the importance of
these findings.</description>
</item>
<item>
<title> A deep learning approach to solar radio flux forecasting</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AcAau.193..595S</link>
<description>The effect of atmospheric drag on spacecraft dynamics is considered one
of the predominant sources of uncertainty in Low Earth Orbit. These
effects are characterised in part by the atmospheric density, a quantity
highly correlated to space weather. Current atmosphere models typically
account for this through proxy indices such as the F10.7, but with
variations in solar radio flux forecasts leading to significant orbit
differences over just a few days, prediction of these quantities is a
limiting factor in the accurate estimation of future drag conditions,
and consequently orbital prediction. In this work, a novel deep residual
architecture for univariate time series forecasting, N-BEATS, is
employed for the prediction of the F10.7 solar proxy on the days-ahead
timescales relevant to space operations. This untailored, pure deep
learning approach has recently achieved state-of-the-art performance in
time series forecasting competitions, outperforming well-established
statistical, as well as statistical hybrid models, across a range of
domains. The approach was found to be effective in single point
forecasting up to 27-days ahead, and was additionally extended to
produce forecast uncertainty estimates using deep ensembles. These
forecasts were then compared to a persistence baseline and two
operationally available forecasts: one statistical (provided by BGS,
ESA), and one multi-flux neural network (by CLS, CNES). It was found
that the N-BEATS model systematically outperformed the baseline and
statistical approaches, and achieved an improved or similar performance
to the multi-flux neural network approach despite only learning from a
single variable.</description>
</item>
<item>
<title> The first ground-level enhancement of solar cycle 25 on 28 October 2021</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...660L...5P</link>
<description>&lt;BR /&gt; Aims: The first relativistic solar proton event of solar cycle 25
was detected on 28 October 2021 by neutron monitors (NMs) on the ground
and particle detectors on board spacecraft in near-Earth space. This is
the first ground-level enhancement (GLE) of the current cycle. A
detailed reconstruction of the NM response together with the
identification of the solar eruption that generated these particles is
investigated based on in situ and remote-sensing measurements. &lt;BR /&gt;
Methods: In situ proton observations from a few MeV to 500 MeV were
combined with the detection of a solar flare in soft X-rays, a coronal
mass ejection, radio bursts, and extreme ultraviolet (EUV) observations
to identify the solar origin of the GLE. Timing analysis was performed,
and a relation to the solar sources was outlined. &lt;BR /&gt; Results: GLE73
reached a maximum particle rigidity of 2.4 GV and is associated with
type III, type II, and type IV radio bursts and an EUV wave. A diversity
of time profiles recorded by NMs was observed. This points to the event
having an anisotropic nature. The peak flux at E &gt; 10 MeV was only 30
pfu and remained at this level for several days. The release time of 1
GV particles was found to be 15:40 UT. GLE73 had a moderately hard
rigidity spectrum at very high energies (  5.5). Comparison of GLE73
to previous GLEs with similar solar drivers is performed. &lt;P /&gt;Movies
are available at &lt;A href="https://www.aanda.org/10.1051/0004-6361/202142
855/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> Type III radio bursts and excitation of Langmuir waves by energetic electrons</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...660A..91M</link>
<description>Context. Solar activity occurs not only in terms of the well-known
11-year Sun spot cycle but also in terms of short-lived phenomena as
radio bursts. For instance, type III radio bursts are the most common
phenomenon of this activity in the Sun's radio radiation. In dynamic
radio spectra, they appear as short-lived stripes of enhanced radio
emission rapidly drifting from high to low frequencies. They are
regarded as the radio signature of beams of energetic electrons
travelling along magnetic field lines in the corona. The radio emission
is thought to be plasma emission, that is to say the radio emission
happens near the electron plasma frequency and/or its harmonics. Plasma
emission means, that energetic electrons excite Langmuir waves, which
convert into radio waves. &lt;BR /&gt; Aims: Initially, energetic electrons
are injected in a small region in the corona. Due to their spatio-
temporal evolution, they develop a beam-like velocity distribution
function (VDF), which is able to excite Langmuir waves. The aim of the
paper is to study the spatio-temporal behaviour of the generation of
Langmuir waves under coronal cirumstances and its effect on type III
radio bursts. &lt;BR /&gt; Methods: The generation of Langmuir waves is
treated by means of the Maxwell-Vlasov equations. The results are
discussed by employing plasma parameters usually found in the corona,
for instance at the 150 MHz level. &lt;BR /&gt; Results: The Langmuir waves
associated with the type III bursts are not generated by a monoenergetic
electron beam, but by a population of energetic electrons with a broad
velocity distribution. Hence, the Langmuir waves are produced by
different parts of the energetic electron population at different times
and positions. &lt;BR /&gt; Conclusions: In the case of type III bursts, the
velocities derived from their drift rates in dynamic radio spectra are
not the velocities of electrons, which generate the onset of the type
III burst at a given frequency. That can lead to an apparent accelerated
motion of the type III radio burst source.</description>
</item>
<item>
<title> Excitation of Langmuir waves at shocks and solar type II radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...660A..71M</link>
<description>Context. In the solar corona, shocks can be generated due to the
pressure pulse of a flare and/or driven by a rising coronal mass
ejection (CME). Coronal shock waves can be observed as solar type II
radio bursts in the Sun's radio radiation. In dynamic radio spectra,
they appear as stripes of an enhanced radio emission slowly drifting
from high to low frequencies. The radio emission is thought to be plasma
emission, that is to say the emission happens near the electron plasma
frequency and/or its harmonics. Plasma emission means that energetic
electrons excite Langmuir waves, which convert into radio waves via non-
linear plasma processes. Thus, energetic electrons are necessary for
plasma emission. In the case of type II radio bursts, the energetic
electrons are considered to be shock accelerated. &lt;BR /&gt; Aims: Shock
drift acceleration (SDA) is regarded as the mechanism for producing
energetic electrons in the foreshock region. SDA delivers a shifted
loss-cone velocity distribution function (VDF) for the energetic
electrons. The aim of the paper is to study in which way and under which
conditions a shifted loss-cone VDF of electrons excites Langmuir waves
in an efficient way in the corona. &lt;BR /&gt; Methods: By means of the
results of SDA, the shape of the resulted VDF was derived. It is a
shifted loss-cone VDF showing both a loss-cone and a beam-like
component. The growth rates for exciting Langmuir waves were calculated
in the framework of Maxwell-Vlasov equations. The results are discussed
by employing plasma and shock parameters usually found in the corona at
the 25 MHz level. &lt;BR /&gt; Results: We have found that moderate coronal
shocks with an Alfven-Mach number in the range 1.59 &lt; M&lt;SUB&gt;A&lt;/SUB&gt; &lt;
2.53 are able to accelerate electrons up to energies sufficient enough
to excite Langmur waves, which convert into radio waves seen as solar
type II radio bursts.</description>
</item>
<item>
<title> Dynamics and Characteristics of Waves in the Zebra Radio Source</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297...35Y</link>
<description>We analyzed the 17 August 1998 zebra event and showed that some quasi-
periodic oscillations modulate the zebra-stripe frequencies. We
determined the period of these oscillations as P&lt;SUB&gt;n&lt;/SUB&gt;=2.01 0.03
(in numbers of zebra stripes) and as P&lt;SUB&gt;f&lt;/SUB&gt;=11.8 0.17 MHz. In
the first part of the analyzed zebra, we found a stable density wave
that slowly propagated with the frequency drift less than 0.4 MHz
s&lt;SUP&gt;1&lt;/SUP&gt;. Then, a stationary density wave appeared followed by a
transformation of the waves to ones with longer periods. These long-
period waves were recorded before and after the time interval when no
zebra stripes were observed. We interpreted these density waves as
magnetosonic waves. We calculated their wavelength and propagating
velocity, considering two types of density models of the solar
atmosphere. We also estimated the characteristic density and magnetic-
field strength as N 9.2 10&lt;SUP&gt;8&lt;/SUP&gt; cm&lt;SUP&gt;1&lt;/SUP&gt; and B 0.73 G,
respectively. We found similar velocities derived from drifts of the
density wave and velocities calculated from the density and magnetic-
field strength considering gyro-harmonic numbers of zebra stripes.</description>
</item>
<item>
<title> A New Multichannel Parallel Real-time FFT Algorithm for a Solar Radio Observation System Based on FPGA</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PASP..134c4502Z</link>
<description>The real-time fast Fourier transform (FFT) is the essential algorithm
for signal processing in a solar radio receiver. However, field-
programmable gate array (FPGA) computation resources have become the
limitation of real-time processing of signals with increasing time and
spectral resolutions. It is necessary to design a real-time parallel FFT
algorithm with reduced resource occupation in the development of future
receiving systems. In this paper, we developed a multichannel parallel
FFT algorithm named the multichannel parallel real-time fast Fourier
transform (MPR-FFT), which can greatly reduce FPGA resource occupation
while increasing the real-time processing speed. In this algorithm, the
4L simultaneous N-point FFTs are first converted into L simultaneous
4N-point FFTs. Fusion processing is then performed to obtain the 4  L 
N-point spectrum. This method has been used in developing a solar radio
spectrometer, which works in the frequency range of 0.5-15 GHz in the
Chashan Observatory. In this spectrometer, 16 channel MPR-FFT with
8k-point data is realized in a Xilinx UltraScale KU115 FPGA. The MPR-FFT
algorithm reduced the computational resources to a large extent compared
to the Cooley-Tukey-based parallel FFT method; for instance, the Look-
Up-Table, Look-Up-Table RAM, Flip-Flop, and Digital Signal Process
slices were reduced by 37%, 50%, 17%, and 2.48%, respectively. Although
the MPR-FFT consumes 14 block RAM resources more than the Cooley-Tukey-
based parallel FFT, the MPR-FFT algorithm presents an overall reduction
in resource usage.</description>
</item>
<item>
<title> Subterahertz radius and limb brightening of the Sun derived from SST and ALMA</title>
<link>https://ui.adsabs.harvard.edu/abs/2022MNRAS.511..877M</link>
<description>Measurements of the radius and limb brightening of the Sun provide
important information about the solar atmosphere structure and
temperature. The solar radius increases as the observation at radio
frequency decreases, indicating that each emission originates higher in
the atmosphere. Thus, different layers of the solar atmosphere can be
probed by observing at multiple wavelengths. In this work, we determined
the average radius and limb brightening at 100, 212, 230, and 405 GHz,
using data from the Solar Submillimeter Telescope and Atacama Large
Millimeter/submillimeter Array's single-dish observations. For the first
time, limb brightening values for frequencies of 212 and 405 GHz were
estimated. At sub-THz frequencies, the observed limb brightening may
affect the solar radius measurements. We use two different and well-
known approaches to determine the radius: The half-power method and the
inflection-point method. We investigate how the antenna beam size and
the limb brightening level, LB, can affect the radius measurements using
both methods. Our results showed that the inflection-point method is the
least affected by these parameters, and should thus be used for solar
radius estimates at radio wavelengths. The measured average radii are
968  3 arcsec (100 GHz), 963  3 arcsec (212 GHz), 963  2 arcsec (230
GHz), and 963  5 arcsec (405 GHz). Finally, we used forward modelling
to estimate the ranges of LB of the solar disc resulting in 5-19 per
cent (100 GHz), 2-12 per cent (212 GHz), 6-18 per cent (230 GHz), and
3-17 per cent (405 GHz). Both radius and limb brightening estimates
agree with previous measurements reported in the literature.</description>
</item>
<item>
<title> Solar Energetic Particles Produced during Two Fast Coronal Mass Ejections</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...928L...6L</link>
<description>Two recent extremely fast coronal mass ejections (CMEs) are of
particular interest. The first one originated from the southern
hemisphere on 2021 October 28 and caused strong solar energetic particle
(SEP) events over a wide longitude range from Earth, STEREO-A, to Mars.
However, the other one, originating from the center of the Earth-viewed
solar disk 5 days later, left weak SEP signatures in the heliosphere.
Based on the white-light images of the CMEs from the Solar and
Heliospheric Observatory (SOHO) and the Ahead Solar Terrestrial
Relations Observatory (STEREO-A), in combination with the observations
of the corresponding solar flares, radio bursts, and in situ magnetic
fields and particles, we try to analyze the series of solar eruptions
during October 28-November 2 as well as their correspondences with the
in situ features. It is found that the difference in SEP features
between the two CMEs is mainly due to (1) the seed particles probably
supplied by associated flares and (2) the magnetic connection influenced
by the preceding solar wind speed.</description>
</item>
<item>
<title> Eruption of the EUV Hot Channel from the Solar Limb and Associated Moving Type IV Radio Burst</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...927..108V</link>
<description>Using the observations from the Solar Dynamics Observatory, we study an
eruption of a hot-channel flux rope (FR) near the solar limb on 2015
February 9. The pre-eruptive structure is visible mainly in EUV 131 
images, with two highly sheared loop structures. They undergo a slow
rising motion and then reconnect to form an eruptive hot channel, as in
the tether-cutting reconnection model. The J-shaped flare ribbons trace
the footpoint of the FR that is identified as the hot channel.
Initially, the hot channel is observed to rise slowly at 40 km
s&lt;SUP&gt;-1&lt;/SUP&gt;, followed by an exponential rise from 22:55 UT at a
coronal height of 87  2 Mm. Following the onset of the eruption at
23:00 UT, the flare reconnection then adds to the acceleration process
of the coronal mass ejection (CME) within 3 R &lt;SUB&gt;&lt;/SUB&gt;. Later on,
the CME continues to accelerate at 8 m s&lt;SUP&gt;-2&lt;/SUP&gt; during its
propagation period. Further, the eruption also launched type II radio
bursts, which were followed by type III and type IVm radio bursts. The
start and end times of the type IVm burst correspond to the CME's core
height of 1.5 and 6.1 R &lt;SUB&gt;&lt;/SUB&gt;, respectively. Also, the spectral
index is negative, suggesting that nonthermal electrons are trapped in
the closed loop structure. Accompanied by this type IVm burst, this
event is unique in the sense that the flare ribbons are very clearly
observed together with the erupting hot channel, which strongly suggests
that the hooked parts of the J-shaped flare ribbons outline the boundary
of the erupting FR.</description>
</item>
<item>
<title> Langmuir-Slow Extraordinary Mode Magnetic Signature Observations with Parker Solar Probe</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...927...95L</link>
<description>Radio emission from interplanetary shocks, planetary foreshocks, and
some solar flares occurs in the so-called "plasma emission" framework.
The generally accepted scenario begins with electrostatic Langmuir waves
that are driven by a suprathermal electron beam on the Landau resonance.
These Langmuir waves then mode-convert to freely propagating
electromagnetic emissions at the local plasma frequency f &lt;SUB&gt; pe
&lt;/SUB&gt; and/or its harmonic 2f &lt;SUB&gt; pe &lt;/SUB&gt;. However, the details of
the physics of mode conversion are unclear, and so far the magnetic
component of the plasma waves has not been definitively measured.
Several spacecraft have measured quasi-monochromatic Langmuir or slow
extraordinary modes (sometimes called z-modes) in the solar wind. These
coherent waves are expected to have a weak magnetic component, which has
never been observed in an unambiguous way. Here we report on the direct
measurement of the magnetic signature of these waves using the Search
Coil Magnetometer sensor of the Parker Solar Probe/FIELDS instrument.
Using simulations of wave propagation in an inhomogeneous plasma, we
show that the appearance of the magnetic component of the slow
extraordinary mode is highly influenced by the presence of density
inhomogeneities that occasionally cause the refractive index to drop to
low values where the wave has strong electromagnetic properties.</description>
</item>
<item>
<title> Robust Absolute Solar Flux Density Calibration for the Murchison Widefield Array</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...927...17K</link>
<description>Sensitive radio instruments are optimized for observing faint
astronomical sources, and usually need to attenuate the received signal
when observing the Sun. There are only a handful of flux density
calibrators that can comfortably be observed with the same attenuation
setup as the Sun. Additionally, for wide field-of-view (FoV) instruments
like the Murchison Widefield Array (MWA) calibrator observations are
generally done when the Sun is below the horizon, to avoid the
contamination from solar emissions. These considerations imply that the
usual radio interferometric approach to flux density calibration is not
applicable for solar imaging. A novel technique, relying on a good sky
model and detailed characterization of the MWA hardware, was developed
for solar flux density calibration for MWA. Though successful, this
technique is not general enough to be extended to the data from the
extended configuration of the MWA Phase II. Here, we present a robust
flux density calibration method for solar observations with MWA
independent of the array configuration. We use different approaches-the
serendipitous presence of strong sources; detection of numerous
background sources using high dynamic range images in the FoV along with
the Sun; and observations of strong flux density calibrators with and
without the additional attenuation used for solar observations-to obtain
the flux scaling parameters required for the flux density calibration.
Using the present method, we have achieved an absolute flux density
uncertainty ~10% for solar observations even in the absence of dedicated
calibrator observations.</description>
</item>
<item>
<title> Trieste CALLISTO station setup and observations of solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AdSpR..69.2589M</link>
<description>Not Available</description>
</item>
<item>
<title> High-resolution observations with ARTEMIS/JLS and the NRH. IV. Imaging spectroscopy of spike-like structures near the front of type-II bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...659A.198A</link>
<description>Context. Narrowband bursts (spikes) are very small duration and
bandwidth bursts which appear on dynamic spectra from microwave to
decametric frequencies. They are believed to be manifestations of small-
scale energy release through magnetic reconnection. &lt;BR /&gt; Aims: We
study the position of the spike-like structures relative to the front of
type-II bursts and their role in the burst emission. &lt;BR /&gt; Methods: We
used high-sensitivity, low-noise dynamic spectra obtained with the
acousto-optic analyzer (SAO) of the ARTEMIS-JLS solar radiospectrograph,
in conjunction with high-time-resolution images from the Nanay
Radioheliograph (NRH) in order to study spike-like bursts near the front
of a type-II radio burst recorded at the west limb during the November
3, 2003 extreme solar event. The spike-like emission in the dynamic
spectrum was enhanced by means of high-pass-time filtering. &lt;BR /&gt;
Results: We identified a number of spikes in the NRH images. Due to the
lower temporal resolution of the NRH, multiple spikes detected in the
dynamic spectrum appeared as single structures in the images. These
spikes had an average size of 200 and their observed brightness
temperature was 1.4 to 5.6  10&lt;SUP&gt;9&lt;/SUP&gt; K, providing a significant
contribution to the emission of the type-II burst front. At variance
with a previous study on the type-IV associated spikes, we found no
systematic displacement between the spike emission and the emission
between spikes. At 327.0 MHz, the type II emission was located about 0.3
R&lt;SUB&gt;&lt;/SUB&gt; above the pre-existing continuum emission, which, in turn,
was located 0.1 R&lt;SUB&gt;&lt;/SUB&gt; above the western limb. &lt;BR /&gt;
Conclusions: This study, combined with our previous results, indicates
that the spike-like chains aligned along the type II burst MHD shock
front are not a perturbation of the type II emission, as in the case of
type IV spikes, but a manifestation of the type II emission itself. The
preponderance of these chains, together with the lack of isolated
structures or irregular clusters, points towards some form of small-
scale magnetic reconnection, organized along the type-II propagating
front. &lt;P /&gt;This work is dedicated to the memory of Costas Caroubalos
(1928-2021), founder of the ARTEMIS radiospectrograh.</description>
</item>
<item>
<title> Non-thermal electron velocity distribution functions due to 3D kinetic magnetic reconnection for solar coronal plasma conditions</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PhPl...29b2104Y</link>
<description>Magnetic reconnection can convert magnetic energy into kinetic energy of
non-thermal electron beams. Those accelerated electrons can, in turn,
cause radio emission in astrophysical plasma environments, such as solar
flares via micro-instabilities. The properties of the electron velocity
distribution functions (EVDFs) of those non-thermal beams generated by
reconnection are, however, still not well understood, in particular,
properties that are necessary conditions for some relevant micro-
instabilities. We aim at characterizing the EVDFs generated in 3D
magnetic reconnection by means of fully kinetic particle-in-cell code
simulations. In particular, our goal is to identify the possible sources
of free energy offered by the generated EVDFs and their dependence on
the strength of the guide field. By applying a machine learning
algorithm on the EVDFs, we find that (1) electron beams with positive
gradients in their 1D parallel (to the local magnetic field direction)
velocity distribution functions are generated in both diffusion region
and separatrices. (2) Electron beams with positive gradients in their
perpendicular (to the local magnetic field direction) velocity
distribution functions are observed in the diffusion region and outflow
region near the reconnection midplane. In particular, perpendicular
crescent-shaped EVDFs (in the perpendicular velocity space) are mainly
observed in the diffusion region. (3) As the guide field strength
increases, the number of locations with EVDFs featuring a perpendicular
source of free energy significantly decreases. The formation of non-
thermal electron beams in the field-aligned direction is mainly due to
magnetized and adiabatic electrons, while in the direction perpendicular
to the local magnetic field, it is attributed to unmagnetized electrons.</description>
</item>
<item>
<title> Comparing results of real-scale time MHD modeling with observational data for first flare M 1.9 in AR 10365</title>
<link>https://ui.adsabs.harvard.edu/abs/2022OAst...31...58B</link>
<description>As shown in the first results of MHD simulations in the real scale of
time, above the active region (AR) 10365, during the first flare M 1.9
(05/26/2003 05:34) at a height of 16-18 mm (lower corona), a singular
line of magnetic field appears. The local maximum of the current density
is situated on this singular line. The magnetic field in the vicinity of
this singular line is the superposition of an X-type magnetic
configuration and a divergent magnetic field. The accumulation of
magnetic energy for solar flare with current sheet creation takes place
near this singular line due to magnetic field deformation by
disturbances in the X-type configuration in spite of the presence of
overlaid diverging magnetic configuration. The magnetic configuration is
so complicated that the singular line can be found only by using
specially developed graphical system of search. The position of singular
line coincides with position of source of flare radio emission at the
frequency 17 GHz above AR 10365 measured by Nobeyama Radioheliograph
(NoRH). Also, MHD simulation shows appearance of the singular line, in
the vicinity of which X-type configuration dominates. However,
apparently due to small disturbance, propagating from the photosphere,
sufficient magnetic energy was not accumulated in this configuration, so
the NoRH does not show the flare source of emission at the frequency 17
GHz in the place, where this singular line is situated.</description>
</item>
<item>
<title> Solar Microwave Emission Associated with Coronal Mass Ejections (CME)</title>
<link>https://ui.adsabs.harvard.edu/abs/2022LatJP..59a..13K</link>
<description>The connection between Coronal Mass Ejections (CME) and radio burst has
been discovered especially at lower frequencies (&lt; 2 GHz). The aim of
the study is to investigate possible connection between CMEs and
variability of radio brightenings at 37 GHz (8 mm) within the time frame
of four days. The millimetre radio observations have been made on RT-14
radio telescope at Metshovi Radio Observatory of Aalto University,
Finland. In addition, 11.2 GHz (2.7 cm) total solar flux information is
included in the analysis. The radio observations were made between March
2011 and September 2017, totally including 24 events. The results
demonstrate that in most of the cases the radio brightening intensity
achieves its maximum before CME occurs. Time of 11.2 GHz intensity
appearance matches with time of CME appearance with difference of two to
three hours. However, in most cases a maximum of 11.2 GHz intensity
appears before CMEs. The study investigates a possibility of predicting
CME appearance based on milli- and centimetre radio observations. The
study also proposes a scenario connection between CMEs and solar
microwave events.</description>
</item>
<item>
<title> Dependence of D-Region Perturbations of the Midlatitude Ionosphere on the Spectral Composition of the X-Ray Radiation of Solar Flares According to Experimental Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62...98G</link>
<description>An experimental study was made of the dependence of the electron-density
perturbations in the Dregions of the midlatitude ionosphere during
solar flares on the spectral composition of X-ray radiation in the
wavelength range from 0.01 to 0.4 nm, i.e., outside the measurement
range of the GOES satellite. For this, the variation in the brightness
temperature of the emission of six flares in 20142017 were calculated,
and the composition of their radiation was determined. It is shown that,
although only a small percent of the total flash radiation energy is in
the 0.010.2 nm wavelength range, it is the hard components that are the
main factor leading to a change in the reflection height of very low
frequency (VLF) radio waves. It is shown that the efficiency of solar
flares significantly depends on the previous solar activity, not only
for class-C flares but also for powerful class-M and -X flares.</description>
</item>
<item>
<title> Solar-Activity Index for the E-Layer Critical Frequency at Middle Latitudes</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62...66D</link>
<description>Based on an analysis of data from the midlatitude ionospheric stations,
it is found that the P = 0.5(F&lt;SUB&gt;1&lt;/SUB&gt; + F&lt;SUB&gt;81&lt;/SUB&gt;) index is an
optimal solar-activity index for the daily values of the E-layer
critical frequency foE, where F&lt;SUB&gt;1&lt;/SUB&gt; and F&lt;SUB&gt;81&lt;/SUB&gt; are the
solar radio-emission flux at a wavelength of 10.7 cm on the given day
and the value of this flux averaged over 81 days, respectively. The
standard deviations  of the foE dependence on P in the daytime hours
are almost equal for winter and summer at a latitude of approximately
50 N. The  value is maximal at lower latitudes for summer and at
higher latitudes for winter. The introduction of the P index into the
Institute of Applied Geophysics (IPG), international reference
ionosphere (IRI), or NeQuick models makes it possible to use these
models to calculate the daily foE values. Based on a preliminary
analysis (noon, moderate solar activity), it is found that the accuracy
of the foE calculation with these models is nearly the same. The
strongest difference between the models is observed for summer; at
latitudes of 5060 N, the IPG and NeQuick models are more accurate
than the IRI model. The IRI model could be preferable for lower
latitudes.</description>
</item>
<item>
<title> Features of the Behavior of Time Parameters of Forbush Decreases Associated with Different Types of Solar and Interplanetary Sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Ge&amp;Ae..62...17M</link>
<description>Forbush decreases occurring from 1997 to 2017 (1055 events in total)
have been analyzed with the use of a database of Forbush effects and
interplanetary disturbances built and currently maintained by the
Pushkov Institute of Terrestrial Magnetism, Ionosphere, and Radio Wave
Propagation of the Russian Academy of Sciences (IZMIRAN). Based on
statistical methods, we compared the temporal evolution of Forbush
decreases in events of four types: (1) those associated with coronal
mass ejections from active regions and accompanied by solar flares; (2)
those induced by interplanetary disturbances due to filament eruptions
from areas beyond active regions; (3) those caused by high-speed streams
from coronal holes; and (4) those associated with two or more sources of
different types of disturbances. In the comparison, we used the
following time parameters of the development of Forbush decreases: the
time intervals from the event onset to the detection of the minimal
density of cosmic rays, the maximal hourly decrease in the density of
cosmic rays, the maximal equatorial anisotropy of cosmic rays, the
maximal speed of the solar wind, the maximal strength of the
interplanetary magnetic field, and the minimal Dst index. Analysis of
the distributions of the time parameters and their intercorrelation has
shown that there are substantial differences between the evolution
scenarios of Forbush decreases in the four sets of examined events.</description>
</item>
<item>
<title> A Broadband Solar Radio Dynamic Spectrometer Working in the Millimeter-wave Band</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJS..258...25S</link>
<description>Most solar radio telescopes operate below ~18 GHz and cannot realize a
complete frequency coverage of the microwave spectrum, especially in the
optically thin regime during solar bursts, which can provide unique
information about the magnetic field in the burst area in the solar
corona. Therefore, the development of high-frequency microwave
observation equipment is demanded by the solar radio community. In this
paper, we present a microwave spectrum observation system operating at
35-40 GHz. In this system, the solar radio signal is acquired by an 80
cm Cassegrain circularly polarized antenna, which is then downconverted
and channelized by a 35-40 GHz analog front end. The processed signal is
finally sent to the digital receiver to generate the microwave dynamic
spectrum, which is transmitted by gigabit Ethernet transmission to a
host computer. The system performance has been tested and obtained as
follows: a noise figure of ~300 K, system linearity of &gt;0.9999, time
resolution of about 134 ms (default), and frequency resolution of 153
kHz. We further conduct calibration for this system and find that the
observed Sun-Moon ratio is about 43.1-53.3 @ 35.25 GHz during the new
Moon, and is quite close to the theoretical value. The coefficient of
variation of the system is ~0.61% in a 9 hr test. The system has been
designed, developed, and tested for over 1 yr in Chashan Solar
Observatory and is expected to play an important role in the microwave
burst study in the 25th solar cycle.</description>
</item>
<item>
<title> Simultaneous Observations of Chromospheric Evaporation and Condensation during a C-class Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...926...23L</link>
<description>We explored simultaneous observations of chromospheric evaporation and
condensation during the impulsive phase of a C6.7 flare on 2019 May 9.
The solar flare was simultaneously observed by multiple instruments,
i.e., the New Vacuum Solar Telescope (NVST), the Interface Region
Imaging Spectrograph, the Atmospheric Imaging Assembly (AIA), Fermi, the
Mingantu Spectral Radioheliograph, and the Nobeyama Radio Polarimeters.
Using the single Gaussian fitting and the moment analysis technique,
redshifted velocities at slow speeds of 15-19 km s&lt;SUP&gt;-1&lt;/SUP&gt; are
found in the cool lines of C II and Si IV at one flare footpoint
location. Redshifts are also seen in the H line-of-sight velocity image
measured by NVST at double footpoints. Those redshifts with slow speeds
can be regarded as the low-velocity downflows driven by the
chromospheric condensation. Meanwhile, the converging motions from
double footpoints to the loop top are found in the high-temperature EUV
images, such as AIA 131, 94, and 335 . Their apparent speeds are
estimated to be roughly 126-210 km s&lt;SUP&gt;-1&lt;/SUP&gt;, which could be
regarded as the high-velocity upflows caused by the chromospheric
evaporation. The nonthermal energy flux is estimated to be about 5.7 
10&lt;SUP&gt;10&lt;/SUP&gt; erg s&lt;SUP&gt;-1&lt;/SUP&gt; cm&lt;SUP&gt;-2&lt;/SUP&gt;. The characteristic
timescale is roughly equal to 1 minute. All these observational results
suggest an explosive chromospheric evaporation during the flare
impulsive phase. While a hard X-ray/microwave pulse and a type III radio
burst are found simultaneously, indicating that the explosive
chromospheric evaporation is driven by the nonthermal electron.</description>
</item>
<item>
<title> Sizes and Shapes of Sources in Solar Metric Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...925..140G</link>
<description>Metric and decametric radio emissions from the Sun are the only direct
source of information about the dynamics of nonthermal electrons in the
upper corona. In addition, the combination of spectral and imaging
(sizes, shapes, and positions) observations of low-frequency radio
sources can be used as a unique diagnostic tool to probe plasma
turbulence in the solar corona and inner heliosphere. The geometry of
the low-frequency sources and its variation with frequency are still not
understood, primarily due to the relatively low spatial resolution
available for solar observations. Here we report the first detailed
multifrequency analysis of the sizes of solar radio sources observed by
the Low Frequency Array. Furthermore, we investigate the source shapes
by approximating the derived intensity distributions using 2D Gaussian
profiles with elliptical half-maximum contours. These measurements have
been made possible by a novel empirical method for evaluating the
instrumental and ionospheric effects on radio maps based on known source
observations. The obtained deconvolved sizes of the sources are found to
be smaller than previous estimations, and often show higher ellipticity.
The sizes and ellipticities of the sources inferred using 2D Gaussian
approximation, and their variation with frequency are consistent with
models of anisotropic radio-wave scattering in the solar corona.</description>
</item>
<item>
<title> Properties and Space Weather Relevance</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....8...39M</link>
<description>A comprehensive statistical analysis on the properties and accompanied
phenomena of all M-class solar flares (as measured in soft X-rays) in
the last two solar cycles (19962019) is presented here with a focus on
their space weather potential. The information about the parent active
region and the underlying sunspot (Hale) type is collected for each
case, where possible, in order to identify photospheric precondition as
precursors for the solar flare eruption or confinement. Associations
with coronal mass ejections, solar energetic particles, and
interplanetary radio emissions are also evaluated and discussed as
possible proxies for flare eruption and subsequent space weather
relevance. The results show that the majority (80%) of the analyzed
M-class flares are of , -, and -- magnetic field configuration.
The M-class population of flares is accompanied by CMEs in 41% of the
cases and about half of the flare sample has been associated with radio
emission from electron beams. A much lower association (10%) is
obtained with shock wave radio signatures and energetic particles.
Furthermore, a parametric scheme is proposed in terms of occurrence
rates between M-class flares and a variety of accompanied solar
phenomena as a function of flare sub-classes or magnetic type. This
study confirms the well-known reduced but inevitable space weather
importance of M-class flares.</description>
</item>
<item>
<title> Predicting the Daily 10.7-cm Solar Radio Flux Using the Long Short-Term Memory Method</title>
<link>https://ui.adsabs.harvard.edu/abs/2022Univ....8...30Z</link>
<description>As an important index of solar activity, the 10.7-cm solar radio flux
(F&lt;SUB&gt;10.7&lt;/SUB&gt;) can indicate changes in the solar EUV radiation,
which plays an important role in the relationship between the Sun and
the Earth. Therefore, it is valuable to study and forecast
F&lt;SUB&gt;10.7&lt;/SUB&gt;. In this study, the long short-term memory (LSTM)
method in machine learning is used to predict the daily value of
F&lt;SUB&gt;10.7&lt;/SUB&gt;. The F&lt;SUB&gt;10.7&lt;/SUB&gt; series from 1947 to 2019 are
used. Among them, the data during 19471995 are adopted as the training
dataset, and the data during 19962019 (solar cycles 23 and 24) are
adopted as the test dataset. The fourfold cross validation method is
used to group the training set for multiple validations. We find that
the root mean square error (RMSE) of the prediction results is only
6.20~6.35 sfu, and the correlation coefficient (R) is as high as
0.9883~0.9889. The overall prediction accuracy of the LSTM method is
equivalent to those of the widely used autoregressive (AR) and
backpropagation neural network (BP) models. Especially for 2-day and
3-day forecasts, the LSTM model is slightly better. All this
demonstrates the potentiality of the LSTM method in the real-time
forecasting of F&lt;SUB&gt;10.7&lt;/SUB&gt; in future.</description>
</item>
<item>
<title> NenuFAR Performance for Solar Radio Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022URSL....4...17B</link>
<description>Not Available</description>
</item>
<item>
<title> First Solar Radio Burst Observations by the Mexican Array Radio Telescope (MEXART) at 140 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297....9H</link>
<description>The National Laboratory of Space Weather in Mexico (Laboratorio Nacional
de Clima Espacial: LANCE) coordinates instrumentation for monitoring the
space-weather impact over Mexico. Two of these instruments are the
Mexican Array Radio Telescope (MEXART) and Compound Astronomical Low
frequency Low cost Instrument for Spectroscopy and Transportable
Observatory (CALLISTO) station of the e-CALLISTO network (CALLMEX). Both
instruments are located at the same facility (Coeneo Michoacan, Mexico)
and share a spectral band centered at 140 MHz. In this work, we show the
capabilities of the e-CALLISTO network as support to identify a solar
radio burst in the signal of the MEXART radiotelescope. We identified 75
solar radio bursts in the MEXART signal: five events of Type II and 70
of Type III between September 2015 and May 2019. The analysis of solar
radio bursts in the MEXART signal provides us valuable information about
the development of the radio event due to their high sensitivity, time
resolution, and isotropic response. In the case of Type-III solar radio
events, we identify four characteristic phases in the dynamical
evolution of the signal at 140 MHz: a pre-phase, a main peak, a decay
phase, and a post-event phase. A Morlet wave transform was done of
MEXART signals in the Type-III solar radio busts; in their spectra, a
pine tree structure was identified preceding the main event in the time
series. These characteristics are not observable in the data from the
e-CALLISTO network.</description>
</item>
<item>
<title> Detections of Multi-Periodic Oscillations During a Circular Ribbon Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022SoPh..297....2N</link>
<description>We present the analysis of three kinds of oscillating behavior using
multi-wavelength observations of the 10 November 2013
(SOL2013-11-10T05:14) circular-ribbon flare. This event is a typical
circular-ribbon flare with an outer spine structure and homologous jets.
We found three kinds of oscillations (or perturbations): i) flux
oscillation (or QPP) with a dominant period of about 20 seconds in
X-ray, EUV, and microwave emissions, ii) periodic jets with an
intermittent cadence of around 72 seconds, iii) an outer loop perturbing
half a cycle with a duration of about 168 seconds. Similar to the
periodic jets that could be produced by a nonthermal process, like
repeated magnetic reconnection, the flare QPP detected in the thermal
emissions could have the same origin as the oscillation seen in the
nonthermal emissions. The outer-loop perturbation is possibly triggered
by a blast wave driven by the circular-ribbon flare, or it might be
modulated by the sausage wave or the slow magnetoacoustic wave. The
results obtained provide data for further numerical studies on the
physical origin of the flare oscillations.</description>
</item>
<item>
<title> Solar Eclipse Observations with Small Radio Telescope in Hong Kong in the 21 CM Radio Frequency Band</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RoAJ...32...35L</link>
<description>Small radio telescope of 21 cm was used for studying the partial solar
eclipse, with magnitude 0.89, in Hong Kong on 21st June, 2020. The radio
telescope SPIDER 300A was designed and constructed by the Radio2Space
Company, Italy. Radio flux density time curves (light curve) and a two-
dimension mapping of the eclipse are presented in this paper. Standard
radio data reduction methods were used to obtain the intensity time
curve. We also adopted the semi-pipeline method for the reduction of
data to obtain the same results as with the built-in software of the
radio telescope SPIDER 300A. The total solar radio flux of the eclipse
was found to reduce by maximum 555%, while the maximum eclipsed area of
the same eclipse is 86.08%. Other radio observations of solar eclipses
in Hong Kong are also discussed in this paper, including SPIDER 300A
observation of partial solar eclipse on 26th December 2019 (APPENDIX A);
and small radio telescope (SRT), developed by the Haystack Observatory,
MIT, USA, observation of 2020 eclipse (APPENDIX B).</description>
</item>
<item>
<title> The Critical Frequency of the Ionospheric F2-LAYER as Obtained from Ionosonde Data and Observations of Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2022RPRA...27..203S</link>
<description>Subject and Purpose. Studying the time variations shown by the critical
frequencies of the ionospheric F2 layer through comparative analysis of
ionosonde data and observations of type III solar radio bursts. Methods
and Methodology. In this work, two independent methods have been used
for identifying critical frequencies in the ionosphere, namely that of
vertical sounding and observations of type III solar radio bursts near
their cut-off frequency in the ionosphere. One of the ionosondes used
for vertical sounding was located near Zmiiv (Kharkiv Region), rather
close to the UTR-2 radio astronomy observatory where the solar bursts
were observed. The radiation from such bursts represented probe signals
for transmissive sounding. The solar radiation was received with an
element of a low-frequency (1 to 40 MHz) antenna array. Results. On May
22, 2021 variations in the critical frequency f0F2 of the ionospheric
F2-layer were followed between 07:00 and 17:00 UT. The value reached a
maximum of 5.9 MHz at 07:45 to 08:00 UT and then decreased smoothlyto
4.9 MHz, staying there from 15:30 till 16:45 UT. At that time, a storm
of type III solar bursts was recorded with the antenna for radio
observations at 140 MHz, revealing a cut-off effect for the bursts. As
has been found,their cut-off frequency can be used for estimating the
critical frequency f0F2 in the ionosphere. Conclusions. The comparative
analysis of solar burst observations and frequency-and-time measurements
with an ionosonde has shown possibilities for evaluating the critical
frequency f0F2 in the ionosphere from the data on the cut-off frequency
for solar radio-frequ</description>
</item>
<item>
<title> Dispersion and damping rate of Langmuir wave in space plasma with regularized Kappa distributed electrons</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PlST...24a5301L</link>
<description>The dispersion of Langmuir wave (LW) in an unmagnetized collisionless
plasma with regularized Kappa distributed electrons is investigated from
the kinetic theory. The frequency and damping rate of LW are analyzed
for the parameters relating to the source region of a type III solar
radio burst. It is found that the linear behavior of LW is greatly
modified by the suprathermal index  and the exponential cutoff
parameter . In the region  &lt; 1.5, the damping rate of LW will be much
larger than the one with Maxwellian distributed electrons. Hence, the
nonlinear process of LW in low  region may exhibit different properties
in comparison with the one in large  region.</description>
</item>
<item>
<title> Observations and Modeling of NOAA AR 12470</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PhDT........10C</link>
<description>Waves and oscillations are important solar phenomena not only because
they can propagate and dissipate energy in the chromosphere, but also
because they carry information about the structure of the atmosphere in
which they propagate. Among these phenomena, the one of the most
interesting ones occurs in the sunspot umbra. In this area, continuously
propagating magnetohydrodynamic (MHD) waves generated from below the
photosphere create the famous 3-minute sunspot umbral oscillations that
affect the line profile of spectral lines due to temperature, density,
and velocity changes of the plasma in the region. In the past decades,
numerous observations and models have been carried out about the nature
of the 3-minute oscillation and its relation with the coronal heating
problem, but the lack of direct observations of the temperature
variation in the chromosphere has made it hard to answer these
questions.The need for a better understanding of the fine structure of
the 3-minute oscillation and its time evolution in sunspots has
intensified with the development of better observing tools. Among modern
observatories, the Atacama Large Millimeter/submillimeter Array (ALMA)
opens up a new era of solar radio observation due to its high spatial
and temporal resolution and image quality. When combined with other
cutting-edge instruments, such as the Goode Solar Telescope (GST) at the
Big Bear Solar Observatory (BBSO), the Atmospheric Imaging Assembly
(AIA) on board the Solar Dynamics Observatory, and Interface Region
Imaging Spectrograph (IRIS), ALMA can provide unique electron
temperature diagnostics that clarify the behavior of the solar
chromosphere's response to propagating waves.In this dissertation, a
study is carried out about sunspot oscillations and wave propagation in
NOAA active region 12470 using an approximately 1 hr long dataset
acquired on 2015 December 17 by the instruments listed above. The
discovery of 3-minute sunspot oscillations seen in the mm-wave band is
reported for the first time. The 2 s cadence of ALMA images makes it
possible to well resolve the typical 3-minute period sunspot oscillation
in the chromosphere. Fourier analysis is applied to the ALMA band 3 and
GST H data sets to obtain the power spectra as well as phase
information of the oscillations. The properties of the wave propagation
are analyzed by combining multiple wavelengths that probe physical
parameters of the solar atmosphere at different heights.The
chromospheric radiation is synthesized in 1-D using a radiation transfer
code which uses the Solar Irradiance Physical Modeling (SRPM) as an
input. A good correlation of the phase relationship between the observed
and modeled oscillations of H and temperature fluctuations has been
found and it is consistent with the result from a possible physical
model for impulse-driven acoustic waves propagating in the
gravitationally stratified medium. An asymmetry in the time profile of
the temperature fluctuations discovered in the ALMA data is found to
require a nonlinear wave solution, which is applied to several
atmospheric models in an attempt to match the asymmetry and the absolute
brightness temperature of the simulations to the observations. The
asymmetry is successfully reproduced using the nonlinear wave scenario,
although the absolute brightness of the simulated atmosphere remains
lower than observed. These results demonstrate the capability of ALMA mm
observations to provide new insight into what is needed for improving
such atmospheric models in the future.</description>
</item>
<item>
<title> A deep learning method for the recognition of solar radio burst spectrum</title>
<link>https://ui.adsabs.harvard.edu/abs/2022PeerJ...8..855G</link>
<description>Not Available</description>
</item>
<item>
<title> A Transient-Motion-Powered Motion Detector</title>
<link>https://ui.adsabs.harvard.edu/abs/2022IITJ....9.3372L</link>
<description>The emerging energy harvesting technology facilitates the development of
ubiquitous and everlasting battery-free motion detectors. This article
introduces a robust design of the transient-motion-powered motion
detector, which is called ViPSN-pluck. "ViPSN" is the acronym for the
vibration-powered sensing node while "pluck" stands for the plucking-
motion energy harvester. By using a piezo-magneto-elastic structure,
ViPSN-pluck can efficiently harvest energy from a transient motion. By
properly making good use of this tiny harvested energy, ViPSN-pluck can
effectively carry out motion detection and Bluetooth low-energy (BLE)
wireless communication. Given the concurrency of mechanical potential
energy precharging and motion detection, the transient-motion plucking
energy harvester used in ViPSN-pluck has the merit of high energy
reliability. This unique feature is unprecedented in the solar and
radio-frequency (RF) energy harvesting cases, which might suffer from
energy outages under fluctuating irradiance or RF signal strength,
respectively. The working principle of ViPSN-pluck, in particular, the
dynamic characteristics of the plucking energy harvester and the energy
matching between generation and utilization, are discussed in detail to
demonstrate the robustness in operation. The cyber-electromechanical
synergy among the mechanical dynamics, power conditioning circuit, and
low-power embedded system is highlighted. The design methodology of
ViPSN-pluck provides a valuable reference for the developments of future
motion-powered Internet of Things devices.</description>
</item>
<item>
<title> Demonstrating the capabilities of CubeSats to monitor essential climate variables of the water cycle [Instruments and Missions]</title>
<link>https://ui.adsabs.harvard.edu/abs/2022IGRSM..10d.260C</link>
<description>The Federated Satellite Systems/&lt;SUP&gt;3&lt;/SUP&gt;Cat-5 (FSSCat) mission was
the winner of the European Space Agency (ESA) Sentinel Small Satellite
(S&lt;SUP&gt;3&lt;/SUP&gt;) Challenge and overall winner of the 2017 Copernicus
Masters competition. It consisted of two six-unit CubeSats. The Earth
observation payloads were 1) the Flexible Microwave Payload 2 (FMPL-2)
onboard &lt;SUP&gt;3&lt;/SUP&gt;Cat-5/A, an L-band microwave radiometer and GNSS
reflectometer (GNSS-R) implemented using a software-defined radio (SDR),
and 2) the HyperScout-2 onboard &lt;SUP&gt;3&lt;/SUP&gt;Cat-5/B, a hyperspectral
camera, with the first experiment using artificial intelligence to
discard cloudy images. FSSCat was launched on 3 September 2020 and
injected into a 535-km synchronous orbit. &lt;SUP&gt;3&lt;/SUP&gt;Cat-5/A was
operated for three months until the payload was probably damaged by a
solar flare and coronal mass ejection. During this time, all scientific
requirements were met, including the generation of coarse-resolution and
downscaled soil moisture (SM) maps, sea ice extent (SIE) maps,
concentration and thickness maps, and even wind speed (WS) and sea
surface salinity (SSS) maps, which were not originally foreseen.
&lt;SUP&gt;3&lt;/SUP&gt;Cat-5/B was operated a few more months until the number of
images acquired met the requirements. This article briefly describes the
FSSCat mission and the FMPL-2 payload and summarizes the main scientific
results.</description>
</item>
<item>
<title> Impact of Solar Activity on Snow Cover Variation Over the Tibetan Plateau and Linkage to the Summer Precipitation in China</title>
<link>https://ui.adsabs.harvard.edu/abs/2022FrEaS...9.1213S</link>
<description>Solar activity is one of the main external forcing factors driving the
Earth's climate system to change. The snow cover over the Tibetan
Plateau is an important physical factor affecting the East Asian
climate. At present, insufficient research on the connection between
solar activity and snow cover over the Tibetan Plateau has been carried
out. Using Solar Radio Flux (SRF), Solar Sunspot Number (SSN), and Total
Solar Irradiance (TSI) data, this paper calculated the correlation
coefficients with snow indices over the Tibetan Plateau, such as winter
and spring snow depth (WSD/SSD) and snow day number (WSDN/SSDN). These
snow indices are obtained from the daily gauge snow data in the Tibetan
Plateau. Through correlation analyses, it is found that there are
significant synchronous or lag correlations between snow indices and
solar parameters on multi-time scales. In particular, the Spring Snow
Day Number (SSDN) is of significant synchronous or lag correlation with
SRF, SSN, and TSI on multi-time scales. It is further found that SSDN
over the Tibetan Plateau has more stable positive correlations with SRF
by using the 21-year running mean and cross spectrum analyses.
Therefore, SSDN can be ascertained to be the most sensitive snow index
to the solar activity compared with other snow indices. Moreover, its
influence on summer precipitation of China is strongly regulated by
solar activity. In high solar activity years (HSAY), the significant
correlated area of summer precipitation in China to SSDN is located
further north than that in low solar activity years (LSAY). Such impact
by solar activity is also remarkable after excluding the impact of ENSO
(i.e., El Nio-Southern Oscillation) events. These results provide
support for the application of snow indices in summer rainfall
prediction in China.</description>
</item>
<item>
<title> Simulations of the Antenna-shielding Effect of the Daocheng Solar Radio Telescope (DSRT)</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ChJSS..42..294L</link>
<description>Not Available</description>
</item>
<item>
<title> Measuring differential rotation from full disk ALMA images of the Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2022CEAB...46....4S</link>
<description>An automatic method for measuring the differential rotation profile of
the Sun from short time span data, based on tracking features with an
optical flow algorithm and robust iterative fitting, is presented. The
method is first tested on the synthetic data and SDO/HMI magnetograms,
and later applied to ALMA full disk band 6 solar images. The method
successfully recovers the differential rotation profile, however, it is
found to be very sensitive to input parameters and image quality, and
further work is needed to devise methods for finding optimal parameters.</description>
</item>
<item>
<title> Fundamental Electromagnetic Emissions by a Weak Electron Beam in Solar Wind Plasmas with Density Fluctuations</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...924L..24K</link>
<description>The generation of Langmuir wave turbulence by a weak electron beam in a
randomly inhomogeneous plasma and its subsequent electromagnetic
radiation are studied owing to two-dimensional particle-in-cell
simulations in conditions relevant to type III solar radio bursts. The
essential impact of random density fluctuations of average levels of a
few percents of the background plasma on the characteristics of the
electromagnetic radiation at the fundamental plasma frequency  &lt;SUB&gt; p
&lt;/SUB&gt; is shown. Not only wave nonlinear interactions but also processes
of Langmuir waves' transformations on the density fluctuations
contribute to the generation of such emissions. During the beam
relaxation, the amount of electromagnetic energy radiated at  &lt;SUB&gt; p
&lt;/SUB&gt; in a plasma with density fluctuations strongly exceeds that
observed when the plasma is homogeneous. The fraction of Langmuir wave
energy involved in the generation of electromagnetic emissions at 
&lt;SUB&gt; p &lt;/SUB&gt; saturates around 10&lt;SUP&gt;-4&lt;/SUP&gt;, i.e., one order of
magnitude above that reached when the plasma is uniform. Moreover,
whereas harmonic emission at 2 &lt;SUB&gt; p &lt;/SUB&gt; dominates over
fundamental emission during the time evolution in a homogeneous plasma,
fundamental emission is strongly dominant when the plasma contains
density fluctuations, at least during several thousands of plasma
periods before being overcome by harmonic emission when the total
electromagnetic energy begins to saturate.</description>
</item>
<item>
<title> Observational Signatures of Tearing Instability in the Current Sheet of a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...924L...7L</link>
<description>Magnetic reconnection is a fundamental physical process converting
magnetic energy into not only plasma energy but also particle energy in
various astrophysical phenomena. In this Letter, we show a unique data
set of a solar flare where various plasmoids were formed by a
continually stretched current sheet. Extreme ultraviolet images captured
reconnection inflows, outflows, and particularly the recurring plasma
blobs (plasmoids). X-ray images reveal nonthermal emission sources at
the lower end of the current sheet, presumably as large plasmoids with a
sufficiently amount of energetic electrons trapped in them. In the radio
domain, an upward, slowly drifting pulsation structure, followed by a
rare pair of oppositely drifting structures, was observed. These
structures are supposed to map the evolution of the primary and the
secondary plasmoids formed in the current sheet. Our results on
plasmoids at different locations and scales shed important light on the
dynamics, plasma heating, particle acceleration, and transport processes
in the turbulent current sheet and provide observational evidence for
the cascading magnetic reconnection process.</description>
</item>
<item>
<title> Spectral Analysis of Solar Radio Type III Bursts from 20 kHz to 410 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ApJ...924...58S</link>
<description>We present the statistical analysis of the spectral response of solar
radio type III bursts over the wide frequency range between 20 kHz and
410 MHz. For this purpose, we have used observations that were carried
out using both spaced-based (Wind/Waves) and ground-based (Nanay
Decameter Array and Nanay Radioheliograph) facilities. In order to
compare the flux densities observed by the different instruments, we
have carefully calibrated the data and displayed them in solar flux
units. The main result of our study is that type III bursts, in the
metric to hectometric wavelength range, statistically exhibit a clear
maximum of their median radio flux density around 2 MHz. Although this
result was already reported by inspecting the spectral profiles of type
III bursts in the frequency range 20 kHz-20 MHz, our study extends such
analysis for the first time to metric radio frequencies (i.e., from 20
kHz to 410 MHz) and confirms the maximum spectral response around 2 MHz.
In addition, using a simple empirical model we show that the median
radio flux S of the studied data set obeys the polynomial form Y = 0.04X
&lt;SUP&gt;3&lt;/SUP&gt; - 1.63X &lt;SUP&gt;2&lt;/SUP&gt; + 16.30X - 41.24, with
$X=\mathrm{ln}({F}_{\mathrm{MHz}})$ and with
$Y=\mathrm{ln}({S}_{\mathrm{SFU}})$ . Using the Sittler and
Guhathakurtha model for coronal streamers, we have found that the
maximum of radio power therefore falls in the range 4 to 10 R
&lt;SUB&gt;&lt;/SUB&gt;, depending on whether the type III emissions are assumed to
be at the fundamental or the harmonic.</description>
</item>
<item>
<title> Short-Term Prediction of Solar F_{10.7} Radiation Flux Based on Deep Learning</title>
<link>https://ui.adsabs.harvard.edu/abs/2022AcASn..63...11G</link>
<description>Solar radiation flux $F_{10.7}$ is widely used in space environment
models such as the empirical model of atmosphere and the ionospheric
model as an input parameter, and its prediction accuracy directly
affects the precision of spacecraft orbit prediction. The relationship
between solar radiation flux ($F_{10.7}$) and sunspot number (SSN) is
calculated by the time series method, and the linear relationship
between them is given. On this basis, we proposed a Short-Term
prediction method for $F_{10.7}$ in the next 7 days based on the 54-day
solar radiation flux index combined with the sunspots number into the
LSTM (Long and Short Term Memory) neural network, compared the
prediction results with those of other forecasting methods. The results
show: (1) The performance of the proposed 7-day method model is better
than that of the Space Weather Prediction Center (SWPC), and the
correlation coefficient (CC) between the predicted and observed values
reaches 0.96. At the same time, the root mean square error is about
11.62 solar radiation flux units, and the RMSE of the forecast result is
lower than that of SWPC, which decreases by about 11\%. (2) According to
the statistical results of 23 and 24 solar activity cycle year, the
optimal MAPE (Mean Absolute Percentage Error) of the average absolute
percentage error of $F_{10.7}$ index on the seventh day of high solar
activity year can reach 12.9\%, and the optimal MAPE of low solar
activity year can reach 2.5\%. (3) The results of combined sunspot
number LSTM and LSTM using only $F_{10.7}$ showed that the newly
introduced sunspot number was effective in improving the prediction of
LSTM, and the root mean square error (RMSE) of these two models were
lower than that of SWPC by about 11\% and 5\%, respectively.</description>
</item>
<item>
<title> Digital Signal Processing in RadioSolariz Project Using SSE2</title>
<link>https://ui.adsabs.harvard.edu/abs/2022ARBl...34...66Z</link>
<description>This paper aims at elaborating on the digital signal processing
techniques used in data manipulation in the radioSolariz solar radio-
telescope project. Focus is drawn on the implementation of different
digital signal processing algorithms through the use of streaming single
instruction  multiple data extensions 2. This complementary instruction
set to general purpose personal computer microprocessors offers
increased computational power by realizing parallel processing. The
benefit is a higher data throughput while lowering the electrical power
consumption of the digital signal processing computer. Optimized code
fragments are shown along with original code snippets and these are
discussed and analyzed. Future work and implementation of other modern
parallel processing technologies are envisaged.</description>
</item>
<item>
<title> Parker Solar Probe detects solar radio bursts related with a behind-the-limb active region</title>
<link>https://ui.adsabs.harvard.edu/abs/2022A&amp;A...657A..21S</link>
<description>Context. The interpretation of solar radio bursts observed by Parker
Solar Probe (PSP) in the encounter phase plays a key role in
understanding intrinsic properties of the emission mechanism in the
solar corona. Lower time-frequency resolution of the PSP receiver can be
overcome by simultaneous ground-based observations using more advanced
antennas and receivers. &lt;BR /&gt; Aims: In this paper we present such
observations for which the active active region 12 765, begetter of type
III, J, and U solar bursts, was within sight of ground-based instruments
and behind the solar limb of the PSP spacecraft. &lt;BR /&gt; Methods: We used
a subarray of the Giant Ukrainian Radio Telescope to get the spectral
properties of radio bursts at the frequency range of 8-80 MHz, as well
as the PSP radio instruments with a bandwidth of 10.5 kHz-19.2 MHz,
during solar observations on June 5, 2020. &lt;BR /&gt; Results: We directly
detected the radio events initiated by the active region behind the
solar limb of the PSP spacecraft, using special conditions in the solar
corona, due to the absence of active regions from the PSP side.
Following the generation mechanism of solar radio emission, we refined
the density model for the solar corona above the active region 12765
responsible for the radio bursts. Based on the PSP spacecraft position
near the Sun and delays of radio waves between space- and ground-based
records, we found the corresponding radio responses on the PSP
spectrogram. &lt;BR /&gt; Conclusions: The absence of sunspots from the PSP
side contributes to the propagation of radio waves from a dense loop of
the Sun to quiet regions with low densities, through which PSP
instruments can detect the radiation.</description>
</item>
<item>
<title> Multi-Instrument Investigation of the Impact of the Space Weather Events of 6-10 September 2017</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SpWea..1902806A</link>
<description>We analyzed the space weather events of 6-10 September 2017 using the
multi-instrument approach. We focused on the four X-class flares which
emanated from the Active Region AR 12673 and the Ground Induced Currents
hazard associated with the geomagnetic storm of 7-8 September 2017. The
flare effect on the equatorial electrojet (EEJ) recorded on board the
SWARM satellite and on the horizontal component of the geomagnetic field
(H) records of ground-based magnetometers was further examined. During
the X2.2/X1.3 flares of 6/7 September, the maximum percentage Global
Navigation Satellite System (GNSS) vertical Total Electron Content
(VTEC) increase was 6.9%/5.0% in Dakar/Porto Velho. During the X9.3/X8.2
flare of 6/10 September it was 7.9%/18.8% in Ascension Island/Kourou.
The strongest Solar Flare Effect occurred in Mbour and Kourou during the
respective flare. However, the highest EEJ increase was observed during
the X2.2 and X9.3 flares. Interestingly, the X.9.3 flare resulted in a
stronger ionospheric response than the X8.2 flare. Furthermore, global
TEC map showed a higher response in the African and South American
longitude during the respective event. The total radio fade-out lasted
from 30 to 90 min at the Hermanus and Sao Luis ionosondes during the
flares, while the risk level to critical ground infrastructures based on
the geomagnetically induced currents hazard was very low risk. Our
results highlight the potential GPS positioning errors induced by sudden
increase in TEC and the loss of high-frequency communication and GNSS
navigation signals associated with these solar events.</description>
</item>
<item>
<title> Quasi-Periodic Energy Release in a Three-Ribbon Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..188Z</link>
<description>Quasi-periodic pulsations (QPPs) are found in solar flares of various
magnetic morphologies, e.g. in two-ribbon or circular-ribbon flares, and
the mechanisms of their generation are not yet clear. Here we present
the first detailed analysis of QPPs (with a period P =54 13 seconds)
found in the Ramaty High Energy Solar Spectroscopic Imager (RHESSI)
observations of a relatively rare three-ribbon M1.1 class flare that
occurred on 5 July 2012 (SOL2012-07-05T06:49). QPPs are manifested in
the temporal profiles of temperature [T ] and emission measure [E M ] of
"super-hot" (T&lt;SUB&gt;s&lt;/SUB&gt;30 - 50 MK) plasma but are almost invisible
in the profiles of "hot" (T&lt;SUB&gt;h&lt;/SUB&gt;15 - 20 MK) plasma parameters
when approximating X-ray spectra of the flare with the bremsstrahlung
spectrum of a two-temperature thermal (Maxwellian) plasma. In addition,
QPPs with a similar period are found in the temporal profiles of the
flux and spectral index of nonthermal electrons if the observed X-ray
spectra are approximated by a combination of the bremsstrahlung spectra
of a single-temperature plasma and nonthermal electrons with a power-law
energy distribution. QPPs are not well expressed in the X-ray flux
according to RHESSI and GOES data, or in radio data. The QPPs are
accompanied by apparent systematic movement of a single X-ray source at
a low speed of 34 21 km s&lt;SUP&gt;1&lt;/SUP&gt; along the central flare ribbon
over a narrow (&lt;5 Mm) "tongue" of negative magnetic polarity, elongated
(20 Mm) between two areas of positive polarity. The results of magnetic
extrapolation in the nonlinear force-free field (NLFFF) approximation
show that the X-ray source could move along curved and twisted field
lines between two sheared flare arcades. It is worth noting that in the
homologous three-ribbon M6.1 flare (SOL2012-07-05T11:39), which occurred
in the same region about five hours later, the X-ray sources moved much
less systematically and did not produce similar QPPs. We interpret the
observed QPPs as a result of successive episodes of energy release in
different spatial locations. In each pulsation, (1 - 4)10&lt;SUP&gt;29&lt;/SUP&gt;
erg is released in the form of thermal energy of hot and super-hot
plasmas (or accelerated electrons), which is comparable with the energy
of a microflare. The total kinetic energy released during all QPPs is
(0.7 - 3.5)10&lt;SUP&gt;30&lt;/SUP&gt; erg, which is about an order of magnitude
less than the free magnetic energy 1.56 10&lt;SUP&gt;31&lt;/SUP&gt; erg released
in the flare region. We discuss possible propagating triggers of the
quasi-periodic energy release (slow magnetoacoustic waves, asymmetric
rise of curved/twisted field lines, flapping oscillations, and thermal
instability in a reconnecting current sheet) and argue that the current
state of available mechanisms and observations does not allow us to
reach an unambiguous conclusion.</description>
</item>
<item>
<title> Common Origin of Quasi-Periodic Pulsations in Microwave and Decimetric Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..185K</link>
<description>We analyse quasi-periodic pulsations (QPP) detected in the microwave and
decimetre radio emission of the 5 September 2017 7:04 UT
(SOL2017-09-05T07:04) solar flare, using simultaneous observations by
the Siberian Radioheliograph 48 (SRH-48, 4 - 8 GHz) and Mingantu
Spectral Radioheliograph (MUSER-I, 0.4 - 2 GHz). The microwave emission
was broadband with a typical gyrosynchrotron spectrum, while a quasi-
periodic enhancement of the decimetric emission appeared in a narrow
spectral band (500 - 700 MHz), consistent with the coherent-plasma-
emission mechanism. The periodicity that we found in microwaves is about
30 seconds, coming from a compact loop-like source with a typical height
of about 31 Mm. The decimetric emission exhibited a periodicity of about
6 seconds. We suggest a qualitative scenario linking the QPPs observed
in both incoherent and coherent spectral bands and their generation
mechanisms. The properties of the QPPs found in the microwave signal are
typical for perturbations of the flare loop by the standing sausage mode
of a fast magnetohydrodynamic (MHD) wave. Our analysis indicated that
this sausage-oscillating flare loop was the primary source of
oscillations in the discussed event. The suggested scenario is that a
fundamental sausage harmonic is the dominant cause for the observed QPPs
in the microwave emission. The initiation of oscillations in the
decimetric emission is caused by the third sausage harmonic via periodic
and nonlinear triggering of the acceleration processes in the current
sheets, formed at the interface between the sausage-oscillating flare
loop and the external coronal loop that extended to higher altitudes.
Our results demonstrate the possible role of MHD wave processes in the
release and transport of energy during solar flares, linking coherent
and incoherent radio emission mechanisms.</description>
</item>
<item>
<title> Measurement of Siberian Radioheliograph cable delays</title>
<link>https://ui.adsabs.harvard.edu/abs/2021STP.....7d..93L</link>
<description>To achieve the maximum dynamic range of solar radio images obtained
using aperture synthesis in relatively wide frequency bands 0.10.5 % of
the operating frequency, it is necessary to compensate the signal
propagation delays in the antenna receive path before calculating
visibility functions (hereinafter visibilities). When visibilities are
corrected without delay compensation, the signal-to-noise ratio
decreases due to residual phase slopes in the receiving system
bandwidth. In addition to enhancing dynamic range, preliminary
compensation for delays simplifies real-time imaging  no antenna gain
calibration is required to get a first approximation image. The
requirements for the accuracy of antenna placement are also reduced  in
contrast to the measurement of the phase visibility error, the
measurement of the delay is actually not so critical to the antenna
position errors that are larger than the operating wavelength. The
instantaneous frequency band of the Siberian Radioheliograph, which
determines the minimum step for measuring the phase slope, and hence the
accuracy of determining the delay, is 10 MHz. At the speed of light in
an optical fiber of ~0.7c, a step of 10 MHz makes it possible to
unambiguously measure the difference between electrical lengths of
cables up to 20 m and to correct antenna positions by radio
observations, even if the error in the position of the antennas exceeds
the operating wavelength. Correction of the band phase slopes during the
observation time adapts the radio telescope to the temperature drift of
delays and decreases antenna gain phase spread. This, in turn, leads to
more stable solutions to systems of equations containing antenna gains
as unknowns.</description>
</item>
<item>
<title> DSC based Dual-Resunet for radio frequency interference identification</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..299Z</link>
<description>Radio frequency interference (RFI) will pollute the weak astronomical
signals receivedby radio telescopes, which in return will seriously
affect the time-domain astronomical observation and research. In this
paper, we use a deep learning method to identify RFI in frequency
spectrum data, and propose a neural network based on Unet that combines
the principles of depthwise separable convolution and residual, named
DSC Based Dual-Resunet. Compared with the existing Unet network, DSC
Based Dual-Resunet performs better in terms ofaccuracy, F1 score, and
MIoU, and is also better in terms of computation cost where the model
size and parameter amount are 12.5% of Unet and the amount of
computation is 38%ofUnet. The experimental results show that the
proposed network is a high-performance and lightweight network, and it
is hopeful to be applied to RFI identification of radio telescopes on a
large scale.</description>
</item>
<item>
<title> Observational results of MUSER during 20142019</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..284Z</link>
<description>The solar radio signal that can be received by the ground-based
telescopes covers a wide frequency range, allowing us to monitor the
complex physical processes occurred from the solar surface to the vast
interplanetary space. MingantU SpEctral Radioheliograph (MUSER), as the
latest generation of solar dedicated radio spectral-imaging instrument
in the centimeter-decimeter wavelengths, has accumulated a large number
of observational data since its commissioning observation in 2014. This
paper presents the main observational results identified by MUSER from
2014 to 2019, including the quiet Sun and 94 solar radio burst events.
We find that there are 81 events accompanied with Geostationary
Operational Environmental Satellites (GOES) soft X-ray (SXR) flares,
among which the smallest flare class is B1.0. There are 13 events
without accompanying any recorded flares, among which the smallest SXR
intensity during the radio burst period is equivalent to level-A. The
main characteristics of all radio burst events are presented, which
shows the powerful ability of MUSER to capture the valuable information
of the solar non-thermal processes and the importance for space weather.
This work also provides a database for further in-depth research.</description>
</item>
<item>
<title> Energy and spectral analysis of confined solar flares from radio and X-ray observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..274T</link>
<description>The energy and spectral shape of radio bursts may help us understand the
generation mechanism of solar eruptions, including solar flares, coronal
mass ejections, eruptive filaments, and various scales of jets. The
different kinds of flares may have different characteristics of energy
and spectral distribution. In this work, we selected 10 mostly confined
flare events during October 2014 to investigate their overall spectral
behaviour and the energy emitted in microwaves by using radio
observations from microwaves to interplanetary radio waves, and X-ray
observations of GOES, RHESSI, and Fermi/GBM. We found that: all the
confined flare events were associated with a microwave continuum burst
extending to frequencies of 9.4  15.4 GHz, and the peak frequencies of
all confined flare events are higher than 4.995 GHz and lower than or
equal to 17 GHz. The median value is around 9 GHz. The microwave burst
energy (or fluence) and the peak frequency are found to provide useful
criteria to estimate the power of solar flares. The observations imply
that the magnetic field in confined flares tends to be stronger than
that in 412 flares studied by Nita et al. (2004). All 10 events studied
did not produce detectable hard X-rays with energies above 300 keV
indicating the lack of efficient acceleration of electrons to high
energies in the confined flares.</description>
</item>
<item>
<title> from solar patrols to pulsars and VLBI</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JAHH...24..957C</link>
<description>The development of radio astronomy in Poland took some time to occur, in
view of the destruction of the country during World War II. Also, the
shift of the country's borders in favor of the Soviet Union led to the
loss of two important astronomy observatories: the historic centers of
astronomy in Wilno and Lww. The relocation of these important
astronomical centers to Toru and Wrocaw in the West needed
considerable effort. Hence radio astronomy was a second priority as the
optical astronomers had to become operational first. Nevertheless, in
the 1950s groups in Krakw and Toru started to erect radio telescopes.
In Krakw solar radio astronomy became established. In Toru, there were
experiments with low frequency parabolic antennas. First, a 15-m dish
was built, and later a 32-m dish became operational. In Krakw the solar
patrol continued and a LOFAR station was added. Contacts with radio
observatories in other parts of the world were established. In 1988 a
new regional university was established in Zielona Gra, and a group
involved in pulsar research was built up there. Astrophysics departments
existed at Warszawa (Warsaw) University and at the Nicolaus Copernicus
Astronomical Center (CAMK) of the Polish Academy of Sciences, and the
universities in Pozna, Gdask and Lublin had astronomical departments,
but none of these was involved in radio astronomy.</description>
</item>
<item>
<title> the Form of Cycles</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61S..75D</link>
<description>Analysis of the features of the form of low solar cycles 23 and 24 for
the solar-activity indices (F is the solar radio flux at a wavelength of
10.7 cm, Rz and Ri are the relative numbers of sunspots, old and new
versions) and the ionospheric index of this activity T. For this, the
analyzed indices are reduced to the Rz scale and smoothed (with a
24-month Gaussian filter) values of these indices are considered. It was
found that the cycle forms were preserved for cycles 23 and 24 and
previous solar cycles by index Rz, i.e., a definite connection was made
between the cycle amplitude and the time of the onset of the cycle
maximum. The same relationship was observed for the Ri index, except for
cycle 23, in which the observed cycle maximum occurred 7 months later
than the expected time based on previous cycles. For indices F and T,
the cycle shapes also persisted up to cycle 22, but the observed cycle
maxima in cycles 23 and 24 occurred almost a year later than expected,
which is one of the properties of the new regime of prolonged low solar
activity. In this mode, the connection between the Ri and F indices is
broken, which leads to different cycle forms for these indices.</description>
</item>
<item>
<title> Increased Microwave Radiation Brightness as a Sign of Flare-Producing Active Regions Based on Observations of NOAA Active Region 12371</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61S..24P</link>
<description>Methods to predict solar flares based on observations in the microwave
range with radio telescopes with high angular resolution continue to be
developed. The results are presented for an analysis of observations of
NOAA active region 12371, in a quasi-quiescent state characterized by
increased brightness of emission in the microwave range, which causes
multiple eruptive events. According to observations with the RATAN-600
radio telescope during the event of June 21, 2015, a sharp change in the
structure of the image of the microwave radiation source above NOAA
region 12 371 was recorded. It was presumably interpreted by short-term
plasma heating over the region of the delta configuration of the
magnetic field in the tail part of the active region. Due to the high
sensitivity of RATAN-600 during polarization measurements, it is
possible to localize the position of the cloud in which the emission or
acceleration of fast particles occurs with known models of the magnetic
field.</description>
</item>
<item>
<title> Spectral Diagnostics of Langmuir Coronal Plasma Turbulence Based on the Radio Emission at the Double Plasma Frequency</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61.1172K</link>
<description>Analysis of the radiation of solar radio bursts with a fine structure
generated at a double plasma frequency makes it possible to obtain
information on the energy density of Langmuir waves in solar plasma and
on the volume of the region of the generation of radio emission when
Langmuir waves merge. As an example, we consider the spectrum of a radio
burst on August 17, 1999. Assuming that this radio burst is the result
of the merging of Langmuir waves, a possible spectrum of Langmuir waves
has been found. This makes it possible to explain the form of the
particular spectrum of the radio burst, and the relationship between the
volume of the emitting region and the energy density of Langmuir waves
has been obtained. It is shown that the linear size of the emitting
region can be ~10&lt;SUP&gt;8&lt;/SUP&gt; cm or less. It is also shown that plasma
inhomogeneity will lead to an increase in the width of the radio
emission spectrum. Small (~10%) changes in the plasma concentration in
discrete sources of radio emission may lead to the formation of local
spectral maxima.</description>
</item>
<item>
<title> the Event of July 4, 2012</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61.1045M</link>
<description>The temporal evolution of thermal bremsstrahlung sub-THz emission from a
flare chromosphere and transition region is analyzed based on the
F-CHROMA solar flare model database (https://www.fchroma.org) and solar
flare observations with the RT-7.5 radio telescope at 93 and 140 GHz on
July 4, 2012. The model is based on the RADYN numerical code, which
describes the response of chromospheric background plasma to the action
of a beam of accelerated electrons in the form of a triangular pulse.
The positive slope of the spectrum in the sub-THz frequency range has
been formed over the entire burst. A thin layer of low temperature and
high plasma density (the so-called chromospheric condensation) appears.
It moves to the region of higher altitudes and effectively absorbs the
sub-THz emission. It is shown based on the RHESSI hard X-ray
observations that the chromospheric thermal plasma cannot provide the
observed sub-THz emission fluxes during the solar flare on July 4, 2012.
The cause of the obtained discrepancy is discussed.</description>
</item>
<item>
<title> The Origin of Time Delays between Sub-Terahertz and Soft X-ray Emission from Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61..993S</link>
<description>The time delays between sub-terahertz (sub-THz) and soft X-ray (SXR)
emission from solar flares with a positive spectrum slope at frequencies
of &gt;100 GHz are considered. Based on a cross-correlation analysis of the
time profiles of sub-THz and SXR emission from 11 flare events obtained
from the KOSMA (230 GHz), SST (212 GHz), and RT-7.5 (93 GHz) telescopes,
as well as the GOES satellite in channel 18 , we identified two main
types of sub-THz events. Type I includes four X-class events with a
well-defined Neupert effect, i.e., the sub-THz flux outpaces the SXR
flux by 29 min. Type II includes seven M-class flares, in which the
time profiles behave similarly and the delays do not exceed 30 s. The
different mechanisms of radio emission in different layers of the solar
atmosphere may be responsible for the positive slope of the sub-THz
spectrum of flares.</description>
</item>
<item>
<title> Decimetric Type-U Solar Radio Bursts and Associated EUV Phenomena on 2011 February 9</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...923..268G</link>
<description>A GOES M1.9 flare took place in active region AR 11153 on 2011 February
9. With a resolution of 200 kHz and a time cadence of 80 ms, the
reverse-drifting (RS) type-III bursts, intermittent sequence of type-U
bursts, drifting pulsation structure (DPS), and fine structures were
observed by the Yunnan Observatories Solar Radio Spectrometer (YNSRS).
Combined information revealed by the multiwavelength data indicated that
after the DPS was observed by YNSRS, the generation rate of type-U
bursts suddenly increased to 5 times what it had been. In this event,
the generation rate of type-U bursts may depend on the magnetic-
reconnection rate. Our observations are consistent with previous
numerical simulation results. After the first plasmoid produced (plasma
instability occurred), the magnetic-reconnection rate suddenly increased
by 5 to 8 times. Furthermore, after the DPS, the frequency range of the
turnover frequency of type-U bursts was obviously broadened to thrice
what it was before, which indicates a fluctuation amplitude of the
density in the loop top. Our observations also support numerical
simulations during the flare-impulsive phase. Turbulence occurs at the
top of the flare loop and the plasmoids can trap nonthermal particles,
causing density fluctuation at the loop top. The observations are
generally consistent with the results of numerical simulations, helping
us to better understand the characteristics of the whole physical
process of eruption.</description>
</item>
<item>
<title> A DEFT Way to Forecast Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...922..218K</link>
<description>Solar flares have been linked to some of the most significant space
weather hazards at Earth. These hazards, including radio blackouts and
energetic particle events, can start just minutes after the flare onset.
Therefore, it is of great importance to identify and predict flare
events. In this paper we introduce the Detection and EUV Flare Tracking
(DEFT) tool, which allows us to identify flare signatures and their
precursors using high spatial and temporal resolution extreme-
ultraviolet (EUV) solar observations. The unique advantage of DEFT is
its ability to identify small but significant EUV intensity changes that
may lead to solar eruptions. Furthermore, the tool can identify the
location of the disturbances and distinguish events occurring at the
same time in multiple locations. The algorithm analyzes high temporal
cadence observations obtained from the Solar Ultraviolet Imager
instrument aboard the GOES-R satellite. In a study of 61 flares of
various magnitudes observed in 2017, the "main" EUV flare signatures
(those closest in time to the X-ray start time) were identified on
average 6 minutes early. The "precursor" EUV signatures (second-closest
EUV signatures to the X-ray start time) appeared on average 14 minutes
early. Our next goal is to develop an operational version of DEFT and to
simulate and test its real-time use. A fully operational DEFT has the
potential to significantly improve space weather forecast times.</description>
</item>
<item>
<title> Multiple Electron Acceleration Instances during a Series of Solar Microflares Observed Simultaneously at X-Rays and Microwaves</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...922..134B</link>
<description>Even small solar flares can display a surprising level of complexity
regarding their morphology and temporal evolution. Many of their
properties, such as energy release and electron acceleration can be
studied using highly complementary observations at X-ray and radio
wavelengths. We present X-ray observations from the Reuven Ramaty High
Energy Solar Spectroscopic Imager and radio observations from the Karl
G. Jansky Very Large Array (VLA) of a series of GOES A3.4-B1.6 class
flares observed on 2013 April 23. The flares, as seen in X-ray and
extreme ultraviolet, originated from multiple locations within active
region NOAA 11726. A veritable zoo of different radio emissions between
1 GHz and 2 GHz was observed cotemporally with the X-ray flares. In
addition to broadband continuum emission, broadband short-lived bursts
and narrowband spikes, indicative of accelerated electrons, were
observed. However, these sources were located up to 150 away from the
flaring X-ray sources but only some of these emissions could be
explained as signatures of electrons that were accelerated near the main
flare site. For other sources, no obvious magnetic connection to the
main flare site could be found. These emissions likely originate from
secondary acceleration sites triggered by the flare, but may be due to
reconnection and acceleration completely unrelated to the cotemporally
observed flare. Thanks to the extremely high sensitivity of the VLA, not
achieved with current X-ray instrumentation, it is shown that particle
acceleration happens frequently and at multiple locations within a
flaring active region.</description>
</item>
<item>
<title> Modeling</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...922..128C</link>
<description>There is a wide consensus that the ubiquitous presence of magnetic
reconnection events and the associated impulsive heating (nanoflares)
are strong candidates for solving the solar coronal heating problem.
Whether nanoflares accelerate particles to high energies like full-sized
flares is unknown. We investigate this question by studying the type III
radio bursts that the nanoflares may produce on closed loops. The
characteristic frequency drifts that type III bursts exhibit can be
detected using a novel application of the time-lag technique developed
by Viall &amp; Klimchuk (2012) even when there are multiple overlapping
events. We present a simple numerical model that simulates the expected
radio emission from nanoflares in an active region, which we use to test
and calibrate the technique. We find that in the case of closed loops
the frequency spectrum of type III bursts is expected to be extremely
steep such that significant emission is produced at a given frequency
only for a rather narrow range of loop lengths. We also find that the
signature of bursts in the time-lag signal diminishes as: (1) the
variety of participating loops within that range increases; (2) the
occurrence rate of bursts increases; (3) the duration of bursts
increases; and (4) the brightness of bursts decreases relative to noise.
In addition, our model suggests a possible origin of type I bursts as a
natural consequence of type III emission in a closed-loop geometry.</description>
</item>
<item>
<title> The Sun at millimeter wavelengths. III. Impact of the spatial resolution on solar ALMA observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..68E</link>
<description>Context. Interferometric observations of the Sun with the Atacama Large
Millimeter/sub-millimeter Array (ALMA) provide valuable diagnostic tools
for studying the small-scale dynamics of the solar atmosphere. &lt;BR /&gt;
Aims: The aims are to perform estimations of the observability of the
small-scale dynamics as a function of spatial resolution for regions
with different characteristic magnetic field topology facilitate a more
robust analysis of ALMA observations of the Sun. &lt;BR /&gt; Methods: A
three-dimensional model of the solar atmosphere from the radiation-
magnetohydrodynamic code Bifrost was used to produce high-cadence
observables at millimeter and submillimeter wavelengths. The synthetic
observables for receiver bands 3-10 were degraded to the angular
resolution corresponding to ALMA observations with different
configurations of the interferometric array from the most compact, C1,
to the more extended, C7. The observability of the small-scale dynamics
was analyzed in each case. The analysis was thus also performed for
receiver bands and resolutions that are not commissioned so far for
solar observations as a means for predicting the potential of future
capabilities. &lt;BR /&gt; Results: The minimum resolution required to study
the typical small spatial scales in the solar chromosphere depends on
the characteristic properties of the target region. Here, a range from
quiet Sun to enhanced network loops is considered. Limited spatial
resolution affects the observable signatures of dynamic small-scale
brightening events in the form of reduced brightness temperature
amplitudes, potentially leaving them undetectable, and even shifts in
the times at which the peaks occur of up to tens of seconds. Conversion
factors between the observable brightness amplitude and the original
amplitude in the fully resolved simulation are provided that can be
applied to observational data in principle, but are subject to
wavelength-dependent uncertainties. Predictions of the typical
appearance at the different combinations of receiver band, array
configuration, and properties of the target region are conducted. &lt;BR /&gt;
Conclusions: The simulation results demonstrate the high scientific
potential that ALMA already has with the currently offered capabilities
for solar observations. For the study of small-scale dynamic events,
however, the spatial resolution is still crucial, and wide array
configurations are preferable. In any case, it is essential to take the
effects due to limited spatial resolution into account in the analysis
of observational data. Finally, the further development of observing
capabilities including wider array configurations and advanced imaging
procedures yields a high potential for future ALMA observations of the
Sun.</description>
</item>
<item>
<title> First observations and performance of the RPW instrument on board the Solar Orbiter mission</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..41M</link>
<description>The Radio and Plasma Waves (RPW) instrument on the ESA Solar Orbiter
mission is designed to measure in situ magnetic and electric fields and
waves from the continuum up to several hundred kHz. The RPW also
observes solar and heliospheric radio emissions up to 16 MHz. It was
switched on and its antennae were successfully deployed two days after
the launch of Solar Orbiter on February 10, 2020. Since then, the
instrument has acquired enough data to make it possible to assess its
performance and the electromagnetic disturbances it experiences. In this
article, we assess its scientific performance and present the first RPW
observations. In particular, we focus on a statistical analysis of the
first observations of interplanetary dust by the instrument's Thermal
Noise Receiver. We also review the electro-magnetic disturbances that
RPW suffers, especially those which potential users of the instrument
data should be aware of before starting their research work.</description>
</item>
<item>
<title> Simulations of radio-wave anisotropic scattering to interpret type III radio burst data from Solar Orbiter, Parker Solar Probe, STEREO, and Wind</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..34M</link>
<description>&lt;BR /&gt; Aims: We use multi-spacecraft observations of individual type III
radio bursts to calculate the directivity of the radio emission. We
compare these data to the results of ray-tracing simulations of the
radio-wave propagation and probe the plasma properties of the inner
heliosphere. &lt;BR /&gt; Methods: We used ray-tracing simulations of radio-
wave propagation with anisotropic scattering on density inhomogeneities
to study the directivity of radio emissions. Simultaneous observations
of type III radio bursts by four widely separated spacecraft were used
to calculate the directivity and position of the radio sources. The
shape of the directivity pattern deduced for individual events is
compared to the directivity pattern resulting from the ray-tracing
simulations. &lt;BR /&gt; Results: We show that simultaneous observations of
type radio III bursts by four different probes provide an opportunity to
estimate the radio source positions and the directivity of the radio
emission. The shape of the directivity varies from one event to another
and it is consistent with anisotropic scattering of the radio waves. &lt;P
/&gt;ARRAY(0x18a8790)</description>
</item>
<item>
<title> Solar Orbiter/RPW antenna calibration in the radio domain and its application to type III burst observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..33V</link>
<description>Context. In order to allow for a comparison with the measurements from
other antenna systems, the voltage power spectral density measured by
the Radio and Plasma waves receiver (RPW) on board Solar Orbiter needs
to be converted into physical quantities that depend on the intrinsic
properties of the radiation itself (e.g., the brightness of the source).
&lt;BR /&gt; Aims: The main goal of this study is to perform a calibration of
the RPW dipole antenna system that allows for the conversion of the
voltage power spectral density measured at the receiver's input into the
incoming flux density. &lt;BR /&gt; Methods: We used space observations from
the Thermal Noise Receiver (TNR) and the High Frequency Receiver (HFR)
to perform the calibration of the RPW dipole antenna system.
Observations of type III bursts by the Wind spacecraft are used to
obtain a reference radio flux density for cross-calibrating the RPW
dipole antennas. The analysis of a large sample of HFR observations
(over about ten months), carried out jointly with an analysis of TNR-HFR
data and prior to the antennas' deployment, allowed us to estimate the
reference system noise of the TNR-HFR receivers. &lt;BR /&gt; Results: We
obtained the effective length, l&lt;SUB&gt;eff&lt;/SUB&gt;, of the RPW dipoles and
the reference system noise of TNR-HFR in space, where the antennas and
pre-amplifiers are embedded in the solar wind plasma. The obtained
l&lt;SUB&gt;eff&lt;/SUB&gt; values are in agreement with the simulation and
measurements performed on the ground. By investigating the radio flux
intensities of 35 type III bursts simultaneously observed by Wind and
Solar Orbiter, we found that while the scaling of the decay time as a
function of the frequency is the same for the Waves and RPW instruments,
their median values are higher for the former. This provides the first
observational evidence that Type III radio waves still undergo density
scattering, even when they propagate from the source, in a medium with a
plasma frequency that is well below their own emission frequency.</description>
</item>
<item>
<title> In-flight performance and first results</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..26S</link>
<description>Context. The Radio and Plasma Waves (RPW) instrument on board Solar
Orbiter has been operating nearly continuously since the launch in
February 2020. The Time Domain Sampler (TDS) receiver of the RPW
instrument is dedicated to waveform measurements of plasma waves and
dust impact signatures in an intermediate frequency range from 0.2 to
200 kHz. &lt;BR /&gt; Aims: This article presents the first data from the RPW-
TDS receiver and discusses the in-flight performance of the instrument
and, in particular, the on-board wave and dust detection algorithm. We
present the TDS data products and its scientific operation. We
demonstrate the content of the dataset on several examples. In
particular, we study the distribution of solar Langmuir waves in the
first year of observations and one Type III burst event. &lt;BR /&gt; Methods:
The on-board detection algorithm is described in detail in this article
and classifies the observed waveform snapshots, identifying plasma waves
and dust impacts based on the ratio of their maximum amplitude to their
median and on the spectral bandwidth. The algorithm allows TDS to
downlink the most scientifically relevant waveforms and to perform an
on-board statistical characterization of the processed data. &lt;BR /&gt;
Results: The detection algorithm of TDS is shown to perform very well in
its detection of plasma waves and dust impacts with a high accuracy. The
initial analysis of statistical data returned by TDS shows that sporadic
Langmuir waves that are not associated with Type III events are
routinely observed in the inner heliosphere, with a clear increase in
occurrence rate closer to the Sun. We also present an example of RPW
observations during an encounter of the source region of a Type III
burst, which exploits the on-board calculated histograms data.</description>
</item>
<item>
<title> The first widespread solar energetic particle event observed by Solar Orbiter on 2020 November 29</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...656A..20K</link>
<description>Context. On 2020 November 29, the first widespread solar energetic
particle (SEP) event of solar cycle 25 was observed at four widely
separated locations in the inner (1 AU) heliosphere. Relativistic
electrons as well as protons with energies &gt; 50 MeV were observed by
Solar Orbiter (SolO), Parker Solar Probe, the Solar Terrestrial
Relations Observatory (STEREO)-A and multiple near-Earth spacecraft. The
SEP event was associated with an M4.4 class X-ray flare and accompanied
by a coronal mass ejection and an extreme ultraviolet (EUV) wave as well
as a type II radio burst and multiple type III radio bursts. &lt;BR /&gt;
Aims: We present multi-spacecraft particle observations and place them
in context with source observations from remote sensing instruments and
discuss how such observations may further our understanding of particle
acceleration and transport in this widespread event. &lt;BR /&gt; Methods:
Velocity dispersion analysis (VDA) and time shift analysis (TSA) were
used to infer the particle release times at the Sun. Solar wind plasma
and magnetic field measurements were examined to identify structures
that influence the properties of the energetic particles such as their
intensity. Pitch angle distributions and first-order anisotropies were
analyzed in order to characterize the particle propagation in the
interplanetary medium. &lt;BR /&gt; Results: We find that during the 2020
November 29 SEP event, particles spread over more than 230 in longitude
close to 1 AU. The particle onset delays observed at the different
spacecraft are larger as the flare-footpoint angle increases and are
consistent with those from previous STEREO observations. Comparing the
timing when the EUV wave intersects the estimated magnetic footpoints of
each spacecraft with particle release times from TSA and VDA, we
conclude that a simple scenario where the particle release is only
determined by the EUV wave propagation is unlikely for this event.
Observations of anisotropic particle distributions at SolO, Wind, and
STEREO-A do not rule out that particles are injected over a wide
longitudinal range close to the Sun. However, the low values of the
first-order anisotropy observed by near-Earth spacecraft suggest that
diffusive propagation processes are likely involved.</description>
</item>
<item>
<title> Multi-Wavelength Observations of Quasi-Periodic Pulsations in a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..171H</link>
<description>We report our analysis of multi-wavelength observations of quasi-
periodic pulsations (QPPs) during the impulsive phase of the C6.7 flare
on 9 May 2019. The flare was simultaneously observed by Fermi, the New
Vacuum Solar Telescope, the Mingantu Spectral Radioheliograph, the
Nobeyama Radio Polarimeters, and the Atmospheric Imaging Assembly (AIA)
of the Solar Dynamics Observatory. Three well-pronounced pulsations are
detected in full-disk hard X-ray and microwave fluxes, as well as the
local light curves at wavelengths of the H line core, AIA 304 , 171 ,
211 , and 335  between 05:43:30 UT and 05:48:15 UT. The quasi-
periods of about 90 - 110 seconds are determined from their Morlet
wavelet power spectra. Meanwhile, a sequence of three groups of Type-III
radio bursts is seen in the radio dynamic spectrum during the same time
interval. Our observations suggest that the flare QPPs are possibly
related to nonthermal electrons accelerated by the intermittent magnetic
reconnection during the flare's impulsive phase.</description>
</item>
<item>
<title> Solar Flare Effects on the Earth's Lower Ionosphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..157H</link>
<description>Solar flares significantly impact the conditions of the Earth's
ionosphere. In particular, the sudden increase in X-ray flux during a
flare penetrates down to the lowest-lying D-region and dominates
ionization at these altitudes (60 - 100 km). Measurements of very low
frequency (VLF: 3 - 30 kHz) radio waves that reflect at D-region
altitudes provide a unique remote-sensing probe to investigate the
D-region response to solar-flare emissions. Here, using a combination of
VLF amplitude measurements at 24 kHz together with X-ray observations
from the Geostationary Operational Environment Satellite (GOES) X-ray
sensor, we present a large-scale statistical study of 334 solar-flare
events and their impacts on the D-region over the past solar cycle.
Focusing on both GOES broadband X-ray channels, we investigate how the
flare peak fluxes and position on the solar disk dictate an ionospheric
response and extend this to investigate the characteristic time delay
between incident X-ray flux and the D-region response. We show that the
VLF amplitude linearly correlates with both the 1 - 8  and 0.5 - 4 
channels, with correlation coefficients of 0.80 and 0.79, respectively.
For the two X-class flares in our sample, however, there appears to be a
turnover in the linear relationship, similar to previous works. Unlike
higher altitude ionospheric regions for which the location of the flare
on the solar disk affects the ionospheric response, we find that the
D-region response to solar flares does not depend on the flare location.
By comparing the time delays between the peak X-ray fluxes in both GOES
channels and VLF amplitudes, we find that there is an important
difference between the D-region response and the X-ray spectral band. We
also demonstrate for several flare events that show a negative time
delay, the peak VLF amplitude matches with the impulsive 25 - 50 keV
hard X-ray fluxes measured by the Ramaty High Energy Solar Spectroscopic
Imager (RHESSI). These results highlight the importance of performing
full spectral analysis when studying the ionospheric responses to solar
flares.</description>
</item>
<item>
<title> Hysteresis, time lag, and relation between solar activity and cosmic rays during solar cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2021NewA...8901652S</link>
<description>We study galactic cosmic ray (GCR) modulation during solar cycle 24. For
this study we utilize neutron monitor data together with sunspot number
(SSN) and 10.7 cm solar radio flux (SRF) data. We plot hysteresis curve
between the GCR intensity and SSN, and GCR intensity and SRF. We
performed time-lag correlation analysis to determine the time lag
between GCR intensity and solar activity parameters. The time lag is
determined not only for the whole solar cycle, but also during the two
polarity states of the heliosphere (A&lt;0 and A&gt;0) in solar cycle 24. We
notice differences in time lags during two polarity epochs of the solar
cycle. We discuss these differences in the light of existing modulation
models. We compare the results of this very weak solar activity cycle
with the corresponding results reported for the previous comparatively
more active solar cycles.</description>
</item>
<item>
<title> Statistical Analysis of the Orbital Motion of Selected Artificial Earth Satellites during Solar Cycle 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2021KPCB...37..310B</link>
<description>A statistical analysis of selected parameters of solar activity and
orbital motion of artificial Earth satellites (AES's) during solar cycle
24 is carried out. Inactive satellites, launch vehicle (LV) stages, and
their debris moving mainly in low orbits are studied. Different analysis
algorithms are applied to the time series of the solar radio flux
F&lt;SUB&gt;10.7&lt;/SUB&gt; and the calculated deceleration rate dP/dt of the
investigated space objects (SOs): their annual statistical indices are
estimated, these parameters are studied for periodicity (wavelet
analysis), and a test additive decomposition into trend and seasonal
components is performed. It is found that the satellite deceleration
rate in the vicinity of the solar maximum (20122014) increases by a
factor of ten. For the solar radio flux F&lt;SUB&gt;10.7&lt;/SUB&gt; and the
kinematic parameter dP/dt of SOs 06073 and 31117, seasonal changes,
cyclicity with a period of 27 days, etc. are confirmed. A clear
anticorrelation between the trends of the corresponding parameters
within 0.730.95 for SO 31117 during 20112018 and 0.820.95 for SO
37794 during 20122018 is observed.</description>
</item>
<item>
<title> Relation of the Monthly Mean Ionospheric T Index to Solar and Geomagnetic Activity Indices</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61..830D</link>
<description>An analysis of the relation of the monthly mean ionospheric T index to
the solar (F107) and geomagnetic (Ap) activity indices is presented
based on a dataset of these indices for 19542020. F107 and Ap are the
monthly mean flux of the solar radio emission at a wavelength of 10.7 cm
and the planetary Ap-index of geomagnetic activity, respectively. It is
found that the effective index F = (F107&lt;SUB&gt;0&lt;/SUB&gt; +
F107&lt;SUB&gt;1&lt;/SUB&gt;)/2 provides a high correlation between the ionospheric
and solar indices; F107&lt;SUB&gt;0&lt;/SUB&gt; and F107&lt;SUB&gt;1&lt;/SUB&gt; are the F107
indices over the given and previous months. The dependence of T on F in
the form of a second-degree polynomial makes it possible to reproduce
9598% of variations in T over the analyzed time interval. Thus, the
additional contribution of Ap to T is insignificant. Nevertheless, the
contribution of Ap to T depends on the time of year: it is insignificant
in January and significant in July. This revealed property of the annual
anomaly in ionospheric parameters is conserved also for the contribution
of the aa index of geomagnetic activity to the ionospheric T index. In
all considered cases, an increase in Ap or aa leads to a decrease in the
ionospheric T index, i.e., a mean (global) decrease in the median of the
concentration in the F2-layer maximum. Under the same other conditions,
such decrease is more significant for July than for January.</description>
</item>
<item>
<title> On the Issue of the Origin of Type II Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...922...82C</link>
<description>Type II solar radio bursts are among the most powerful events in the
solar radio emission in the meter wavelength range. It is generally
accepted that the agents generating type II radio bursts are
magnetohydrodynamic shock waves. But the relationship between the shock
waves and the other manifestations of the large-scale disturbances in
the solar atmosphere (coronal mass ejections, Morton waves, EUW waves)
remains unclear. To clarify a problem, it is important to determine the
conditions of generation of type II radio bursts. Here, the model of the
radio source is based on the generation of radio emission within the
front of the collisionless shock wave where the Buneman instability of
plasma waves is developed. In the frame of this model, the Alfvn
magnetic Mach number must exceed the critical value, and there is a
strict restriction on the perpendicularity of the front. The model
allows us to obtain the information about the parameters of the shock
waves and the parameters of the medium by the parameters of type II
bursts. The estimates, obtained in this paper for several events with
the band splitting of the fundamental and harmonic emission bands of the
type II bursts, confirm the necessary conditions of the model. In this
case the registration of type II radio bursts is an indication of the
propagation of shock waves in the solar atmosphere, and the absence of
type II radio bursts is not an indication of the absence of shock waves.
Such a situation should be taken into account when investigating the
relationship between type II radio bursts and other manifestations of
solar activity.</description>
</item>
<item>
<title> Detection of Flare Multiperiodic Pulsations in Mid-ultraviolet Balmer Continuum, Ly, Hard X-Ray, and Radio Emissions Simultaneously</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...921..179L</link>
<description>Quasi-periodic pulsations (QPPs), which usually appear as temporal
pulsations of the total flux, are frequently detected in the light
curves of solar/stellar flares. In this study, we present the
investigation of nonstationary QPPs with multiple periods during the
impulsive phase of a powerful flare on 2017 September 6, which were
simultaneously measured by the Hard X-ray Modulation Telescope (Insight-
HXMT), as well as the ground-based BLENSW. The multiple periods,
detected by applying a wavelet transform and Lomb-Scargle periodogram to
the detrended light curves, are found to be ~20-55 s in the Ly and mid-
ultraviolet Balmer continuum emissions during the flare impulsive phase.
Similar QPPs with multiple periods are also found in the hard X-ray
emission and low-frequency radio emission. Our observations suggest that
the flare QPPs could be related to nonthermal electrons accelerated by
the repeated energy release process, i.e., triggering of repetitive
magnetic reconnection, while the multiple periods might be modulated by
the sausage oscillation of hot plasma loops. For the multiperiodic
pulsations, other generation mechanisms could not be completely ruled
out.</description>
</item>
<item>
<title> Localized Acceleration of Energetic Particles by a Weak Shock in the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...921...61L</link>
<description>Globally propagating shocks in the solar corona have long been studied
to quantify their involvement in the acceleration of energetic
particles. However, this work has tended to focus on large events
associated with strong solar flares and fast coronal mass ejections
(CMEs), where the waves are sufficiently fast to easily accelerate
particles to high energies. Here we present observations of particle
acceleration associated with a global wave event which occurred on 2011
October 1. Using differential emission measure analysis, the global
shock wave was found to be incredibly weak, with an Alfvn Mach number
of ~1.008-1.013. Despite this, spatially resolved type III radio
emission was observed by the Nanay RadioHeliograph at distinct
locations near the shock front, suggesting localized acceleration of
energetic electrons. Further investigation using magnetic field
extrapolation identified a fan structure beneath a magnetic null located
above the source active region, with the erupting CME contained within
this topological feature. We propose that a reconfiguration of the
coronal magnetic field driven by the erupting CME enabled the weak shock
to accelerate particles along field lines initially contained within the
fan and subsequently opening into the heliosphere, producing the
observed type III emission. These results suggest that even weak global
shocks in the solar corona can accelerate energetic particles via
reconfiguration of the surrounding magnetic field.</description>
</item>
<item>
<title> Characterising coronal turbulence using snapshot imaging of radio bursts in 80-200 MHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...655A..77M</link>
<description>Context. Metrewave solar type-III radio bursts offer a unique means to
study the properties of turbulence across coronal heights. Theoretical
models have shown that the apparent intensity and size of the burst
sources evolve at sub-second scales under the influence of local
turbulence. The properties of the evolution vary with observation
frequency. However, observational studies remained difficult due to the
lack of high fidelity imaging capabilities at these fine temporal scales
simultaneously across wide spectral bands. &lt;BR /&gt; Aims: I present a
spectroscopic snapshot imaging (0.5 s, 160 kHz resolution) study of a
type-III burst event across the 80-200 MHz band. By modelling the
temporal variability of the source sizes and intensity at every
observation frequency, the characteristics of coronal turbulence are
studied across a heliocentric height range of 1.54-1.75 R&lt;SUB&gt;&lt;/SUB&gt;.
&lt;BR /&gt; Methods: To understand the morphological evolution of the type-
III source, a 2D Gaussian fitting procedure is used. The observed trends
in the source area and integrated flux density are analysed in the
framework of theoretical and data-driven models. &lt;BR /&gt; Results: The
strength of density fluctuations (N/N) in the corona is derived as a
function of height (R). Combined with the archival low frequency data,
N/N values across 1.5-2.2 R&lt;SUB&gt;&lt;/SUB&gt; agree within a few factors.
The burst decay time (&lt;SUB&gt;decay&lt;/SUB&gt;) and the full width at half
maximum of the source showed a power-law dependence with frequency,
roughly consistent with the results from data-driven models. However,
the values of &lt;SUB&gt;decay&lt;/SUB&gt; across frequencies turned out higher
than the expected trend. The intrinsic sizes of the burst source were
derived, correcting for scatter broadening. This roughly matched the
expected size of flux tubes at the coronal heights explored. I also
report the observation of an intrinsic anti-phased pulsation in the area
and flux density of the source.</description>
</item>
<item>
<title> A Machine Learning Perspective</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SpWea..1902794S</link>
<description>Several techniques have been developed in the last two decades to
forecast the occurrence of Solar Proton Events (SPEs), mainly based on
the statistical association between the &gt;10 MeV proton flux and
precursor parameters. The Empirical model for Solar Proton Events Real
Time Alert (ESPERTA; Laurenza et al., 2009, &lt;A href="https://doi.org/10.
1029/2007sw000379"&gt;https://doi.org/10.1029/2007sw000379&lt;/A&gt;) provides a
quite good and timely prediction of SPEs after the occurrence of M2
soft x-ray (SXR) bursts, by using as input parameters the flare
heliolongitude, the SXR and the 1 MHz radio fluence. Here, we
reinterpret the ESPERTA model in the framework of machine learning and
perform a cross validation, leading to a comparable performance.
Moreover, we find that, by applying a cut-off on the M2 flares
heliolongitude, the False Alarm Rate (FAR) is reduced. The cut-off is
set to E20 where the cumulative distribution of M2 flares associated
with SPEs shows a break which reflects the poor magnetic connection
between the Earth and eastern hemisphere flares. The best performance is
obtained by using the SMOTE algorithm, leading to probability of
detection of 0.83 and a FAR of 0.39. Nevertheless, we demonstrate that a
relevant FAR on the predictions is a natural consequence of the sample
base rates. From a Bayesian point of view, we find that the FAR
explicitly contains the prior knowledge about the class distributions.
This is a critical issue of any statistical approach, which requires to
perform the model validation by preserving the class distributions
within the training and test datasets.</description>
</item>
<item>
<title> Forecasting the Remaining Duration of an Ongoing Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SpWea..1902754R</link>
<description>The solar X-ray irradiance is significantly heightened during the course
of a solar flare, which can cause radio blackouts due to ionization of
the atoms in the ionosphere. As the duration of a solar flare is not
related to the size of that flare, it is not directly clear how long
those blackouts can persist. Using a random forest regression model
trained on data taken from X-ray light curves, we have developed a
direct forecasting method that predicts how long the event will remain
above background levels. We test this on a large collection of flares
observed with GOES-15, and show that it generally outperforms simple
linear regression, giving a median error of less than 2 min for the
approximate end time of a flare. This random forest model is
computationally light enough to be performed in real time, allowing for
the prediction to be made during the course of a flare.</description>
</item>
<item>
<title> Particle-in-cell simulations of the plasma emission in type III solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SSPMA..51j9611L</link>
<description>Not Available</description>
</item>
<item>
<title> Detection and mitigation of RFI in SBRS observation data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..195Q</link>
<description>In view of the inconsistency of channel gains and a large amount of
interference noise in Solar Broadband Radio Spectrometer (SBRS)
observation data, they will seriously affect the analysis of SBRS data.
In this paper, a method of Radio Frequency Interference (RFI) detection
and mitigation for SBRS observation data is reported. Firstly, the SBRS
observation data are preprocessed, a part of the observation data was
selected to calculate the mean and variance to achieve the normalization
of the entire observation data, which can avoid the influence of strong
noise on the normalization result. Furthermore, we proposed an adaptive
threshold RFI detection method based on fusion wavelet transform
reconstruction and an RFI elimination method based on neighborhood
weighted filling. It is worth mentioning that to detect RFI interference
signals of different magnitudes, we adopted an iterative approach to the
RFI detection and mitigation process. Through qualitative analysis of
real observation data and quantitative analysis of simulated data, it is
shown that the method proposed in this paper can effectively eliminate
RFI in SBRS observation data, and improve the quality of observation
data for further scientific analysis.</description>
</item>
<item>
<title> The first detection of the solar U+III association with an antenna prototype for the future lunar observatory</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..187S</link>
<description>We report about observations of solar U+III bursts on 2020 June 5 by
means of a new active antenna designed to receive radiation in 4-70 MHz.
This instrument can serve as a prototype of the ultra-long-wavelength
radio telescope for observations on the farside of the Moon. Our
analysis of experimental data is based on simultaneous records obtained
with the antenna arrays GURT and NDA in high frequency and time
resolution, e-Callisto network as well as by using the space-based
observatories STEREO and WIND. The results from this observational study
confirm the model of Reid and Kontar.</description>
</item>
<item>
<title> ORFEES - a radio spectrograph for the study of solar radio bursts and space weather applications</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JSWSC..11...57H</link>
<description>Radio bursts are sensitive tracers of non-thermal electron populations
in the solar corona. They are produced by electron beams and shock waves
propagating through the corona and the heliosphere, and by trapped
electron populations in coronal mass ejections (CMEs) and in quiescent
active regions. Combining space-borne and ground-based radio
spectrographs allows one to track disturbances between the low corona,
near or at the sites of particle acceleration, and the spacecraft. Radio
observations are, therefore, a significant tool in probing the solar
origin of heliospheric disturbances, which is a central research topic
as witnessed by the Parker Solar Probe and Solar Orbiter missions. The
full scientific return of these projects needs vigorous ground-based
support, which at radio wavelengths covers altitudes up to about a solar
radius above the photosphere. Besides research in solar and heliospheric
physics, monitoring solar radio bursts also supports space weather
services. On occasion, radio bursts can themselves be a space weather
hazard. The Nanay radio astronomy station in central France has a long
tradition of monitoring radio emission at decimetre-to-meter
wavelengths. This article describes the radio spectrograph ORFEES
(Observations Radiospectrographiques pour FEDOME et l'Etude des
Eruptions Solaires). It observes the whole-Sun flux density between 144
and 1004 MHz, pertaining to regions between the low corona and about
half a solar radius above the photosphere. ORFEES results from a
partnership between Observatoire de Paris and the French Air Force,
which operates the experimental space weather service FEDOME. The
primary use of the instrument at the Paris Observatory is astrophysical
observation. Low-resolution data with rapid availability are presently
produced for the French Air Force. Similar information can be made
available to a broader range of space weather service providers. This
article gives an overview of the instrument design and access to the
data and shows a few illustrative observations.</description>
</item>
<item>
<title> Impact of solar and geomagnetic activities on total column ozone in China</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JASTP.22305738C</link>
<description>Dynamic impacts on sunspot number (SSN), solar radio flux at 10.7 cm
(F10.7) and amplitude antipodal (aa) index influencing long-term trends
of total column ozone (TCO) obtained from three stations; Xianghe
(39.975N, 116.37E), Linan (30.3N, 119.73E), and Kunming (25.03N,
102.683E) over China have been studied. Descriptive, regression and
neural network training techniques are used from 1980 to 2018. The
annual mean TCO concentrations are 333.61  1.15 DU, 280.87  0.58 DU,
and 260.33  0.49 DU at Xianghe, Linan, and Kunming stations,
respectively. The mean monthly peak TCO values are ~417.13 DU (March),
316.79 DU (April), and 291.03 DU (April) at Xianghe, Linan, and Kunming,
respectively. Irrespective of the decreasing seasonal trend during
spring at Xianghe, the springtime TCO amount is greater than the TCO
values in other seasons at all stations. Our analyses show direct
forcing of SSN, F10.7, and aa on TCO changes throughout the different
periods considered. At Xianghe, the value of r ranges between 0.09 and
0.48 and the p-value &lt; 0.05 whereas the most contributing factor is aa
index (about 40 %) to ozone enhancement. There is a dramatic improvement
of the impact of the quasi-biennial oscillation (QBO)-modulated (70 hPa
and 50 hPa) SSN, F10.7, and aa on TCO during winter in all the stations
particularly the aa, which appreciated from ~40 % to 66 %. Ozone is
affected negatively during descending and low solar cycle (SC) phases
whereas it enhances during ascending and high SC phases with 30 hPa QBO
as the most active force of enhancement. Our finding is a profitable
tool for atmospheric model development, which could be used to predict
future phenomena.</description>
</item>
<item>
<title> equatorial studies</title>
<link>https://ui.adsabs.harvard.edu/abs/2021InJPh..95.1967A</link>
<description>Various solar flares and coronal mass ejections were associated with the
intense solar activity located at RGN 2673 based on NASA's record. The
effects of solar activity change the condition of the ionosphere leading
to fading or loss of signal. The duration of signal loss may last for a
few minutes or more than an hour depending on the scale of the solar
flare. Having said that, such an event disturbed the HF (high-frequency)
radio communication with high sunspot number (SSn) from 4th to 10th
September 2017. The R1-R2 (minor moderate) and R3 (strong) radio
blackouts occurred on 4th, 6th and 10th of September 2017. Therefore,
this study aims to investigate and analyse the effects of intense solar
activity towards HF radio communication based on the observations of
Jicamarca (11.571 S, 76.525 W) and Fortaleza (3.7327 S, 38.527 W)
ionosondes located at low latitudes and an amateur radio application
executed at a ground station in UKM (2.92 N, 101.77 E). According to
the data coverage from both the ionosondes on the specific dates, an
increased value of critical frequency of F2 layer (foF2) during HF radio
blackout was identified to be associated with high SSn. The X-class
flares recorded on all three dates in September 2017 caused the foF2 to
enhance with recovery times of tens of minutes to hours, based on the
decay time of the flare. Moreover, HF selection for amateur radios
experienced an increase of more than 8 MHz during the day compared to
around 7 MHz on a normal day. This result is essential for frequency
planning, especially for HF amateur radio users in and around Malaysia.</description>
</item>
<item>
<title> A Case Study</title>
<link>https://ui.adsabs.harvard.edu/abs/2021GeoRL..4895138L</link>
<description>Combining in situ measurements of energetic electrons and remote sensing
observations of hard X-rays and type III radio bursts, we examine the
release times of energetic electrons in the July 23, 2016 event. We find
that the releases of in situ energetic electrons from the Sun are
delayed from those electrons that are responsible for the hard X-rays.
We further find that the release time of in situ electrons is a function
of electron energy. Under the assumption that the acceleration mechanism
for the upward propagating electrons is of Fermi-type and is controlled
by an energy-dependent diffusion coefficient, we fit these release times
by a simple functional form, related to the turbulence spectral index.
Implications of our study on the underlying electron acceleration
mechanisms and the magnetic reconnection process in solar flares are
discussed. Our results demonstrate the power of the recently developed
fractional velocity dispersion analysis (FVDA) method in solar flare
studies.</description>
</item>
<item>
<title> An analysis based on 19-year measurements in Boston, USA</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ER....20111532Z</link>
<description>Solar radiation plays a major role in atmospheric photochemistry,
contributing to the formation and growth of ultrafine particles (PN). PN
affect global Earth's radiation balance, climate system, and human
health. However, the impact of solar activity on ambient PN remains
unclear. In this study, we investigated the associations between daily
ambient PN concentrations [particle number (PN)/cm&lt;SUP&gt;3&lt;/SUP&gt;] and
solar radio flux [solar activity index (F&lt;SUB&gt;10.7&lt;/SUB&gt; in sfu)] as a
solar activity parameter, shortwave solar radiation (SWR), daylight time
(DL), cosmic ray-induced ionization (CRII), and air pollution
[PM&lt;SUB&gt;2.5&lt;/SUB&gt;, black carbon (BC) and SO&lt;SUB&gt;2&lt;/SUB&gt;] over a 19-year
period in Boston, MA. We used generalized additive models adjusted for
local environmental conditions. We found that F&lt;SUB&gt;10.7&lt;/SUB&gt; was the
strongest predictor for daily PN concentrations over all time lags (0-28
days of lags) and seasons. The effects were higher in winter and fall.
In winter, an interquartile (IQR) of 60 sfu F&lt;SUB&gt;10.7&lt;/SUB&gt;
corresponded to an increase of 5770 PN/cm&lt;SUP&gt;3&lt;/SUP&gt; in the day of PN
collection. In fall, an IQR of 75.5 sfu F&lt;SUB&gt;10.7&lt;/SUB&gt; was associated
with an increase of 5429 PN/cm&lt;SUP&gt;3&lt;/SUP&gt;. The effects of
F&lt;SUB&gt;10.7&lt;/SUB&gt; on PN concentrations were slightly greater when the
models were adjusted for air pollution. In summer, ambient PN
concentrations were statistically significantly associated with
F&lt;SUB&gt;10.7&lt;/SUB&gt;, SWR, and BC, with the strongest association found for
PN and BC in the day of PN collection. Unlike the effects of
F&lt;SUB&gt;10.7&lt;/SUB&gt;, SWR and local pollutants on PN concentrations, DL and
CRII were negatively associated with ambient PN in the analyses. These
findings suggest that solar activity may have a significant impact on
daily ambient PN concentrations that affect the Earth's climate system
and human health.</description>
</item>
<item>
<title> Harmonic Maser Emissions from Electrons with Loss-cone Distribution in Solar Active Regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...920L..40N</link>
<description>Electron cyclotron maser emission (ECME) is regarded as a plausible
source for coherent radio radiations from solar active regions (e.g.,
solar radio spikes). In this Letter, we present a 2D3V fully kinetic
electromagnetic particle-in-cell simulation to investigate the wave
excitations and subsequent nonlinear processes induced by the energetic
electrons in the loss-cone distribution. The ratio of the plasma
frequency to the electron gyrofrequency &lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt; is
set to 0.25, adequate for solar active region conditions. As a main
result, we obtain strong emissions at the second-harmonic X mode (X2).
While the fundamental X mode (X1) and the Z mode are amplified directly
via the electron cyclotron maser instability, the X2 emissions can be
produced by nonlinear coalescence between two Z modes and between Z and
X1 modes. This represents a novel generation mechanism for the harmonic
emissions in plasmas with a low value of &lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;,
which may resolve the escaping difficulty of explaining solar radio
emissions with the ECME mechanism.</description>
</item>
<item>
<title> Wave Excitation by Power-law-Distributed Energetic Electrons with Pitch-angle Anisotropy in the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...920..147Z</link>
<description>Radio waves from the Sun are emitted, as a rule, due to energized
electrons. Observations infer that the related energized electrons
follow (negative) power-law velocity distributions above a break
velocity U&lt;SUB&gt;b&lt;/SUB&gt;. They might also distribute anisotropically in
the pitch-angle space. To understand radio wave generation better, we
study the consequences of anisotropic power-law-distributed energetic
electrons in current-free collisionless coronal plasmas utilizing
2.5-dimensional particle-in-cell simulations. We assume that the
velocity distribution f&lt;SUB&gt;u&lt;/SUB&gt; of the energized electrons follows a
plateau (f&lt;SUB&gt;u&lt;/SUB&gt;/u = 0) and a power-law distribution with
spectral index  for velocities below and above U&lt;SUB&gt;b&lt;/SUB&gt;,
respectively. In the pitch-angle space, these energized electrons are
spread around a center &lt;SUB&gt;c&lt;/SUB&gt; = 0.5. We found that the energetic
plateau-power-law electrons can more efficiently generate coherent waves
if the anisotropy of their pitch-angle distribution is sufficiently
strong, i.e., a small pitch-angle spread &lt;SUB&gt;s&lt;/SUB&gt;. The break
velocity U&lt;SUB&gt;b&lt;/SUB&gt; affects the excitation dominance between the
electrostatic and electromagnetic waves: for larger U&lt;SUB&gt;b&lt;/SUB&gt;
electrostatic waves are mainly excited, while intermediate values of
U&lt;SUB&gt;b&lt;/SUB&gt; are required for an excitation dominated by
electromagnetic waves. The spectral index  controls the growth rate,
efficiency, saturation, and anisotropy of the excited electromagnetic
waves as well as the energy partition in different wave modes. These
excited electromagnetic waves are predominantly right-handed polarized,
in X- and Z-modes, as observed, e.g., in solar radio spikes.
Additionally about 90% of the kinetic energy loss of the energetic
electrons is dissipated, heating the ambient thermal electrons. This may
contribute to the coronal heating.</description>
</item>
<item>
<title> Insights from Snapshot Spectroscopic Radio Observations of a Weak Type I Solar Noise Storm</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...920...11M</link>
<description>We present a high-fidelity snapshot spectroscopic radio imaging study of
a weak type I solar noise storm that took place during an otherwise
exceptionally quiet time. Using high-fidelity images from the Murchison
Widefield Array, we track the observed morphology of the burst source
for 70 minutes and identify multiple instances where its integrated flux
density and area are strongly anticorrelated with each other. The type I
radio emission is believed to arise due to electron beams energized
during magnetic reconnection activity. The observed anticorrelation is
interpreted as evidence for presence of MHD sausage wave modes in the
magnetic loops and strands along which these electron beams are
propagating. Our observations suggest that the sites of these small
scale reconnections are distributed along the magnetic flux tube. We
hypothesize that small scale reconnections produces electron beams which
quickly get collisionally damped. Hence, the plasma emission produced by
them span only a narrow bandwidth and the features seen even a few
mehahertz apart must arise from independent electron beams.</description>
</item>
<item>
<title> Space weather study through analysis of solar radio bursts detected by a single-station CALLISTO spectrometer</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AnGeo..39..945N</link>
<description>This article summarises the results of an analysis of solar radio bursts
(SRBs) detected by the Compound Astronomical Low-cost Low-frequency
Instrument for Spectroscopy and Transportable Observatory (CALLISTO)
spectrometer hosted by the University of Rwanda. The data analysed were
detected during the first year (2014-2015) of the instrument operation.
Using quick plots provided by the e-CALLISTO website, a total of 201
intense and well-separated solar radio bursts detected by the CALLISTO
station located in Rwanda, are found consisting of 4 type II, 175 type
III and 22 type IV radio bursts. It is found that all analysed type II
and  37 % of type III bursts are associated with impulsive solar
flares, while the minority ( 13 %) of type IV radio bursts are
associated with solar flares. Furthermore, all type II radio bursts are
associated with coronal mass ejections (CMEs),  44 % of type III bursts
are associated with CMEs, and the majority ( 82 %) of type IV bursts
were accompanied by CMEs. With aid of the atmospheric imaging assembly
(AIA) images on board the Solar Dynamics Observatory (SDO), the location
of open magnetic field lines of non-flare-associated type III radio
bursts are shown. The same images are used to show the magnetic loops in
the solar corona for type IV radio bursts observed in the absence of
solar flares and/or CMEs. Findings from this study indicate that
analysis of SRBs that are observed from the ground can provide a
significant contribution to the early diagnosis of solar transients
phenomena, such as solar flares and CMEs, which are major drivers of
potential space weather hazards.</description>
</item>
<item>
<title> Trends and characteristics of high-frequency type II bursts detected by CALLISTO spectrometers</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..68.3464U</link>
<description>Solar radio type II bursts serve as early indicators of incoming geo-
effective space weather events such as coronal mass ejections (CMEs). In
order to investigate the origin of high-frequency type II bursts (HF
type II bursts), we have identified 51 of them (among 180 type II bursts
from SWPC reports) that are observed by ground-based Compound
Astronomical Low-cost Low-frequency Instrument for Spectroscopy and
Transportable Observatory (CALLISTO) spectrometers and whose upper-
frequency cutoff (of either fundamental or harmonic emission) lies in
between 150 MHz-450 MHz during 2010-2019. We found that 60% of HF type
II bursts, whose upper-frequency cutoff  300 MHz originate from the
western longitudes. Further, our study finds a good correlation (~ 0.73)
between the average shock speed derived from the radio dynamic spectra
and the corresponding speed from CME data. Also, we found that analyzed
HF type II bursts are associated with wide and fast CMEs located near
the solar disk. In addition, we have analyzed the spatio-temporal
characteristics of two of these high-frequency type II bursts and
compared the derived from radio observations with those derived from
multi-spacecraft CME observations from SOHO/LASCO and STEREO
coronagraphs.</description>
</item>
<item>
<title> Correlation analyses between solar activity parameters and cosmic ray muons between 2002 and 2012 at high cutoff rigidity</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..68.2941M</link>
<description>Solar activity modulates cosmic ray (CR) flux with different magnitudes
on different time scales. Several investigations from locations with
different, mainly low, cutoff rigidity utilizing different solar
activity parameters have been carried out to characterize their
influence on the observed CR flux. &lt;P /&gt;In this study, the effect of
seven solar, interplanetary, and geophysical parameters on the secondary
CR muons has been investigated and established using correlation
analyses. Daily mean values of the CR data for the period between 2002
and 2012 were obtained from the King Abdulaziz City for Science and
Technology (KACST) muon detector, Riyadh, central Saudi Arabia (Rc =
14.4 GV). Considered parameters are sunspot number, radial component of
the interplanetary magnetic field, Kp index, solar radio emission flux
at 10.7 cm, Dst index, solar wind speed, and solar wind density. Same
analyses have been carried out using data from the Oulu neutron monitor
(Rc = 0.8 GV) for comparison purposes. &lt;P /&gt;Obtained results showed that
the intensities of the secondary CRs from both stations are
significantly correlated with the Dst index and plasma density, and
anti-correlated with the rest of the variables. These results are in
agreement with those obtained by several investigators. Magnitude and
strength of the correlations between the considered variables and CRs
were higher and stronger for the CR neutrons than the CR muons. These
findings may be due to the greater influence of seasonal variations on
the CR muons than on the CR neutrons. Additionally, the muon detector is
sensitive (due to its high cutoff rigidity) to higher-energy CR
particles, which are less affected by solar disturbances. &lt;P /&gt;Time-lag
cross-correlation analyses between the monthly mean CR values from both
stations and the monthly mean values of the considered variables were
conducted. Comparable results with the previous investigations were
found. &lt;P /&gt;Multivariable models using the seven parameters were
developed to predict the CR variations for both sites. For the data from
the KACST detector, the model was able to predict the measured data with
a correlation coefficient of 0.48 and a standard deviation of 0.60%. On
the other hand, the developed model for the Oulu neutron monitor has a
correlations coefficient of 0.77 and a standard deviation of 3.7%.</description>
</item>
<item>
<title> Multiwavelength observations of a metric type-II event</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...654A.112A</link>
<description>We have studied a complex metric radio event that originated in a
compact flare, observed with the ARTEMIS-JLS radiospectrograph on
February 12, 2010. The event was associated with a surge observed at 195
and 304  and with a coronal mass ejection observed by instruments on
board STEREO A and B near the eastern and western limbs respectively. On
the disk the event was observed at ten frequencies by the Nanay
Radioheliograph (NRH), in H by the Catania observatory, in soft X-rays
by GOES SXI and Hinode XRT, and in hard X-rays by RHESSI. We combined
these data, together with MDI longitudinal magnetograms, to get as
complete a picture of the event as possible. Our emphasis is on two
type-II bursts that occurred near respective maxima in the GOES light
curves. The first, associated with the main peak of the event, showed an
impressive fundamental-harmonic structure, while the emission of the
second consisted of three well-separated bands with superposed
pulsations. Using positional information for the type-IIs from the NRH
and triangulation from STEREO A and B, we found that the type-IIs were
associated neither with the surge nor with the disruption of a nearby
streamer, but rather with an extreme ultraviolet (EUV) wave probably
initiated by the surge. The fundamental-harmonic structure of the first
type-II showed a band split corresponding to a magnetic field strength
of 18 G, a frequency ratio of 1.95 and a delay of 0.230.65 s of the
fundamental with respect to the harmonic; moreover it became stationary
shortly after its start and then drifted again. The pulsations
superposed on the second type-II were broadband and had started before
the burst. In addition, we detected another pulsating source, also
before the second type-II, polarized in the opposite sense; the
pulsations in the two sources were out of phase and hence hardly
detectable in the dynamic spectrum. The pulsations had a measurable
reverse frequency drift of about 2 s&lt;SUP&gt;1&lt;/SUP&gt;.</description>
</item>
<item>
<title> Generation of interplanetary type II radio emission</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...654A..64J</link>
<description>Context. Coronal mass ejections (CMEs) are eruptive phenomena that can
accelerate energetic particles and drive shock waves. The CME-driven
shocks propagate from the low corona to interplanetary space. The radio
emission that results from fast electrons energised by shock waves are
called type II bursts. This radio emission can provide information on
the physical properties of the shock and its evolution as it travels
through the corona and interplanetary space. &lt;BR /&gt; Aims: We present a
comprehensive analysis of the shock wave associated with two type II
radio bursts observed on 27 September 2012. The aim of the study is to
isolate and understand the shock wave properties necessary for
accelerating electrons, leading to the production of the radio emission.
&lt;BR /&gt; Methods: First, we modelled the 3D expansion of the shock wave by
exploiting multi-viewpoint reconstruction techniques based on extreme
ultraviolet imaging. The physical properties of the shock front were
then deduced by comparing the triangulated 3D expansion with properties
of the background corona provided by a 3D magnetohydrodynamic model. The
radio triangulation technique provided the location of radio source on
the surface of the modelled wave in order to compare radio sources with
the shock properties. &lt;BR /&gt; Results: This study is focused on the
temporal evolution of the shock wave parameters and their role in the
generation of radio emission. Results show a close relationship between
the shock wave strength and its geometry. We deduce from this analysis
that there may be several mechanisms at play that generally contribute
to the generation of radio emission. &lt;BR /&gt; Conclusions: The comparison
between the reconstructed sources of radio emission and the ambient
shock wave characteristics reveals the complex relationship between
shock parameters and show how they can influence the morphology of the
observed type II radio emission.</description>
</item>
<item>
<title> On the Magnetoacoustic Waves and Physical Conditions in Zebra Radio Sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..139Y</link>
<description>Analysis of the solar radio zebra-pattern (ZP) spectrum for the burst on
21 June 2011 has shown that the frequencies corresponding to the stripes
of this ZP experience quasiperiodic oscillations relative to some
average values. The period of such oscillations, expressed in the number
of the ZP stripes, is 2.41 0.21 , and expressed in frequencies, it is
(5.00 0.68 ) MHz. The change in the period of oscillations with time
anticorrelates with the amplitude of the oscillations. The values of the
harmonic numbers for the corresponding bands are given, and thus the
magnetic-field strength is also estimated on the basis of the theory of
double plasma resonance (DPR). In addition, a possible change in the
L&lt;SUB&gt;bh&lt;/SUB&gt;/L&lt;SUB&gt;nh&lt;/SUB&gt; parameter in the ZP-generation region is
taken into account (L&lt;SUB&gt;bh&lt;/SUB&gt; and L&lt;SUB&gt;nh&lt;/SUB&gt; respectively are
the magnetic-field and density scales). Calculations of the frequency-
drift rate, carried out using an improved method for its determination,
have shown that the drift values (3 -8 MHzs&lt;SUP&gt;1&lt;/SUP&gt;) are in
accordance with Kaneda et al. (Astrophys. J. Lett.855, L29, 2018). By
using two density models of the solar atmosphere, the wavelength of
these oscillations has also been determined. For the model presented by
Aschwanden (Space Sci. Rev.101, 1, 2002), the wavelength is about 1370
km while for the barometric density model, the wavelength is about 4650
km. The wavelength increases with time; for example, in the first model,
the wavelength increases with time from 1200 to 1490 km. The calculated
kink and sausage wave velocities turned out to be significantly lower
than the observed ones. The reason for this discrepancy requires
additional analysis.</description>
</item>
<item>
<title> Kodaikanal Solar Observatory Radio Spectrograph</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..132B</link>
<description>The Indian Institute of Astrophysics (IIA) has commissioned a low
frequency (&lt;100 MHz) spectrograph at its Kodaikanal Solar Observatory
(KSO) for coordinated observations of transients in the solar atmosphere
with other existing optical observing facilities there. The hardware
set-up and initial observations are presented. The availability of
different instruments in the same observatory helps to quickly plan and
jointly observe the energetic phenomena and their signatures in all the
three major atmospheric regions of the Sun, i.e. photosphere,
chromosphere and corona.</description>
</item>
<item>
<title> Long-term trends of the F2-region at mid-latitudes in the Southern Hemisphere</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JASTP.22005683S</link>
<description>The long-term variations in f&lt;SUB&gt;o&lt;/SUB&gt;F2 at Hobart (52.88S,
147.32E), Canberra (35.28S, 149.13 E) and Christchurch (43.53S,
172.64E) stations, located in the mid-latitude zone in the Southern
Hemisphere were analyzed using 1947-2006 years of the data. The
saturation, solar and geomagnetic activity and seasonal effects were
removed mainly by using 12-month running mean, linear and multiple
regression (twofold regression) methods to find possible signatures of
climate change in long-term trends in the f&lt;SUB&gt;o&lt;/SUB&gt;F2. The solar
activity proxies, sunspot number, R&lt;SUB&gt;Z,&lt;/SUB&gt; and F10.7 solar radio
flux were used in regression to find the f&lt;SUB&gt;o&lt;/SUB&gt;F2 residuals at
midday (12 LT) and midnight (00 LT) of the stations. The long-term
trends obtained at 12 LT are more significant and consistent with the
model results. The trends estimated with F10.7 solar flux are negative
and the trends estimated with R&lt;SUB&gt;Z&lt;/SUB&gt; are positive (small and not
significant). The f&lt;SUB&gt;o&lt;/SUB&gt;F2 decreased by 0.1-0.4 MHz for the 5
solar cycles period which could be mainly due to enhanced CO&lt;SUB&gt;2&lt;/SUB&gt;
in the troposphere that is cooling the upper atmosphere. Further
research is needed to see if the f&lt;SUB&gt;o&lt;/SUB&gt;F2 trends are also
affected by other factors such as thermospheric winds, neutral
constituents, the secular variation of Earth's magnetic field, long-term
changes in stratospheric ozone, solar and geomagnetic activities.</description>
</item>
<item>
<title> Model of the E-Layer Critical Frequency for the Auroral Region</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ge&amp;Ae..61..713D</link>
<description>A new foE model for the auroral region is constructed; the model is
based on an analysis of the models of auroral electron precipitations,
the boundaries of the discrete and diffusive aurora, the main
ionospheric trough, and measurements of the E-layer critical frequency
foE. The model is an analytical model. It consists of solar
(foE&lt;SUB&gt;sol&lt;/SUB&gt;) and auroral (foE&lt;SUB&gt;avr&lt;/SUB&gt;) components. The
solar component of the model does not depend of geomagnetic activity. It
depends on solar activity via the F index, which is determined by the
solar radio emission flux at a wavelength of 10.7 cm over the previous
day and three solar rotations. The auroral component of the model does
not depend of solar activity. It depends on geomagnetic activity via the
effective Kp* index, which takes into account the prehistory of changes
in this activity. The model indirectly takes into account the dependence
of the relative contribution of foE&lt;SUB&gt;sol&lt;/SUB&gt; and foE&lt;SUB&gt;avr&lt;/SUB&gt;
to the total foE value on the difference in the heights of the maxima of
these model components via the addition of a coefficient. The model
qualitatively takes into account the effect of the winter anomaly in
foE&lt;SUB&gt;avr&lt;/SUB&gt; via the addition of a function. It is found that the
errors of the new foE model in the auroral region at the nighttime hours
are much lower than those in the international IRI model (with the
STORM-E option) for both moderate and high geomagnetic activity. For
example, the comparison with data from ionospheric stations shows that
the IRI model underestimates foE in these conditions by approximately a
factor of 2 on average. The average shift in foE relative to the
experimental data in the new model does not exceed 20%.</description>
</item>
<item>
<title> Auto Recognition of Solar Radio Bursts Using the C-DCGAN Method</title>
<link>https://ui.adsabs.harvard.edu/abs/2021FrP.....9..428Y</link>
<description>Solar radio bursts can be used to study the properties of solar
activities and the underlying coronal conditions on the basis of the
present understanding of their emission mechanisms. With the
construction of observational instruments, around the world, a vast
volume of solar radio observational data has been obtained. Manual
classifications of these data require significant efforts and human
labor in addition to necessary expertise in the field.
Misclassifications are unavoidable due to subjective judgments of
various types of radio bursts and strong radio interference in some
events. It is therefore timely and demanding to develop techniques of
auto-classification or recognition of solar radio bursts. The latest
advances in deep learning technology provide an opportunity along this
line of research. In this study, we develop a deep convolutional
generative adversarial network model with conditional information
(C-DCGAN) to auto-classify various types of solar radio bursts, using
the solar radio spectral data from the Culgoora Observatory (1995, 2015)
and the Learmonth Observatory (2001, 2019), in the metric decametric
wavelengths. The technique generates pseudo images based on available
data inputs, by modifying the layers of the generator and discriminator
of the deep convolutional generative adversarial network. It is
demonstrated that the C-DCGAN method can reach a high-level accuracy of
auto-recognition of various types of solar radio bursts. And the issue
caused by inadequate numbers of data samples and the consequent over-
fitting issue has been partly resolved.</description>
</item>
<item>
<title> Catalog of Long-term Transient Sources in the First 10 yr of Fermi-LAT Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJS..256...13B</link>
<description>We present the first Fermi Large Area Telescope (LAT) catalog of long-
term -ray transient sources (1FLT). This comprises sources that were
detected on monthly time intervals during the first decade of Fermi-LAT
operations. The monthly timescale allows us to identify transient and
variable sources that were not yet reported in other Fermi-LAT catalogs.
The monthly data sets were analyzed using a wavelet-based source
detection algorithm that provided the candidate new transient sources.
The search was limited to the extragalactic regions of the sky to avoid
the dominance of the Galactic diffuse emission at low Galactic
latitudes. The transient candidates were then analyzed using the
standard Fermi-LAT maximum likelihood analysis method. All sources
detected with a statistical significance above 4 in at least one
monthly bin were listed in the final catalog. The 1FLT catalog contains
142 transient -ray sources that are not included in the 4FGL-DR2
catalog. Many of these sources (102) have been confidently associated
with active galactic nuclei (AGNs): 24 are associated with flat-spectrum
radio quasars, 1 with a BL Lac object, 70 with blazars of uncertain
type, 3 with radio galaxies, 1 with a compact steep-spectrum radio
source, 1 with a steep-spectrum radio quasar, and 2 with AGNs of other
types. The remaining 40 sources have no candidate counterparts at other
wavelengths. The median -ray spectral index of the 1FLT-AGN sources is
softer than that reported in the latest Fermi-LAT AGN general catalog.
This result is consistent with the hypothesis that detection of the
softest -ray emitters is less efficient when the data are integrated
over year-long intervals.</description>
</item>
<item>
<title> Implications of Flat Optically Thick Microwave Spectra in Solar Flares for Source Size and Morphology</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...919...44S</link>
<description>The study aims to examine the spectral dynamics of the low-frequency,
optically thick gyrosynchrotron microwave emission in solar flares to
determine the characteristics of the emitting source. We present the
high-resolution spectra of a set of microwave bursts observed by the
Expanded Owens Valley Solar Array (EOVSA) during its commissioning phase
in the 2.5-18 GHz frequency range with 1 second time resolution. Out of
the 12 events analyzed in this study, nine bursts exhibit a direct
decrease with time in the optically thick spectral index &lt;SUB&gt;l&lt;/SUB&gt;,
an indicator of source morphology. Particularly, five bursts display a
"flat" spectrum (&lt;SUB&gt;l&lt;/SUB&gt;  1.0) compared to that expected for a
homogeneous/uniform source (&lt;SUB&gt;l&lt;/SUB&gt;  2.9). These flat spectra at
low frequencies (&lt;10 GHz) can be defined as the emission from a
spatially inhomogeneous source with a large area and/or with multiple
emission components. In a subset of six events with partial cross-
correlation data, both the events with flat spectra show a source size
of ~120 at 2.6-3 GHz. Modeling based on inhomogeneity supports the
conclusion that multiple discrete sources can only reproduce a flat
spectrum. We report that these flat spectra appear predominantly in the
decay phase and typically grow flatter over the duration in most of the
bursts, which indicates an increasing inhomogeneity and complexity of
the emitting volume as the flare progresses. This large volume of flare
emission filled with the trapped energetic particles is often invisible
in other wavelengths, like hard X-rays, presumably due to the
collisionless conditions in these regions of low ambient density and
magnetic field strength.</description>
</item>
<item>
<title> Radio, X-Ray, and Extreme-ultraviolet Observations of Weak Energy Releases in the "Quiet" Sun</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...918L..18R</link>
<description>We analyzed ground-based low frequency (&lt;100 MHz) radio spectral and
imaging data of the solar corona obtained with the facilities in the
Gauribidanur observatory during the same time as the very weak soft
X-ray flares (sub-A-class, flux &lt;10&lt;SUP&gt;-7&lt;/SUP&gt;Wm&lt;SUP&gt;-2&lt;/SUP&gt; in the
1-8  wavelength range) from the quiet Sun observed with the X-ray Solar
Monitor (XSM) on board Chandrayaan-2 during the recent solar minimum.
Nonthermal type I radio burst activity was noticed in close temporal
association with the X-ray events. The estimated brightness temperature
(T&lt;SUB&gt;b&lt;/SUB&gt;) of the bursts at a typical frequency like 80 MHz is 3 
10&lt;SUP&gt;5&lt;/SUP&gt; K. Extreme-ultraviolet (EUV) observations at 94  with
the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics
Observatory (SDO) revealed a brightening close to the same location and
time as the type I radio bursts. As far as we know reports of
simultaneous observations of X-ray and/or EUV counterpart to weak
transient radio emission at low frequencies from the quiet Sun in
particular are rare. Considering this and the fact that low frequency
radio observations are sensitive to weak energy releases in the solar
atmosphere, the results indicate that coordinated observations of
similar events would be useful to understand transient activities in the
quiet Sun.</description>
</item>
<item>
<title> Non-thermal Electron Energization During the Impulsive Phase of an X9.3 Flare Revealed by Insight-HXMT</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...918...42Z</link>
<description>The X9.3 flare SOL20170906T11:55 was observed by the CsI detector aboard
the first Chinese X-ray observatory Hard X-ray Modulation telescope
(Insight-HXMT). Using the wavelets method, we report 22 s quasiperiodic
pulsations during the impulsive phase. The spectra from 100 keV to 800
keV show the evolution with the gamma-ray flux of a power-law photon
index from ~1.8 before the peak, ~2.0 around the flare peak, to ~1.8
again. The gyrosynchrotron microwave spectral analysis reveals a 36"6 
0"6 radius gyrosynchrotron source with mean transverse magnetic field
around 608.2 Gauss. The penetrated 10 keV non-thermal electron density
is about 10&lt;SUP&gt;6.7&lt;/SUP&gt; cm&lt;SUP&gt;-3&lt;/SUP&gt; at peak time. The magnetic
field strength followed the evolution of high-frequency radio flux.
Further gyrosynchrotron source modeling analysis implies that there
exists a quite steady gyrosynchrotron source, and the non-thermal
electron density and transverse magnetic field evolution are similar to
higher-frequency light curves. The temporal spectral analysis reveals
that those non-thermal electrons are accelerated by repeated magnetic
reconnection, likely from a lower corona source.</description>
</item>
<item>
<title> Analysis of Type II and Type III Radio Bursts Associated with SEPs from Non-Interacting/Interacting Radio-Loud CMEs</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ap.....64..327K</link>
<description>We analyze radio bursts observed in events with interacting/non-
interacting CMEs that produced major SEPs (I&lt;SUB&gt;p&lt;/SUB&gt; &gt; 10 MeV) from
April 1997 to December 2014. We compare properties of meter (m),
decahectometer (DH) type II and DH type III bursts, and time lags for
interacting-CME-associated (IC) events and non-interacting-CME-
associated (NIC) events. About 70% of radio emissions were observed in
events of both types from meters to kilometers. We found high
correlations between the drift rates and mid-frequencies of type II
radio bursts calculated as the mean geometric between their starting and
ending frequencies for both NIC and IC-associated events (correlation
coefficient R&lt;SUP&gt;2&lt;/SUP&gt; = 0.98, power-law index  = 1.68  0.16 and
R&lt;SUP&gt;2&lt;/SUP&gt; = 0.93,  = 1.64  0.19 respectively). We also found a
correlation between the frequency drift rates of DH type II bursts and
space speeds of CMEs in NIC-associated events. The absence of such
correlation for IC-associated events confirms that the shock speeds
changed in CME-CME interactions. For the events with western source
locations, the mean peak intensity of SEPs in IC-associated events is
four times larger than that in NIC-associated SEP events. From the mean
time lags between the start times of SEP events and the start of m, DH
type II, and DH type III radio bursts, we inferred that particle
enhancements in NIC-associated SEP events occurred earlier than in IC-
associated SEP events. The difference between NIC events and IC events
in the mean values of parameters of type II and type III bursts is
statistically insignificant.</description>
</item>
<item>
<title> Response and periodic variation of total atmospheric ozone to solar activity over Mountain Waliguan</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..68.2257O</link>
<description>Modern-Era Retrospective Analysis for Research and Applications,
Version-2 (MERRA-2) total column ozone (TCO) data from 1980 to 2018 and
ground based TCO data were used to investigate its responses to periodic
variations concerning stratospheric dynamics such as tropopause heights
and Quasi-Biennial Oscillations (QBO), and solar activity signatures of
Magnesium II core-to-wing ratio (Mg II) and F10.7 cm solar radio flux
(F10.7) observed over Mountain (Mt.) Waliguan (36.17N, 100.53E),
China. Cross-correlation and wavelet analyses were used for carrying out
the investigation. The MgII and F10.7 show a periodicity of around an
11-year solar cycle (SC) while the TCO trend is though periodic and it
does not exhibit one to one correspondence with the 11-year SC. The
highest value in TCO is 355.7 DU noted in February (1982) whereas, the
lowest value of TCO is 256.02 DU in October (1988) during the entire
study period. The average value in TCO is 291.17  0.94 DU with an
amplitude of variation of 99.68 DU (~28%). The trend of TCO depicts a
persistent distinct seasonal pattern with maxima in winter/spring
(December through April) and minima in summer/autumn (August through
November). The long-term variability shows a notable decreasing trend in
TCO by ~30%, 13%, and 5% per decade for SCs 21-23, where SC 24
represents an increasing trend of ~1% per decade. Hence, this
illustrates the significant recovery of TCO over Mt. Waliguan, China
which is as a result of the reduction of the ozone depletion agents
arising as a positive outcome of the implementation of the Montreal
regulatory policy. From wavelet analysis, the F10.7, MgII, tropopause
height, QBO and TCO show a significant dominant periodicity of 10-12
months. It is concluded that the variations in mean TCO are strongly
correlated with variations of the F10.7 cm and Mg-II solar indices, and
the mean TCO responds rapidly to solar activity variations.</description>
</item>
<item>
<title> Growth of Radio Astronomy in India</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ARA&amp;A..59....1S</link>
<description>In this autobiographical account, I first describe my family, then
childhood and education in India. During 1953-55, I worked in the new
field of radio astronomy at the Division of Radiophysics of the
Commonwealth Scientific and Industrial Research Organisation in
Australia. During 1956-57, I worked at the Radio Astronomy Station of
Harvard University at Fort Davis, Texas, where I made observations of
solar radio bursts at decimeter wavelengths. I then joined Stanford
University as a graduate student in 1957. I contributed to the
successful operation of the Stanford Cross Antenna and then used it for
studying microwave radio emission from the Sun. I was awarded the Ph.D.
degree by Stanford University in 1960 and was then appointed as an
Assistant Professor for three years. With an urge to contribute to
evolving scientific endeavors in India, I joined the Tata Institute of
Fundamental Research (TIFR) at Mumbai, India, in April 1963. In my stay
of more than three decades at TIFR, I conceived of, and guided,
construction of two of the world's largest radio telescopes, namely the
Ooty Radio Telescope and the Giant Metrewave Radio Telescope. These
instruments have led to several outstanding contributions and
discoveries in the areas of radio galaxies, quasars, pulsars, and
cosmology.</description>
</item>
<item>
<title> Particle-in-cell simulation of plasma emission in solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...653A.169L</link>
<description>&lt;BR /&gt; Aims: The present study aims to shed light on our understanding
of the radiation processes of solar radio bursts associated with
nonthermal electron propagation in the corona and interplanetary space.
&lt;BR /&gt; Methods: We performed 2.5-dimensional particle-in-cell (PIC)
simulations to investigate the plasma emission excited by a relativistic
electron beam using different pitch angles in the magnetized plasma. &lt;BR
/&gt; Results: Langmuir waves at the fundamental and harmonic frequencies
were excited via the energy dissipation of the electron beam. For the
first time, the backward Langmuir waves up to the third harmonic
frequencies were reproduced in the cases of large pitch angles, likely
arising from the relecting and scattering of density fluctuations to the
Langmuir waves during electrom beam-plasma interaction. Electromagnetic
(EM) waves were generated via the mode conversion of electrostatic (ES)
waves and the nonlinear wave coupling. Specifically, the harmonic EM
emission comes from the coupling of forward and backward Langmuir waves,
namely, L + L'  2H, while the higher harmonic EM emissions generally
come from the coupling of the Langmuir wave and lower-order harmonic EM
wave, namely, L + (n  1)H  nH. When the electron beam exhibits a large
pitch angle, another possible mechanism for the third harmonic EM
emission might be the coalescence of three ES waves, namely, L + L' + L
 3H.</description>
</item>
<item>
<title> Statistical analysis of solar radio fiber bursts and relations with flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...653A..38W</link>
<description>Fiber bursts are a type of fine structure that frequently occurs in
solar flares. Although observations and theory of fiber bursts have been
studied for decades, their microphysical process, emission mechanism,
and especially the physical links with the flaring process still remain
unclear. We performed a detailed statistical study of fiber bursts
observed by the Chinese Solar Broadband Radio Spectrometers in Huairou
with high spectral-temporal resolutions in the frequency ranges of
1.102.06 GHz and 2.603.80 GHz during 20002006. We identify more than
900 individual fiber bursts in 82 fiber events associated with 48 solar
flares. From the soft X-ray observations of the Geostationary
Operational Environmental Satellite, we found that more than 40% of
fiber events occurred in the preflare and rising phases of the
associated solar flares. Most fiber events are temporally associated
with hard X-ray bursts observed by RHESSI or microwave bursts observed
by the Nobeyama Radio Polarimaters, which implies that they are closely
related to the nonthermal energetic electrons. The results indicate that
most fiber bursts have a close temporal relation with energetic
electrons. Most fiber bursts are strongly polarized, and their average
duration, relative bandwidth, and relative frequency-drift rate are
about 1.22 s, 6.31%, and 0.069 s&lt;SUP&gt;1&lt;/SUP&gt;. The average duration and
relative bandwidth of fiber bursts increase with solar flare class. The
fiber bursts associated with X-class flares have a significantly lower
mean relative frequency-drift rate. The average durations in the
postflare phase are clearly longer than the duration in the preflare and
rising phases. The relative drift rate in the rising phase is clearly
higher than that in preflare and postflare phases. The hyperbola
correlation of the average duration and the relative drift rate of the
fiber bursts is very interesting. These characteristics are very
important for understanding the formation of solar radio fiber bursts
and for revealing the nonthermal processes of the related solar flares.</description>
</item>
<item>
<title> A Search for the Counterparts of Quiet-Sun Radio Transients in Extreme Ultraviolet Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..131M</link>
<description>Nonthermal radio transients from the quiet Sun have been recently
discovered and it has been hypothesized using rough calculations that
they might be important for coronal heating. It is well realized that
energy calculations using coherent emissions are often subject to poorly
constrained parameters and hence have large uncertainties. However,
energy estimates using observations in the extreme ultraviolet (EUV) and
soft X-ray bands are routinely done and the techniques are pretty well
established. This work presents the first attempt to identify the EUV
counterparts of these radio transients and then use them to estimate the
energy deposited into the corona during the event. I show that the group
of radio transients studied here is associated with a brightening
observed in the EUV waveband and is produced by an energy release of
10&lt;SUP&gt;25&lt;/SUP&gt; ergs. The fact that the flux density of the radio
transient is only 2 mSFU suggests that it might be possible to do large
statistical studies in the future for understanding the relationship
between these radio transients and other EUV and X-ray counterparts, as
well as for understanding their importance in coronal heating.</description>
</item>
<item>
<title> Quasi-Periodic Pulsations Detected in Ly  and Nonthermal Emissions During Solar Flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..130L</link>
<description>We report quasi-periodic pulsations (QPPs) with double periods during
three solar flares (viz. SOL2011-Feb-15T01:44, SOL2011-Sep-25T04:31,
SOL2012-May-17T01:25). The flare QPPs were observed from light curves in
Ly- , hard X-ray (HXR), and microwave emissions, with the Ly- emission
recorded by the Geostationary Operational Environmental Satellite, the
HXR emission recorded by the Reuven Ramaty High-Energy Solar
Spectroscopic Imager and the Fermi Gamma-ray Burst Monitor, and the
microwave emission recorded by the Nobeyama Radio Polarimeters and
Radioheliograph. By using the Markov chain Monte Carlo (MCMC) method,
QPPs with double periods of about two minutes and one minute were first
found in the Ly- emission. Then using the same method, a QPP with
nearly the same period of about two minutes was also found in HXR and
microwave emissions. Considering the possible common origin (nonthermal
electrons) between Ly- and HXR/microwave emission, we suggest that the
two-minute QPP results from the periodic acceleration of nonthermal
electrons during magnetic reconnections. The ratio between the double
periods in the Ly- emission was found to be close to two, which is
consistent with the theoretical expectation between the fundamental and
harmonic modes. However, we cannot rule out other possible driving
mechanisms for the one-minute QPPs in HXR/microwave emissions due to
their relatively large deviations.</description>
</item>
<item>
<title> Radio Interferometric Observations of the Sun Using Commercial Dish TV Antennas</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296..121G</link>
<description>The radio astronomy group in the Indian Institute of Astrophysics (IIA)
has been carrying out routine observations of radio emission from the
solar corona at low frequencies (40 - 440 MHz) at the Gauribidanur
observatory, about 100 km north of Bangalore. Since IIA has been
performing regular observations of the solar photosphere and
chromosphere using different optical telescopes in its Kodaikanal Solar
Observatory (KSO) also (see https://www.iiap.res.in/kodai.htm), the
possibilities of obtaining two-dimensional radio images of the solar
chromosphere using low-cost instrumentation to supplement the optical
observations are being explored. As a part of the exercise, recently the
group had developed prototype instrumentation for interferometric
observations of radio emission from the solar chromosphere at high
frequencies (11.2 GHz) using two commercial dish TV antennas. The
hardware set-up and initial observations are presented.</description>
</item>
<item>
<title> Evolvement of microwave spike bursts in a solar flare on 2006 December 13</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..148T</link>
<description>Solar radio spikes are one of the most intriguing spectral types of
radio bursts. Their very short lifetimes, small source size and super-
high brightness temperature indicate that they should be involved in
some strong energy release, particle acceleration and coherent emission
processes closely related to solar flares. In particular, for the
microwave spike bursts, their source regions are much close to the
related flaring source region which may provide the fundamental
information of the flaring process. In this work, we identify more than
600 millisecond microwave spikes which recorded by the Solar Broadband
Radio Spectrometer in Huairou (SBRS/Huairou) during an X3.4 solar flare
on 2006 December 13 and present a statistical analysis about their
parametric evolution characteristic. We find that the spikes have nearly
the same probability of positive and negative frequency drifting rates
not only in the flare rising phase, but also in the peak and decay
phases. So we suppose that the microwave spike bursts should be
generated by shock-accelerated energetic electrons, just like the
terminational shock (TS) wave produced by the reconnection outflows near
the loop top. The spike bursts occurred around the peak phase have the
highest central frequency and obviously weak emission intensity, which
imply that their source region should have the lowest position with
higher plasma density due to the weakened magnetic reconnection and the
relaxation of TS during the peak phase. The right-handed polarization of
the most spike bursts may be due to the TS lying on the top region of
some very asymmetrical flare loops.</description>
</item>
<item>
<title> Correction of the temperature effect in calibration of a solar radio telescope</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..147G</link>
<description>This work analyzes the annual fluctuation of the observation data of the
Mingantu Solar radio Telescope (MST) in S, C and X bands. It is found
that the data vary with local air temperature as the logarithmic
attenuation of equipment increases with temperature and frequency. A
simplified and effective calibration method is proposed, which is used
to calibrate the MST data in 2018-2020, while the correction
coefficients are calculated from data in 2018-2019. For S, C and X
bands, the root mean square errors of one polarization are 2.7, 5.7 and
20 sfu, and the relative errors are 4%, 6% and 8% respectively. The
calibration of MUSER and SBRS spectra is also performed. The relative
errors of MUSER at 1700 MHz, SBRS at 2800 MHz, 3050 MHz and 3350 MHz are
8%, 8%, 11% and 10% respectively. We found that several factors may
affect the calibration accuracy, especially at X-band. The method is
expected to work for other radio telescopes with similar design.</description>
</item>
<item>
<title> spectrometer commissioning and observations of type III solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21..145R</link>
<description>The Astrophysics Directorate of CONIDA has installed two radio
spectrometer stations belonging to the e-CALLISTO network in Lima, Peru.
Given their strategic location near the Equator, it is possible to
observe the Sun evenly throughout the whole year. The receiver located
at Pucusana, nearby the capital city of Lima, took data from October
2014 until August 2016 in the metric and decimetric bands looking for
radio bursts. During this period, this e-CALLISTO detector was unique in
its time-zone coverage. To asses the suitability of the sites and the
performance of the antennas, we analyzed the radio ambient background
and measured their radiation pattern and beamwidth. To demonstrate the
capabilities of the facilities for studying solar dynamics in these
radio frequencies, we have selected and analyzed type III Solar Radio
Bursts. The study of this kind of burst helps to understand the electron
beams traversing the solar corona and the solar atmospheric density. We
have characterized the most common radio bursts with the following mean
values: a negative drift rate of -25.8  3.7 MHz s&lt;SUP&gt;-1&lt;/SUP&gt;, a
duration of 2.6  0.3 s and 35 MHz bandwidth in the frequency range of
114 to 174 MHz. In addition, for some events, it was possible to
calculate a global frequency drift which on average was 0.4  0.1 MHz
s&lt;SUP&gt;-1&lt;/SUP&gt;.</description>
</item>
<item>
<title> A long-term multifrequency study of solar rotation using the solar radio flux and its relationship with solar cycles</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.505.5228S</link>
<description>This paper examines long-term (more than four solar cycles) temporal and
spatial fluctuations in the solar rotation by investigating radio-
emission escapes from various layers of the solar atmosphere during the
years 1967-2010. The flux modulation approach can also be used to
investigate variations in solar rotation, which is a contentious topic
in solar physics. This study makes use of a time-series of radio flux
data at various frequencies (245-15 400 MHz) obtained at Sagamore Hill
Solar Radio Observatory in Massachusetts, USA, and at other
observatories from 1967 to 2010. The periodicity present in the temporal
variation of the time-series is estimated through a Lomb-Scargle
periodogram. The rotation period estimated for five radio emissions
(606, 1415, and 2695 MHz from the corona, and 4995 and 8800 MHz from the
transition region) through a statistical approach shows continuous
temporal and spatial variations throughout the years. The smoothed
rotation period shows the presence of periodic ~22-yr and ~11-yr
components. The 22-yr component could be linked to the reversal of the
solar magnetic field (Hale) cycle, while the 11-yr component is most
likely related to the sunspot (Schwabe) cycle. In addition to these two
components, random components are also prominently present in the
analysed data. The cross-correlation between the sunspot number and the
rotation period obtained shows a strong correlation with the 11-yr
Schwabe and 22-yr Hale cycle. The corona rotates faster or slower than
the transition region in different epochs. The alternation of the faster
rotation speed between the corona and transition region also follows the
22-yr cycle.</description>
</item>
<item>
<title> The Role of Flare-Driven Ionospheric Electron Density Changes on the Doppler Flash Observed by SuperDARN HF Radars</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JGRA..12629300C</link>
<description>Trans-ionospheric high frequency (HF: 3-30 MHz) signals experience
strong attenuation following a solar flare-driven sudden ionospheric
disturbance (SID). Solar flare-driven HF absorption, referred to as
short-wave fadeout, is a well-known impact of SIDs, but the initial
Doppler frequency shift phenomena, also known as "Doppler flash" in the
traveling radio wave is not well understood. This study seeks to advance
our understanding of the initial impacts of solar flare-driven SID using
a physics-based whole atmosphere model for a specific solar flare event.
First, we demonstrate that the Doppler flash phenomenon observed by
Super Dual Auroral Radar Network (SuperDARN) radars can be successfully
reproduced using first-principles based modeling. The output from the
simulation is validated against SuperDARN line-of-sight Doppler velocity
measurements. We then examine which region of the ionosphere, D, E, or
F, makes the largest contribution to the Doppler flash. We also consider
the relative contribution of change in refractive index through the
ionospheric layers versus lowered reflection height. We find: (a) the
model is able to reproduce radar observations with an root-median-
squared-error and a mean percentage error () of 3.72 m/s and 0.67%,
respectively; (b) the F-region is the most significant contributor to
the total Doppler flash (48%), 30% of which is contributed by the
change in F-region's refractive index, while the other 18% is due to
change in ray reflection height. Our analysis shows lowering of the
F-region's ray reflection point is a secondary driver compared to the
change in refractive index.</description>
</item>
<item>
<title> Data set for solar flare prediction using helioseismic and magnetic imager vector magnetic field data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021DIB....3707203H</link>
<description>It is known that solar flares can affect the near-Earth space, incurring
in consequences for radio communications. Therefore, there is a need to
research systems for monitoring solar events. This article presents a
data set which can be used in the analysis of such events. This data set
originated from a set of records from magnetic attributes and solar
flare data. In order to create this data set, authors used the SunPy
library which provided access to data from the Joint Science Operations
Center (JSOC) and Space Weather Prediction Center (SWPC). By integrating
data from those two sources, 8,874 samples were obtained comprehending
the period between May, 2010 and December, 2019. The collected data were
stored as a CSV data set. This data set can be used to support the
research of solar flare forecasting, as well as to be compared to other
data sets or expanded with new attributes.</description>
</item>
<item>
<title> A study based on the dominance of hemispheric sunspot activity during the solar cycles 18-24</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ChJPh..72....1E</link>
<description>Solar activity indices differ over the solar disk, and different
activity parameters are not considered to be symmetric between the
northern and southern solar hemispheres. In the present paper, the daily
data of a set of solar parameters (solar radio flux F10.7, total solar
irradiance TSI, plage area PA, coronal index CI, solar flare index SFI,
and solar mean magnetic field B) as well as the daily hemispheric
sunspot areas (SSAs) and sunspot numbers (SSNs) during a timeframe
1945-2017 (covering almost the last seven solar cycles, 18  24) have
been employed to investigate the north-south (N-S) asymmetry of the
considered solar parameters based on the dominance of hemispheric
distributions of SSAs and SSNs. The N-S asymmetry for each solar
parameter has been investigated and the results revealed that it is a
significant aspect through different years in the entire period. The
grand average of each solar parameter for the northern and southern
groups over each solar activity cycle has been calculated to investigate
the statistical significance of N-S asymmetry of each solar parameter in
each solar activity cycle. The solar cycles 19 and 24 displayed the
dominance of the southern F10.7 and PA over the northern one. However,
the solar cycle 23 showed the reverse. The grand average of CI displayed
the southern preference in the solar cycle 19 while, the northern
dominance of CI is revealed for the solar cycle 23. The grand averages
of CI demonstrated nearly symmetric distribution in solar cycles 18, and
20-22. The N-S asymmetry of the grand averages of SFI exhibited a
southern dominance during solar cycles 21 and 24. On the other hand, the
northern preference is observed for the grand average of SFI through the
solar cycle 23. The asymmetry of the grand averages of B obviously has
the same dominance (sign) of hemispheric sunspot activity indices for
the solar cycles 21-24. The periodic behavior of the N-S asymmetry of
SSAs, SSNs, F10.7, and B has been investigated using Fast Fourier
Transformation. Many mid- and long term periodicities have been
detected. We present our results and discuss their possible
explanations.</description>
</item>
<item>
<title> First Frequency-time-resolved Imaging Spectroscopy Observations of Solar Radio Spikes</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...917L..32C</link>
<description>Solar radio spikes are short duration and narrow bandwidth fine
structures in dynamic spectra observed from the GHz to tens of MHz
range. Their very short duration and narrow frequency bandwidth are
indicative of subsecond small-scale energy release in the solar corona,
yet their origin is not understood. Using the LOw Frequency ARray, we
present spatially, frequency, and time resolved observations of
individual radio spikes associated with a coronal mass ejection.
Individual radio spike imaging demonstrates that the observed area is
increasing in time and the centroid positions of the individual spikes
move superluminally parallel to the solar limb. Comparison of spike
characteristics with that of individual Type IIIb striae observed in the
same event show similarities in duration, bandwidth, drift rate,
polarization, and observed area, as well the spike and striae motion in
the image plane suggesting fundamental plasma emission with the spike
emission region on the order of ~10&lt;SUP&gt;8&lt;/SUP&gt; cm, with brightness
temperature as high as 10&lt;SUP&gt;13&lt;/SUP&gt; K. The observed spatial,
spectral, and temporal properties of the individual spike bursts are
also suggestive of the radiation responsible for spikes escaping through
anisotropic density turbulence in closed loop structures with scattering
preferentially along the guiding magnetic field oriented parallel to the
limb in the scattering region. The dominance of scattering on the
observed time profile suggests the energy release time is likely to be
shorter than what is often assumed. The observations also imply that the
density turbulence anisotropy along closed magnetic field lines is
higher than along open field lines.</description>
</item>
<item>
<title> Second Harmonic Electromagnetic Emissions by an Electron Beam in Solar Wind Plasmas with Density Fluctuations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...917L..23K</link>
<description>Two-dimensional particle-in-cell simulations are performed to study the
electromagnetic radiation emitted at the second harmonic 2&lt;SUB&gt;p&lt;/SUB&gt;
of the plasma frequency by a weak electron beam propagating in a
background plasma with random density fluctuations, in solar wind
conditions relevant to Type III solar radio bursts. The dynamics of the
waves, the beam, and the plasma are calculated over several thousands of
plasma periods. For relevant comparisons, simulations with and without
applied density fluctuations are performed for the same parameters. This
Letter evidences for the first time the impact of density fluctuations
on the physical mechanisms driving the generation of electromagnetic
waves emitted at 2&lt;SUB&gt;p&lt;/SUB&gt;. Results obtained show that (i) the beam
radiates electromagnetic waves at 2&lt;SUB&gt;p&lt;/SUB&gt; as a result of
nonlinear processes of Langmuir waves' coalescence, despite wave
scattering on the density fluctuations that strongly affect the Langmuir
spectra; (ii) the fraction of initial beam energy transferred
asymptotically to the electromagnetic waves at 2&lt;SUB&gt;p&lt;/SUB&gt; is by one
order of magnitude smaller when the plasma involves density fluctuations
of average level around 5%; (iii) compared to the homogeneous case, the
ratio of electromagnetic energy radiated at 2&lt;SUB&gt;p&lt;/SUB&gt; to the energy
carried by the Langmuir wave turbulence is significantly larger during
all the nonlinear stage; (iv) asymptotically, when the plasma is
inhomogeneous, electromagnetic emissions at 2&lt;SUB&gt;p&lt;/SUB&gt; present
isotropized spectra whereas quadrupolar radiation occurs for the
homogeneous plasma case.</description>
</item>
<item>
<title> The Possibility of Observing Several Hydrogen Radio Lines in Solar Activity Features over Sunspots</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ARep...65..705D</link>
<description>The first solar radio line attributed to atomic hydrogen was
theoretically grounded by J.P. Wild in 1952. Its Zeeman profile was
calculated and reliably established in the radiation from quiet Sun
regions and activity features over sunspots in 2018 using observations
with the RATAN-600 radio telescope, leading to the determination of
several parameters of the line emitting regions and the estimation of
magnetic fields in the solar atmosphere. In this paper, we calculate the
Zeeman profile for two more hydrogen radio lines and show that they can
be observed in activity features over sunspots.</description>
</item>
<item>
<title> 2019 International Women's Day event. Two-step solar flare with multiple eruptive signatures and low Earth impact</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...652A.159D</link>
<description>Context. We present a detailed analysis of an eruptive event that
occurred on 2019 March 8 in the active region AR 12734, which we refer
as the International Women's Day event. The event under study is
intriguing based on several aspects: (1) low-coronal eruptive signatures
come in `pairs', namely, there is a double-peaked flare, two coronal
dimmings, and two extreme ultraviolet (EUV) waves; (2) although the
event is characterized by a complete chain of eruptive signatures, the
corresponding coronagraphic signatures are weak; and (3) although the
source region of the eruption is located close to the center of the
solar disc and the eruption is thus presumably Earth-directed,
heliospheric signatures are very weak with very weak Earth impact. &lt;BR
/&gt; Aims: In order to understand the initiation and evolution of this
particular event, we performed a comprehensive analysis using a combined
observational-modeling approach. &lt;BR /&gt; Methods: We analyzed a number of
multi-spacecraft and multi-instrument (both remote-sensing and in situ)
observations, including soft X-ray, EUV, radio and white-light emission,
as well as plasma, magnetic field, and particle measurements. We
employed 3D nonlinear force-free modeling to investigate the coronal
magnetic field configuration in and around the active region, the
graduated cylindrical shell model to make a 3D reconstruction of the CME
geometry, and the 3D magnetohydrodynamical numerical model EUropean
Heliospheric FORecasting Information Asset to model the background state
of the heliosphere. &lt;BR /&gt; Results: Our results reveal a two-stage C1.3
flare, associated with two EUV waves that occur in close succession and
two-stage coronal dimmings that evolve co-temporally with the flare and
type II and III radio bursts. Despite its small GOES class, a clear drop
in magnetic free energy and helicity is observed during the flare. White
light observations do not unambiguously indicate two separate CMEs, but
rather a single entity most likely composed of two sheared and twisted
structures corresponding to the two eruptions observed in the low
corona. The corresponding interplanetary signatures are that of a small
flux rope swith indications of strong interactions with the ambient
plasma, which result in a negligible geomagnetic impact. &lt;BR /&gt;
Conclusions: Our results indicate two subsequent eruptions of two
systems of sheared and twisted magnetic fields, which already begin to
merge in the upper corona and start to evolve further out as a single
entity. The large-scale magnetic field significantly influences both the
early and the interplanetary evolution of the structure. During the
first eruption, the stability of the overlying field was disrupted,
enabling the second eruption. We find that during the propagation in the
interplanetary space the large-scale magnetic field, that is, the
location of heliospheric current sheet between the AR and the Earth, is
likely to influence propagation, along with the evolution of the erupted
structure(s). &lt;P /&gt;Movies are available at &lt;A href="https://www.aanda.or
g/10.1051/0004-6361/202140752/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> ALMA observations of the variability of the quiet Sun at millimeter wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...652A..92N</link>
<description>&lt;BR /&gt; Aims: We address the variability of the quiet solar chromosphere
at 1.26 mm and 3 mm with a focus on the study of spatially resolved
oscillations and transient brightenings, which are small, weak events of
energy release. Both phenomena may have a bearing on the heating of the
chromosphere. &lt;BR /&gt; Methods: We used Atacama Large
Millimeter/submillimeter Array (ALMA) observations of the quiet Sun at
1.26 mm and 3 mm. The spatial and temporal resolution of the data were 1
 2 and 1 s, respectively. The concatenation of light curves from
different scans yielded a frequency resolution in spectral power of
0.50.6 mHz. At 1.26 mm, in addition to power spectra of the original
data, we degraded the images to the spatial resolution of the 3 mm
images and used fields of view that were equal in area for both data
sets. The detection of transient brightenings was made after the effect
of oscillations was removed. &lt;BR /&gt; Results: At both frequencies, we
detected p-mode oscillations in the range 3.64.4 mHz. The corrections
for spatial resolution and field of view at 1.26 mm decreased the root
mean square (rms) of the oscillations by a factor of 1.6 and 1.1,
respectively. In the corrected data sets, the oscillations at 1.26 mm
and 3 mm showed brightness temperature fluctuations of 1.7  1.8% with
respect to the average quiet Sun, corresponding to 137 and 107 K,
respectively. We detected 77 transient brightenings at 1.26 mm and 115
at 3 mm. Although their majority occurred in the cell interior, the
occurrence rate per unit area of the 1.26 mm events was higher than that
of the 3 mm events; this conclusion does not change if we take into
account differences in spatial resolution and noise levels. The energy
associated with the transient brightenings ranged from 1.8 
10&lt;SUP&gt;23&lt;/SUP&gt; to 1.1  10&lt;SUP&gt;26&lt;/SUP&gt; erg and from 7.2 
10&lt;SUP&gt;23&lt;/SUP&gt; to 1.7  10&lt;SUP&gt;26&lt;/SUP&gt; erg for the 1.26 mm and 3 mm
events, respectively. The corresponding power-law indices of the energy
distribution were 1.64 and 1.73. We also found that ALMA bright network
structures corresponded to dark mottles or spicules that can be seen in
broadband H images from the GONG network. &lt;BR /&gt; Conclusions: The
fluctuations associated with the p-mode oscillations represent a
fraction of 0.550.68 of the full power spectrum. Their energy density
at 1.26 mm is 3  10&lt;SUP&gt;2&lt;/SUP&gt; erg cm&lt;SUP&gt;3&lt;/SUP&gt;. The computed low-
end energy of the 1.26 mm transient brightenings is among the smallest
ever reported, irrespective of the wavelength of the observation.
Although the occurrence rate per unit area of the 1.26 mm transient
brightenings was higher than that of the 3 mm events, their power per
unit area is smaller likely due to the detection of many weak 1.26 mm
events.</description>
</item>
<item>
<title> Multi-objective Optimization of Interferometric Array u-v Coverage</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PASP..133g4503Z</link>
<description>A new principle is introduced to optimize the configuration of an
interferometric array, based on the trade-off between the uniform and
Gaussian u-v distributions. The multi-objective optimization method,
nondominated sorting genetic algorithm II (NSGA-II), is applied to
achieve the optimal trade-off. The resulting array having a single
configuration can meet the observation requirements of both compact and
extended sources. This method has been successfully applied to design a
16-element array as the initial stage of the Daocheng Solar Radio
Telescope to illustrate its feasibility. NSGA-II is improved by
introducing artificial intervention into the genetic operator to solve
the equality constraints. The improved NSGA-II is applied to obtain the
Pareto optimal set, and a 16-element array configuration is retrieved
with the best u-v trade-off between the snapshot mode and Earth rotation
synthesis mode.</description>
</item>
<item>
<title> Development of a local empirical model of ionospheric total electron content (TEC) and its application for studying solar-ionospheric effects</title>
<link>https://ui.adsabs.harvard.edu/abs/2021NatSR..1115070D</link>
<description>Regular and irregular variations in total electron content (TEC) are one
of the most significant observables in ionospheric studies. During the
solar cycle 24, the variability of ionosphere is studied using global
positioning system derived TEC at a mid-latitude station, Tehran
(35.70N, 51.33E). Based on solar radio flux and seasonal and local time-
dependent features of TEC values, a semi-empirical model is developed to
represent its monthly/hourly mean values. Observed values of TEC and the
results of our semi-empirical model then are compared with estimated
values of a standard plasmasphere-ionosphere model. The outcome of this
model is an expected mean TEC value considering the monthly/hourly
regular effects of solar origin. Thus, it is possible to use it for
monitoring irregular effects induced by solar events. As a result, the
connection of TEC variations with solar activities are studied for the
case of coronal mass ejections accompanying extreme solar flares. TEC
response to solar flares of class X is well reproduced by this model.
Our resulting values show that the most powerful flares (i.e. class X)
induce a variation of more than 20 percent in daily TEC extent.</description>
</item>
<item>
<title> Radial differential rotation of solar corona using radio emissions</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.505L..16S</link>
<description>The present work is an effort to investigate possible radial variations
in the solar coronal rotation by analysing the solar radio emission data
at 15 different frequencies (275-1755 MHz) for the period starting from
1994 July to 1999 May. We used a time series of disc-integrated radio
flux recorded daily at these frequencies through radio telescopes
situated at the Astronomical Observatory of the Jagellonian University
in Cracow. The different frequency radiation originates from different
heights in the solar corona. Existing models indicate its origin at the
height range from nearly ~12 000 km (for emission at 275 MHz), below up
to ~2400 km (for emission at 1755 MHz). There are some data gaps in the
time series used for the study, so we used statistical analysis using
the Lomb-Scargle periodogram (LSP). This method has successfully
estimated the periodicity present in time series even with such data
gaps. The rotation period estimated through LSP shows variation in the
rotation period, which is compared with the earlier reported estimate
using auto correlation technique. This study indicates some similarity
as well as a contradiction with studies reported earlier. The radial and
temporal variation in the solar rotation period are presented and
discussed for the whole period analysed.</description>
</item>
<item>
<title> A geometrical description for interplanetary propagation of Earth-directed CMEs based on radiative proxies</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.504.5899S</link>
<description>We present a 3D geometrical model to describe the propagation and
expansion of coronal mass ejections (CMEs) in the interplanetary space
based on radiative proxies to be implemented in previous procedures that
use SXR and microwave emissions to estimate the Earth-directed CME
propagation speed. We carefully selected a sample of 45 well-defined
CME-ICME events to evaluate our model. We computed this 3D geometrical
model for each event as a tool to improve the arrival time predictions
based on radiative proxies. We conducted a different analysis for each
radiative proxy: SXR emission and microwave emission at 9 GHz, and we
compared the results separately with the observations by the Wind
spacecraft. In general, the results showed that the implementation of
our 3D geometrical model improves the predictions and provides an
important complement to the arrival time prediction method based on
radiative proxies, especially for CME events whose source origin were
located at helio longitudes far from the central meridian at least 10.
Improvements for this tool based on observations by Parker Solar Probe
and Solar Orbiter must be developed in the future work.</description>
</item>
<item>
<title> Glaciological Monitoring Using the Sun as a Radio Source for Echo Detection</title>
<link>https://ui.adsabs.harvard.edu/abs/2021GeoRL..4892450P</link>
<description>Ice-penetrating radar observations are critical for projecting ice-sheet
contribution to sea-level rise; however, these prognostic models have
significant uncertainties due to an incomplete understanding of glacial
subsurface processes. Existing radars that can characterize subsurface
conditions are too resource-intensive to simultaneously monitor ice
sheets at both the necessary temporaldaily to multiannualand
spatialtributary to continentalscales. Here, we investigate using an
ambient radio source, instead of transmitting a signal, for
glaciological monitoring. We demonstrate, for the first time, passive
radio sounding using the Sun to accurately measure ice thickness on
Store Glacier, Greenland. Passive radar sounding could provide low-
resource time-series measurements of the cryosphere, enabling us to
observe and understand evolving englacial and subglacial conditions
across Greenland and Antarctica with unprecedented coverage and
resolution.</description>
</item>
<item>
<title> Eruptive versus confined X-class flares in solar cycles 23 and 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2021BlgAJ..35...87M</link>
<description>A systematic analysis on the properties of all GOES X-class solar flares
(SFs) in solar cycles 23 and 24 (1996-2019) is performed. The occurrence
rates and parameters of the eruptive and confined SFs are presented. The
aspect of eruptivity versus confinement is investigated with respect to
the co-occurrence of coronal mass ejections (CMEs), radio emissions,
energetic protons and geomagnetic storms. The absence of interplanetary
type III radio bursts, in addition to the lack of CMEs, is found to be a
very good proxy for confinement, in contrast to the sunspot type of the
parent active region, as both eruptive and confined SFs are
predominantly of -- magnetic type. The remaining parameters, protons
and geomagnetic storms, imply observing from a specific location in the
heliophere and thus are biased for Earth-reaching phenomena. Finally,
the relationships between the two types of SFs and the considered here
solar activity phenomena are discussed in view of previous studies.</description>
</item>
<item>
<title> An Interplanetary Type IIIb Radio Burst Observed by Parker Solar Probe and Its Emission Mechanism</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...915L..22C</link>
<description>Type IIIb radio bursts were identified as a chain of quasi-periodic
striae in dynamic spectra, drifting from high to low frequencies in a
manner similar to type III bursts, which fine structures may provide a
clue to a better understanding of emission mechanisms. The approaching
observation of the Parker Solar Probe (PSP) spacecraft provides a new
chance of probing type IIIb bursts in the vicinity of the Sun. In this
Letter, combining the in situ measurement of PSP and the empirical model
of solar atmospheres in open magnetic field regions, we analyze in
detail a typical event of interplanetary (IP) type IIIb bursts observed
by PSP, which was first reported by Pulupa et al. Our results show that
the electron cyclotron maser (ECM) emission can probably play an
important role in the excitation mechanism of the IP type IIIb burst and
the formation of the fine striae structure may be attributed to the
modulation of Alfvn waves on the growth rate of the ECM instability.</description>
</item>
<item>
<title> Broken Power-law Energy Spectra of the Accelerated Electrons Detected in Radio and Hard X-Rays during the SOL2013-05-13 Event</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...915L...1D</link>
<description>Solar flares, resulting from magnetic activity of the Sun, are among the
most energetic events in the solar system and in extreme cases directly
affect our highly technological society. In this work, we analyze a
solar flare detected at millimeter and centimeter wavelengths, as well
as X-rays above 1 MeV. Observations of solar flares at these energy
bands provide diagnostics of the energetic accelerated electrons and the
magnetic fields where the emission is produced. During the SOL2013-05-13
solar flare, radio data were obtained by the telescope system
POlarisation Emission of Millimeter Activity at the Sun, which observes
the Sun at 45 and 90 GHz with polarization measurements, and at
microwaves (1-15 GHz) by the Radio Solar Telescope Network. For the same
event, X-ray emission was detected by the RHESSI and Fermi satellites.
Spectra at both wavelengths were constructed and fit separately to yield
the accelerated electron energy distribution that produced the emission.
The optically thin radio spectral index was calculated by fitting the
Ramaty model of gyrosynchrotron emission to the observed radio spectrum,
whereas the hard X-ray spectral index was obtained from the spectral fit
assuming a thermal emission model plus a nonthermal broken power-law
distribution. Finally, both spectral indexes were compared and confirmed
that the index obtained from the radio spectrum agrees with the index of
the X-ray spectrum for energies above the break energy of ~600 keV.
Thus, the hard X-rays more energetic than 600 keV and high radio
frequencies of solar flares are emitted by the same population of high-
energy accelerated electrons. This result indicates that the accelerated
electrons have an energy distribution best represented by a broken power
law, with a breakup above energies around 1 MeV.</description>
</item>
<item>
<title> Radio evidence for a shock wave reflected by a coronal hole</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...651L..14M</link>
<description>We report the first unambiguous observational evidence in the radio
range of the reflection of a coronal shock wave at the boundary of a
coronal hole. The event occurred above an active region located at the
northwest limb of the Sun and was characterized by an eruptive
prominence and an extreme-ultraviolet wave steepening into a shock. The
EUV observations acquired by the Atmospheric Imaging Assembly instrument
on board the Solar Dynamics Observatory and the Extreme Ultraviolet
Imager instrument on board the Solar TErrestrial RElations Observatory
were used to track the development of the EUV front in the inner corona.
Metric type II radio emission, a distinguishing feature of shock waves
propagating in the inner corona, was simultaneously recorded by ground-
based radio spectrometers. The radio dynamic spectra displayed an
unusual reversal of the type II emission lanes, together with type III-
like herringbone emission, indicating shock-accelerated electron beams.
Combined analysis of imaging data from the two space-based EUV
instruments and the Nanay Radioheliograph evidences that the reverse-
drifting type II emission was produced at the intersection of the shock
front, reflected at a coronal hole boundary, with an intervening low-
Alfvn-speed region characterized by an open field configuration. We
also provide an outstanding data-driven reconstruction of the
spatiotemporal evolution in the inner corona of the shock-accelerated
electron beams produced by the reflected shock.</description>
</item>
<item>
<title> Harmonic electron-cyclotron maser emissions driven by energetic electrons of the horseshoe distribution with application to solar radio spikes</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...651A.118N</link>
<description>Context. Electron-cyclotron maser emission (ECME) is the favored
mechanism for solar radio spikes and has been investigated extensively
since the 1980s. Most studies relevant to solar spikes employ a loss-
cone-type distribution of energetic electrons, generating waves mainly
in the fundamental X/O mode (X1/O1), with a ratio of plasma oscillation
frequency to electron gyrofrequency (&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;)
lower than 1. Despite the great progress made in this theory, one major
problem is how the fundamental emissions pass through the second-
harmonic absorption layer in the corona and escape. This is generally
known as the escaping difficulty of the theory. &lt;BR /&gt; Aims: We study
the harmonic emissions generated by ECME driven by energetic electrons
with the horseshoe distribution to solve the escaping difficulty of ECME
for solar spikes. &lt;BR /&gt; Methods: We performed a fully kinetic
electromagnetic particle-in-cell simulation with
&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt; = 0.1, corresponding to the strongly
magnetized plasma conditions in the flare region, with energetic
electrons characterized by the horseshoe distribution. We also varied
the density ratio of energetic electrons to total electrons
(n&lt;SUB&gt;e&lt;/SUB&gt;/n&lt;SUB&gt;0&lt;/SUB&gt;) in the simulation. To analyze the
simulation result, we performed a fast Fourier transform analysis on the
fields data. &lt;BR /&gt; Results: We obtain efficient amplification of waves
in Z and X2 modes, with a relatively weak growth of O1 and X3. With a
higher-density ratio, the X2 emission becomes more intense, and the rate
of energy conversion from energetic electrons into X2 modes can reach
0.06% and 0.17%, with n&lt;SUB&gt;e&lt;/SUB&gt;/n&lt;SUB&gt;0&lt;/SUB&gt; = 5% and 10%,
respectively. &lt;BR /&gt; Conclusions: We find that the horseshoe-driven ECME
can lead to an efficient excitation of X2 and X3 with a low value of
&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;, providing novel means for resolving the
escaping difficulty of ECME when applied to solar radio spikes. The
simultaneous growth of X2 and X3 can be used to explain some harmonic
structures observed in solar spikes. &lt;P /&gt;Movies associated to Figs. 1,
4, and 5 are available at &lt;A href="https://www.aanda.org/10.1051/0004-63
61/202140427/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> ALMA small-scale features in the quiet Sun and active regions</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...651A...6B</link>
<description>&lt;BR /&gt; Aims: The main aim of the present analysis is to decipher (i) the
small-scale bright features in solar images of the quiet Sun and active
regions obtained with the Atacama Large Millimeter/submillimeter Array
(ALMA) and (ii) the ALMA correspondence of various known chromospheric
structures visible in the H images of the Sun. &lt;BR /&gt; Methods: Small-
scale ALMA bright features in the quiet Sun region were analyzed using
single-dish ALMA observations (1.21 mm, 248 GHz) and in an active region
using interferometric ALMA measurements (3 mm, 100 GHz). With the
single-dish observations, a full-disk solar image is produced, while
interferometric measurements enable the high-resolution reconstruction
of part of the solar disk, including the active region. The selected
quiet Sun and active regions are compared with the H (core and wing
sum), EUV, and soft X-ray images and with the magnetograms. &lt;BR /&gt;
Results: In the quiet Sun region, enhanced emission seen in the ALMA is
almost always associated with a strong line-of-sight magnetic field.
Four coronal bright points were identified, while other small-scale ALMA
bright features are most likely associated with magnetic network
elements and plages. In the active region, in 14 small-scale ALMA bright
features randomly selected and compared with other images, we found five
good candidates for coronal bright points, two for plages, and five for
fibrils. Two unclear cases remain: a fibril or a jet, and a coronal
bright point or a plage. A comparison of the H core image and the 3 mm
ALMA image of the analyzed active region showed that the sunspot appears
dark in both images (with a local ALMA radiation enhancement in sunspot
umbra), the four plage areas are bright in both images and dark small H
filaments are clearly recognized as dark structures of the same shape
also in ALMA.</description>
</item>
<item>
<title> A Bayesian Inference-Based Empirical Model for Scintillation Indices for High-Latitude</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SpWea..1902710M</link>
<description>Solar wind parameters, the solar radio flux index (F10.7), the Sun's
declination and the SuperMAG Electrojet index are used to construct a
Bayesian inference-based empirical model for scintillation indices
(S&lt;SUB&gt;4&lt;/SUB&gt; and &lt;SUB&gt;&lt;/SUB&gt;) at high latitudes. For the present
study, measurements from three Global Positioning System (GPS) L1
receivers located in the auroral zone, the cusp and in the polar cap are
selected, respectively. The solar wind characteristics include the solar
wind speed (V&lt;SUB&gt;SW&lt;/SUB&gt;) and ram pressure (&lt;SUB&gt;SW&lt;/SUB&gt;) as well as
the Geocentric Solar Magnetospheric (GSM) B&lt;SUB&gt;y&lt;/SUB&gt; and the
B&lt;SUB&gt;z&lt;/SUB&gt; components of the interplanetary magnetic field (IMF).
Following a brief assessment on the independence of the variables
(predictors), prior probabilities of occurrence in the case of a
multinomial classification are constructed. Posterior-probabilities are
then deduced for any arbitrary set of predictors. We show that the model
captures most variations seen in the measured indices whether they are
associated or not with transient interplanetary events. Although the
model tends to underestimate the actual phase index measurements, 95% of
the validated events are predicted with an error less than 0.034 rad in
&lt;SUB&gt;&lt;/SUB&gt;. For the amplitude scintillation index, 5% of validated
events have an error larger than 0.019.</description>
</item>
<item>
<title> SDO and Udaipur-CALLISTO Observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...85J</link>
<description>In this article, we present a multi-wavelength investigation of a
C-class flaring activity that occurred in the active region NOAA 12734
on 8 March 2019. The investigation utilizes data from the Atmospheric
Imaging Assembly (AIA) and the Helioseismic Magnetic Imager (HMI) on
board the Solar Dynamics Observatory (SDO) and the Udaipur-CALLISTO
solar radio spectrograph of the Physical Research Laboratory. This low
intensity C1.3 event is characterized by typical features of a long-
duration event (LDE), viz. extended flare arcade, large-scale two-ribbon
structures and twin coronal dimmings. The eruptive event occurred in a
coronal sigmoid and displayed two distinct stages of energy release,
manifested in terms of temporal and spatial evolution. The formation of
twin-dimming regions are consistent with the eruption of a large flux
rope with footpoints lying in the western and eastern edges of the
coronal sigmoid. The metric radio observations obtained from Udaipur-
CALLISTO reveals a broad-band (50 -180 MHz), stationary plasma emission
for 7 min during the second stage of the flaring activity that resemble
a type IV radio burst. A type III decametre-hectometre radio bursts with
starting frequency of 2.5 MHz precedes the stationary type IV burst
observed by Udaipur-CALLISTO by 5 min. The synthesis of multi-
wavelength observations and non-linear force-free field (NLFFF) coronal
modeling together with magnetic decay index analysis suggest that the
sigmoid flux rope underwent a zipping-like uprooting from its western to
eastern footpoints in response to the overlying asymmetric magnetic
field confinement. The asymmetrical eruption of the flux rope also
accounts for the observed large-scale structures viz. apparent eastward
shift of flare ribbons and post-flare loops along the polarity inversion
line (PIL), and provides evidence for lateral progression of magnetic
reconnection site as the eruption proceeds.</description>
</item>
<item>
<title> risk factors for Global Navigation Satellite Systems</title>
<link>https://ui.adsabs.harvard.edu/abs/2021STP.....7b..28D</link>
<description>Extreme space weather events affect the stability and quality of the
global navigation satellite systems (GNSS) of the second generation
(GPS, GLONASS, Galileo, BeiDou/Compass) and GNSS augmentation. We review
the theory about mechanisms behind the impact of geomagnetic storms,
ionospheric irregularities, and powerful solar radio bursts on the GNSS
user segment. We also summarize experimental observations of the space
weather effects on GNSS performance in 20002020 to confirm the theory.
We analyze the probability of failures in measurements of radio
navigation parameters, decrease in positioning accuracy of GNSS users in
dual-frequency mode and differential navigation mode (RTK), and in
precise point positioning (PPP). Additionally, the review includes data
on the occurrence of dangerous and extreme space weather phenomena and
the possibility for predicting their impact on the GNSS user segment.
The main conclusions of the review are as follows: 1) the positioning
error in GNSS users may increase up to 10 times in various modes during
extreme space weather events, as compared to the background level; 2)
GNSS space and ground segments have been significantly modernized over
the past decade, thus allowing a substantial increase in noise
resistance of GNSS under powerful solar radio burst impacts; 3) there is
a great possibility for increasing the tracking stability and accuracy
of radio navigation parameters by introducing algorithms for adaptive
lock loop tuning, taking into account the influence of space weather
events; 4) at present, the urgent scientific and technical problem of
modernizing GNSS by improving the scientific methodology, hardware and
software for monitoring the system integrity and monitoring the
availability of required navigation parameters, taking into account the
impact of extreme space weather events, is still unresolved.</description>
</item>
<item>
<title> Recent Observational Studies on the Fine Structures of Solar Type II Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PrA....39..129F</link>
<description>In the solar radio dynamic spectrum, type II radio bursts appear as
narrow-band features drifting slowly from higher to lower frequency.
These signals are due to plasma radiation excited by energetic
electrons. For fundamental plasma radiation, the emission is close to
the local plasma frequency. Type II bursts provide important insights in
the studies of shock waves driven by solar eruptions, shock-accelerated
energetic electrons and space weather forecasting. In addition, type II
radio bursts have a variety of fine structures in the dynamic spectrum.
According to their spectrotemporal features, they can be roughly
categorized into type II radio bursts with band-splitting, multi-branch,
herringbone, and sudden-spectral change structures. These fine
structures can be used to diagnose coronal parameters such as electron
density and magnetic field strength, to determine the speed and
configuration of the associated shock waves, and to further understand
the solar eruption processes. However, there are still many unresolved
problems in the cause of these fine structures, which require further
research. In particular, it is of great importance to use data with high
angular resolution available from newly-built radio heliographs in China
for research. This article reviews recent progresses on observational
studies of the fine structures of type II radio bursts and outlines
outstanding issues for future studies.</description>
</item>
<item>
<title> probing high-energy structures around the central molecular zone</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.504.1609W</link>
<description>Recent observations have revealed interstellar features that apparently
connect energetic activity in the central region of our Galaxy to its
halo. The nature of these features, however, remains largely uncertain.
We present a Chandra mapping of the central 2  4 field of the Galaxy,
revealing a complex of X-ray-emitting threads plus plume-like structures
emerging from the Galactic Centre (GC). This mapping shows that the
northern plume or fountain is offset from a well-known radio lobe (or
the GCL), which however may represent a foreground H II region, and that
the southern plume is well wrapped by a corresponding radio lobe
recently discovered by MeerKAT. In particular, we find that a distinct
X-ray thread, G0.17-0.41, is embedded well within a non-thermal radio
filament, which is locally inflated. This thread with a width of ~1.6
arcsec (FWHM) is ~2.6 arcmin or 6 pc long at the distance of the GC and
has a spectrum that can be characterized by a power law or an optically-
thin thermal plasma with temperature  3 keV. The X-ray-emitting
material is likely confined within a strand of magnetic field with its
strength  1 mG, not unusual in such radio filaments. These
morphological and spectral properties of the radio/X-ray association
suggest that magnetic field re-connection is the energy source. Such re-
connection events are probably common when flux tubes of antiparallel
magnetic fields collide and/or become twisted in and around the diffuse
X-ray plumes, representing blowout superbubbles driven by young massive
stellar clusters in the GC. The understanding of the process,
theoretically predicted in analog to solar flares, can have strong
implications for the study of interstellar hot plasma heating, cosmic
ray acceleration and turbulence.</description>
</item>
<item>
<title> On the influence of Langmuir wave spectra on the spectra of electromagnetic waves generated in solar plasma with double plasma frequency</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.503.5740K</link>
<description>In this paper, we consider the spectral dependences of transverse
electromagnetic waves generated in solar plasma at the coalescence of
Langmuir waves. It is shown that different spectra of Langmuir waves
lead to characteristic types of transversal electromagnetic wave
spectra, what makes it possible to diagnose the features of the spectra
of Langmuir waves generated in solar plasma.</description>
</item>
<item>
<title> Plasmaspheric scale height modeling based on COSMIC radio occultation data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JASTP.21705555W</link>
<description>The scale height in the plasmasphere (H&lt;SUB&gt;P&lt;/SUB&gt;) is an important
factor to present the dynamic nature and variations of the plasmasphere.
It is challenging to build reliable plasmaspheric scale height model
because of poor coverage and limited continuity of plasmaspheric sounder
data. In this paper, an empirical orthogonal function (EOF) analysis
method is applied to organize the H&lt;SUB&gt;P&lt;/SUB&gt; obtained from total
electron content (TEC) measurements of precise orbit determination (POD)
antennas and electron density profiles of Constellation Observing System
for Meteorology, Ionosphere, and Climate (COSMIC) mission, from the year
2007-2014, to reconstruct a global plasmaspheric scale height model. The
model depends on parameters including the month of the year, the local
time, the geographic latitude and the solar radio flux index F10.7.
Comparison of this model and the scale height deduced from the
International Satellites for Ionospheric Studies (ISIS) data shows
remarkable consistency in H&lt;SUB&gt;P&lt;/SUB&gt; values and variations.</description>
</item>
<item>
<title> Scaling features and IMF dependence</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JASTP.21705531C</link>
<description>We investigated the average polar patterns of ionospheric electron
density and the corresponding patterns of scaling features as a function
of interplanetary magnetic field orientation. The focus is on the
Northern Hemisphere using electron density data recorded on-board ESA
Swarm A satellite. The first- and second-order scaling exponents have
been evaluated by means of the q&lt;SUP&gt;th&lt;/SUP&gt; -order structure
functions. We used electron density measurements over a period of 15
months from April 1, 2014 to June 30, 2015, which corresponds to the
maximum of solar cycle 24 and which is characterized by an average value
of the solar radio flux (F10.7) index equal to (140  30) sfu. Electron
density, first- and second-order scaling exponents have been mapped and
discussed for four main IMF orientations provided by B&lt;SUB&gt;y&lt;/SUB&gt; and
B&lt;SUB&gt;z&lt;/SUB&gt; components under conditions of high solar activity. Large
spatial changes of the second-order scaling exponent pattern are
observed with a steepening of the associated spectral exponent in
correspondence with the nightside polar cap trailing edge.
Intermittency, defined as the departure from linearity of the dependence
of scaling exponents on moment order q, is also evaluated finding that
it is generally higher near the equatorward boundary of the auroral oval
than elsewhere. On the whole, the found patterns of the electron density
first- and second-order scaling exponents suggest the occurrence of
turbulence at the high latitudes.</description>
</item>
<item>
<title> the Gauribidanur and Greenland sites</title>
<link>https://ui.adsabs.harvard.edu/abs/2021InJPh..95.1051W</link>
<description>The instability of the Sun's magnetic field can ignite many eruptive
events on the solar surface, including flares, coronal mass ejections,
and prominence eruptions. The inner heliosphere environment is affected,
and consequently, these events are said to contribute to the celestial
weather change. As one of the many eruptive events, a solar flare is of
the most frequent due to the magnetic reconnection process in which the
accelerated electrons from the reconnection sites escape into the
interplanetary space and cause solar radio bursts type III (SRBT III).
When it is observed near the Earth, this SRBT III is in the form of
radio dynamics spectrum; thus, monitoring this spectrum is vital to the
further analysis of the said SRBT III. In this paper, we investigate the
background levels: short and long periods of the CALLISTO instruments
from two different stations where for each site, a 10-day background-
level observation is randomly selected. For the purpose of this study,
the mean differences and coefficient of variation (CV) distributions for
every frequency channel are determined where most of the frequency
channels have displayed small mean differences between these two
background levels: short and long periods and the CV distributions as
well. These short-period observations, within 15 min of the background
levels, are found significant enough to warrant further analysis of the
solar radio bursts detected by the CALLISTO instruments.</description>
</item>
<item>
<title> Gyroresonance and Free-Free Radio Emissions from Multithermal Multicomponent Plasma</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...914...52F</link>
<description>The solar atmosphere contains thermal plasma at a wide range of
temperatures. This plasma is often quantified, in both observations and
models, by a differential emission measure (DEM). The DEM is a
distribution of the thermal electron density squared over temperature.
In observations, the DEM is computed along a line of sight, while in the
modeling it is over an elementary volume element (voxel). This
description of the multithermal plasma is convenient and widely used in
the analysis and modeling of extreme ultraviolet emission, which has an
optically thin character. However, there is no corresponding treatment
in the radio domain, where the optical depth of emission can be large,
more than one emission mechanism is involved, and plasma effects are
important. Here, we extend the theory of thermal gyroresonance and free-
free radio emissions in the classical single-temperature Maxwellian
plasma to the case of a multitemperature plasma. The free-free component
is computed using the DEM and temperature-dependent ionization states of
coronal ions, contributions from collisions of electrons with neutral
atoms, the exact Gaunt factor, and the magnetic field effect. For the
gyroresonant component, another measure of the multitemperature plasma
is used, which describes the distribution of the thermal electron
density over temperature. We give representative examples demonstrating
important changes in the emission intensity and polarization due to the
effects considered. The theory is implemented in available computer
code.</description>
</item>
<item>
<title> Coronal Conditions for the Occurrence of Type II Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...913...99K</link>
<description>Type II radio bursts are generally observed in association with flare-
generated or coronal-mass-ejection-driven shock waves. The exact shock
and coronal conditions necessary for the production of type II radio
emission are still under debate. Shock waves are important for the
acceleration of electrons necessary for the generation of the radio
emission. Additionally, the shock geometry and closed field line
topology, e.g., quasi-perpendicular shock regions or shocks interacting
with streamers, play an important role for the production of the
emission. In this study we perform a 3D reconstruction and modeling of a
shock wave observed during the 2014 November 5 solar event. We determine
the spatial and temporal evolution of the shock properties and examine
the conditions responsible for the generation and evolution of type II
radio emission. Our results suggest that the formation and evolution of
a strong, supercritical, quasi-perpendicular shock wave interacting with
a coronal streamer were responsible for producing type II radio
emission. We find that the shock wave is subcritical before and
supercritical after the start of the type II emission. The shock
geometry is mostly quasi-perpendicular throughout the event. Our
analysis shows that the radio emission is produced in regions where the
supercritical shock develops with an oblique to quasi-perpendicular
geometry.</description>
</item>
<item>
<title> Energy Budget of Plasma Motions, Heating, and Electron Acceleration in a Three-loop Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...913...97F</link>
<description>Nonpotential magnetic energy promptly released in solar flares is
converted to other forms of energy. This may include nonthermal energy
of flare-accelerated particles, thermal energy of heated flaring plasma,
and kinetic energy of eruptions, jets, upflows/downflows, and stochastic
(turbulent) plasma motions. The processes or parameters governing
partitioning of the released energy between these components are an open
question. How these components are distributed between distinct flaring
loops and what controls these spatial distributions are also unclear.
Here, based on multiwavelength data and 3D modeling, we quantify the
energy partitioning and spatial distribution in the well-observed
SOL2014-02-16T064620 solar flare of class C1.5. Nonthermal emission of
this flare displayed a simple impulsive single-spike light curve lasting
about 20 s. In contrast, the thermal emission demonstrated at least
three distinct heating episodes, only one of which was associated with
the nonthermal component. The flare was accompanied by upflows and
downflows and substantial turbulent velocities. The results of our
analysis suggest that (i) the flare occurs in a multiloop system that
included at least three distinct flux tubes; (ii) the released magnetic
energy is divided unevenly between the thermal and nonthermal components
in these loops; (iii) only one of these three flaring loops contains an
energetically important amount of nonthermal electrons, while two other
loops remain thermal; (iv) the amounts of direct plasma heating and that
due to nonthermal electron loss are comparable; and (v) the kinetic
energy in the flare footpoints constitutes only a minor fraction
compared with the thermal and nonthermal energies.</description>
</item>
<item>
<title> The active region source of a type III radio storm observed by Parker Solar Probe during encounter 2</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...650A...7H</link>
<description>Context. We investigated the source of a type III radio burst storm
during encounter 2 of NASA's Parker Solar Probe (PSP) mission. &lt;BR /&gt;
Aims: It was observed that in encounter 2 of NASA's PSP mission there
was a large amount of radio activity and, in particular, a noise storm
of frequent, small type III bursts from 31 March to 6 April 2019. Our
aim is to investigate the source of these small and frequent bursts. &lt;BR
/&gt; Methods: In order to do this, we analysed data from the Hinode EUV
Imaging Spectrometer, PSP FIELDS, and the Solar Dynamics Observatory
Atmospheric Imaging Assembly. We studied the behaviour of active region
12737, whose emergence and evolution coincides with the timing of the
radio noise storm and determined the possible origins of the electron
beams within the active region. To do this, we probed the dynamics,
Doppler velocity, non-thermal velocity, FIP bias, and densities, and
carried out magnetic modelling. &lt;BR /&gt; Results: We demonstrate that
although the active region on the disc produces no significant flares,
its evolution indicates it is a source of the electron beams causing the
radio storm. They most likely originate from the area at the edge of the
active region that shows strong blue-shifted plasma. We demonstrate that
as the active region grows and expands, the area of the blue-shifted
region at the edge increases, which is also consistent with the
increasing area where large-scale or expanding magnetic field lines from
our modelling are anchored. This expansion is most significant between 1
and 4 April 2019, coinciding with the onset of the type III storm and
the decrease of the individual burst's peak frequency, indicating that
the height at which the peak radiation is emitted increases as the
active region evolves.</description>
</item>
<item>
<title> Periodicities in an active region correlated with Type III radio bursts observed by Parker Solar Probe</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...650A...6C</link>
<description>Context. Periodicities have frequently been reported across many
wavelengths in the solar corona. Correlated periods of ~5 min,
comparable to solar p-modes, are suggestive of coupling between the
photosphere and the corona. &lt;BR /&gt; Aims: Our study investigates whether
there are correlations in the periodic behavior of Type III radio bursts
which are indicative of nonthermal electron acceleration processes, and
coronal extreme ultraviolet (EUV) emission used to assess heating and
cooling in an active region when there are no large flares. &lt;BR /&gt;
Methods: We used coordinated observations of Type III radio bursts from
the FIELDS instrument on Parker Solar Probe (PSP), of EUV emissions by
the Solar Dynamics Observatory (SDO) Atmospheric Imaging Assembly (AIA)
and white light observations by SDO Helioseismic and Magnetic Image
(HMI), and of solar flare X-rays by Nuclear Spectroscopic Telescope
Array (NuSTAR) on April 12, 2019. Several methods for assessing
periodicities are utilized and compared to validate periods obtained.
&lt;BR /&gt; Results: Periodicities of ~5 min in the EUV in several areas of
an active region are well correlated with the repetition rate of the
Type III radio bursts observed on both PSP and Wind. Detrended 211 and
171  light curves show periodic profiles in multiple locations, with
171  peaks sometimes lagging those seen in 211 . This is suggestive of
impulsive events that result in heating and then cooling in the lower
corona. NuSTAR X-rays provide evidence for at least one microflare
during the interval of Type III bursts, but there is not a one-to-one
correspondence between the X-rays and the Type III bursts. Our study
provides evidence for periodic acceleration of nonthermal electrons
(required to generate Type III radio bursts) when there were no
observable flares either in the X-ray data or the EUV. The acceleration
process, therefore, must be associated with small impulsive events,
perhaps nanoflares.</description>
</item>
<item>
<title> Temporal and Spatial Association Between a Solar Flare, CME, and Radio Burst on 19 November 2013</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...77S</link>
<description>We present multi-wavelength and multi-instrument observations and
analysis of a major X 1.0 class flare, radio burst, halo coronal mass
ejection (CME), and loop eruption from the solar active region NOAA
11893 on 19 November 2013 (SOL2013-11-19T10:26). The aim of this work is
twofold: The first aim to study the evolution of the loop eruption and
the second is to find the link between this eruption and radio
emissions. Initial signatures of eruption from the solar source region
are confirmed using observations from the Atmospheric Imaging Assembly
onboard the Solar Dynamics Observatory in the hot channel at 94 
wavelength. These observations confirm that the source of the CME was
associated with a magnetic-loop eruption, which was visible before the
flare initiation. The photospheric magnetic configuration displayed a
complex network of   sunspots. After the eruption, a CME was observed
by the Solar and Heliospheric Observatory/Large Angle and Spectrometric
Coronagraph with linear speed and acceleration of 740 kms&lt;SUP&gt;1&lt;/SUP&gt;
and 2 ms&lt;SUP&gt;2&lt;/SUP&gt;, respectively. Dynamic radio-spectrum observation
from the Learmonth Observatory in the metric frequency range shows Type-
III and Type-II radio emissions that reveal the field-line opening and
coronal-shock formation closely associated with the CME. From the metric
Type-II radio observation and assuming Newkirk's density model, we
estimate the shock formation height range of 1.14 -1.54 &lt;SUB&gt;R&lt;/SUB&gt;
with the corresponding shock speed (650 kms&lt;SUP&gt;1&lt;/SUP&gt;). With the
heliographic observations from the Nanay heliograph at different
frequencies we could disentangle Type-II bursts from Type-III bursts.
Likely, the Type-III burst would correspond to the loop eruption while
the Type-II comes from the northern flank of the CME.</description>
</item>
<item>
<title> A Quarter Century of Wind Spacecraft Discoveries</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RvGeo..5900714W</link>
<description>The Wind spacecraft, launched on November 1, 1994, is a critical element
in NASA's Heliophysics System Observatory (HSO) - a fleet of spacecraft
created to understand the dynamics of the Sun-Earth system. The
combination of its longevity (&gt;25 years in service), its diverse
complement of instrumentation, and high resolution and accurate
measurements has led to it becoming the "standard candle" of solar wind
measurements. Wind has over 55 selectable public data products with over
1,100 total data variables (including OMNI data products) on
SPDF/CDAWeb alone. These data have led to paradigm shifting results in
studies of statistical solar wind trends, magnetic reconnection, large-
scale solar wind structures, kinetic physics, electromagnetic
turbulence, the Van Allen radiation belts, coronal mass ejection
topology, interplanetary and interstellar dust, the lunar wake, solar
radio bursts, solar energetic particles, and extreme astrophysical
phenomena such as gamma-ray bursts. This review introduces the mission
and instrument suites then discusses examples of the contributions by
Wind to these scientific topics that emphasize its importance to both
the fields of heliophysics and astrophysics.</description>
</item>
<item>
<title> BoxCox multi-output linear regression for 10.7 cm solar radio flux prediction</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21...94C</link>
<description>We consider the problem of predicting the mid-term daily 10.7cm solar
radio flux (F10.7), a widely-used solar activity index. A novel approach
is proposed for this task, in which BoxCox transformation with a proper
parameter is first applied to make the data satisfy the property of
homoscedasticity that is a basic assumption of regression models, and
then a multi-output linear regression model is used to predict future
F10.7 values. The experiment shows that the BoxCox transformation
significantly improves the predictive performance and our new approach
works substantially better than the prediction from the US Airforce and
other alternative methods like Auto-regressiveModel, Multi-layer
Perceptron, and Support Vector Regression.</description>
</item>
<item>
<title> Solar radio filtering algorithm based on improved long short-term memory</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21...79D</link>
<description>The effective observation of burst events in solar radio research has
been impeded by various interference signals, especially interference
signals with a wide frequency range and high intensity, as they can
partially or completely obscure the observation of burst events. Image
processing methods that directly remove the interference signal channels
and subtract the average of the interference signal channel are not
suitable for processing all types of interference signals. This paper
proposes the use of a specific kind of recurrent neural networks, called
long short-term memory networks, to predict the value of the radio
frequency interference signals with high intensity of the burst event in
the solar radio spectrum. The predicted interference can then be removed
in accordance with the principle that signals can be linearly added.
Therefore, predicted value is subtracted from the data containing the
burst event signals and the RFI signals (The radio frequency
interference signals to be processed in this article refer to the signal
of the broadcast signal that can be received in the frequency range, the
signal transmitted by the mobile phone, and the signal transmitted by
the sea vessel, and the like) to remove the interference. Then, in order
to reduce the error caused by the stepwise prediction in the network and
further improve the prediction accuracy, this paper analyzes the
characteristics of the value of the radio interference and applies the
digital mapping method to convert the prediction problem into the
classification problem in the time series. The experimental results show
that the proposed method can effectively remove the radio interference
in the solar spectrum and clearly show the burst events.</description>
</item>
<item>
<title> Survey of electron density changes in the daytime ionosphere over the Arecibo Observatory due to lightning and solar flares</title>
<link>https://ui.adsabs.harvard.edu/abs/2021NatSR..1110250D</link>
<description>Optical observations of transient luminous events and remote-sensing of
the lower ionosphere with low-frequency radio waves have demonstrated
that thunderstorms and lightning can have substantial impacts in the
nighttime ionospheric D region. However, it remains a challenge to
quantify such effects in the daytime lower ionosphere. The wealth of
electron density data acquired over the years by the Arecibo Observatory
incoherent scatter radar (ISR) with high vertical spatial resolution
(300-m in the present study), combined with its tropical location in a
region of high lightning activity, indicate a potentially transformative
pathway to address this issue. Through a systematic survey, we show that
daytime sudden electron density changes registered by Arecibo's ISR
during thunderstorm times are on average different than the ones
happening during fair weather conditions (driven by other external
factors). These changes typically correspond to electron density
depletions in the D and E region. The survey also shows that these
disturbances are different than the ones associated with solar flares,
which tend to have longer duration and most often correspond to an
increase in the local electron density content.</description>
</item>
<item>
<title> Fine structure of type III solar radio bursts from Langmuir wave motion in turbulent plasma</title>
<link>https://ui.adsabs.harvard.edu/abs/2021NatAs...5..796R</link>
<description>The Sun frequently accelerates near-relativistic electron beams that
travel out through the solar corona and interplanetary space.
Interacting with their plasma environment, these beams produce type III
radio burststhe brightest astrophysical radio sources seen from Earth.
The formation and motion of type III fine frequency structures is a
puzzle, but is commonly believed to be related to plasma turbulence in
the solar corona and solar wind. Combining a theoretical framework with
kinetic simulations and high-resolution radio type III observations
using the Low-Frequency Array, we quantitatively show that the fine
structures are caused by the moving intense clumps of Langmuir waves in
a turbulent medium. Our results show how type III fine structure can be
used to remotely analyse the intensity and spectrum of compressive
density fluctuations, and can infer ambient temperatures in
astrophysical plasma, substantially expanding the current diagnostic
potential of solar radio emission.</description>
</item>
<item>
<title> The lower dayside ionosphere of Mars from 14 years of MaRS radio science observations</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Icar..35914213P</link>
<description>This work uses a subset of "quiet" MaRS ionospheric dayside observations
(MaRS&lt;SUB&gt;quiet&lt;/SUB&gt;, 2004-2017) and a 1-D photochemical model (IonA-2)
to investigate the potential formation processes of the excess electron
densities merged with the base of the main ionosphere (Mm). 42% of the
investigated MaRS observations contain identified Mm, which occur in a
large variety of shapes ranging from smoothly decreasing electron
densities to peak structures below the base of M1. The Mm appear over
the full range of accessible solar zenith angles (50 - 90) and are
found between approximately 70 and 110 km altitude. Their base is found
on average deeper in the atmosphere than the base of the averaged
undisturbed MaRS electron density profiles. This indicates a dependence
of the Mm formation on energy sources that penetrate deep into the
atmosphere. This is supported by a strong positive correlation with
increasing solar activity when solar flares, coronal mass ejections, and
enhanced short solar X-ray and Ly- intensities are more common. No
relationship is found between the Mm occurrence rate and the
magnitude/inclination of the weak crustal crustal magnetic field in
MaRS&lt;SUB&gt;quiet&lt;/SUB&gt;. &lt;P /&gt;Investigations with the IonA-2 photochemical
model for undisturbed and flare conditions show that the ionization of
the local neutral atmosphere by solar X-ray radiation &lt;2 nm provides a
satisfying explanation for detected Mm features with smoothly decreasing
electron densities below the M1 base in combination with moderate slopes
of the lower Mm region &lt;SUB&gt;Mm&lt;/SUB&gt; and altitudes of the lower
boundary h&lt;SUB&gt;L,S&lt;/SUB&gt;. While sufficient ionization energy reaches the
region of interest during flares, no Mm features with peaks below the M1
base occur in any of the model electron density profiles. This supports
the conclusion that the subgroup of merged excess electron densities
with peaks or intermediate features (Mi) below the M1 base must have an
origin different from the sole variability of solar X-ray radiation
during undisturbed and solar flare conditions. The size of the
identified Mm makes an exclusive meteoric origin of the Mm peak
structures unlikely. &lt;P /&gt;It is indicative from the IonA-2 model results
that the general increase/decrease of solar X-ray &lt;2 nm leads to a
correlated response of the Mm region. The sporadic occurrence of the
merged excess electron densities in the MaRS observations is therefore
assumed to be a combination of observational (increased observation
noise level compared to the available amount of X-ray radiation &lt;2 nm,
shift of the lower baseline by ionospheric deviations from radial
symmetry) and environmental (e.g. variations in solar X-ray) factors.</description>
</item>
<item>
<title> Medium-term Predictions of F10.7 and F30 cm Solar Radio Flux with the Adaptive Kalman Filter</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJS..254....9P</link>
<description>The solar radio flux at F10.7 and F30 cm is required by most models
characterizing the state of the Earth's upper atmosphere, such as the
thermosphere and ionosphere, to specify satellite orbits, re-entry
services, collision avoidance maneuvers, and modeling of the evolution
of space debris. We develop a method called RESONANCE (Radio Emissions
from the Sun: ONline ANalytical Computer-aided Estimator) for the
prediction of the 13-month smoothed monthly mean F10.7 and F30 indices
1-24 months ahead. The prediction algorithm has three steps. First, we
apply a 13-month optimized running mean technique to effectively reduce
the noise in the radio flux data. Second, we provide initial predictions
of the F10.7 and F30 indices using the McNish-Lincoln method. Finally,
we improve these initial predictions by developing an adaptive Kalman
filter with identification of the error statistics. The rms error of
predictions with lead times from 1 to 24 months is 5-27 solar flux units
(sfu) for the F10.7 index and 3-16 sfu for F30, which statistically
outperforms current algorithms in use. The proposed approach based on
the Kalman filter is universal and can be applied to improve the initial
predictions of a process under study provided by any other forecasting
method. Furthermore, we present a systematic evaluation of re-entry
forecast as an application to test the performance of F10.7 predictions
on past ESA re-entry campaigns for payloads, rocket bodies, and space
debris that re-entered from 2006 to 2019 June. The test results
demonstrate that the predictions obtained by RESONANCE in general also
lead to improvements in the forecasts of re-entry epochs.</description>
</item>
<item>
<title> Statistics of Low Frequency Cutoffs for Type III Radio Bursts Observed by Parker Solar Probe during Its Encounters 1-5</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...913L...1M</link>
<description>The low frequency cutoffs f&lt;SUB&gt;lo&lt;/SUB&gt; and the observed plasma
frequency f&lt;SUB&gt;p&lt;/SUB&gt; of 176 type III radio bursts are investigated in
this paper. These events are observed by the Parker Solar Probe when it
is in the encounter phase from the first to the fifth orbit. The result
shows that the distribution of cutoffs f&lt;SUB&gt;lo&lt;/SUB&gt; is widely spread
between 200 kHz and 1.6 MHz. While the plasma frequency f&lt;SUB&gt;p&lt;/SUB&gt; at
the spacecraft is between 50 and 250 kHz, which is almost all smaller
than f&lt;SUB&gt;lo&lt;/SUB&gt;. The result also shows that the maximum probability
distribution of f&lt;SUB&gt;lo&lt;/SUB&gt; (680 kHz) is remarkably higher than that
observed by Ulysses and Wind (100 kHz) in previous research. Three
possible reasons, i.e., solar activity intensity, event electing
criteria, and radiation attenuation effect, are also preliminarily
discussed.</description>
</item>
<item>
<title> Observational Evidence for Beat Phenomenon in Complex Solar Type III Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...912...61T</link>
<description>We present new observational evidence for one of the most important
three wave interactions, called the electrostatic decay instability
(ESD) $L\to {L}^{{\prime} }+S$ in the source regions of complex solar
type III radio bursts (L is the electron beam-excited Langmuir wave, and
${L}^{{\prime} }$ and S are the ESD excited daughter Langmuir and ion
sound waves, respectively). The STEREO in situ wave observations in the
source regions of complex type III bursts show that Langmuir waves often
occur as one-dimensional magnetic field aligned beat-type wave packets,
with peak intensities well in excess of the threshold for excitation of
ESD, and with spectra containing (a) two closely spaced narrow peaks (L
and ${L}^{{\prime} }$ ) corresponding probably to the beating modes
responsible for the beat patterns at frequencies very close to the local
electron plasma frequency, f&lt;SUB&gt;pe&lt;/SUB&gt;, and (b) narrow peaks at ion
sound frequencies, f&lt;SUB&gt;S&lt;/SUB&gt;, which are very close to beat
frequencies. Using the FFT and higher order spectral techniques, we show
that the frequency, wavevector and phase resonance conditions required
for excitation of ESD are well satisfied for these wave packets, and the
speeds of electron beams derived from the resonance conditions agree
reasonably well with those derived from the drift rates of the
associated type III events. We also show that the merging of (L) and (
${L}^{{\prime} }$ ) most probably is the excitation mechanism of the
second harmonic radio emission ${T}_{2{f}_{{pe}}}$ of these type III
bursts.</description>
</item>
<item>
<title> comparison with IRI-2016 and IRI-2012 models</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ap&amp;SS.366...46P</link>
<description>In this study the statistics of ionospheric total electron content
(TEC), derived from a GSV4004B dual-frequency Global Positioning System
(GPS) receiver at Agartala station (23.450N, 91.150E) located in
northern equatorial ionization anomaly (EIA) crest region of the Indian
subcontinent, is reported with a performance analysis of IRI-2016 and
IRI-2012 models during the ascending, maxima, declining and minima
phases (2013-2018) of the solar cycle 24. Variations of model total
electron content, as obtained from the IRI-2016 and IRI-2012 for the
three options of topside electron density namely NeQuick, IRI 2001 and
IRI 01-corr, are compared with the observed total electron content
during different periods of interest viz. monthly, seasonal, annual and
the correlations with solar activity parameters viz. sunspot number
(SSN), 10.7 cm solar radio flux (F10.7), solar EUV flux, are also
investigated. All the three options of IRI-2016 and IRI-2012 models show
an earlier occurrence of diurnal maximum total electron content, as
compared to the observed diurnal maximum GPS total electron content,
throughout all the months during the complete period of observation. As
the solar activity decreases (from 2015 to 2018), the model starts
underestimating GPS total electron content, which becomes significantly
high during the very low solar activity period of 2017-18 for all the
months. IRI-2016 model underestimates the GPS total electron content
before the hours of diurnal maximum and overestimates after the hours of
diurnal maximum in the years from 2013-2018. IRI-2012 model
underestimates the GPS total electron content before the hours of
diurnal maximum and overestimates after the hours of diurnal maximum in
the years from 2013-17 but overestimate during the whole day in the year
of 2018. Overestimation by IRI-2012 is much more than that by IRI-2016
in the year of 2018. Predictions given by IRI-2016 are better than that
given by IRI-2012 for our region. The seasonal mean maximum total
electron content values are highest during the spring equinox months and
lowest during the winter months except the year of 2014 and 2013. The
correlation analysis, between the GPS total electron content and solar
indices, show that the correlation coefficient is higher for the solar
EUV flux, as compared to the sunspot number (SSN) and 10.7 cm solar
radio flux (F10.7).</description>
</item>
<item>
<title> First Type III Solar Radio Bursts of Solar Cycle 25</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...57K</link>
<description>The minimum of the previous solar cycle, Solar Cycle 24, occurred in
December 2019, which also marked the start of the new Solar Cycle 25.
The first radio bursts of the new solar cycle were observed in the
spring season 2020. In this work we will present three type III solar
bursts which were observed in May and June 2020 at radio frequencies
between 18 - 90 MHz. There are two radio observatories in Finland that
are capable of doing low-frequency solar radio observations: Aalto
University Metshovi Radio Observatory (MRO) and Kilpisjrvi Atmospheric
Imaging Receiver Array (KAIRA) of the Sodankyl Geophysical Observatory,
University of Oulu. The instruments of the two institutes have different
design and characteristics, and they operate in rather different radio
interference environments. We will compare simultaneous observations
from these two instruments and we will also discuss the properties of
these type III solar bursts.</description>
</item>
<item>
<title> An investigation of flare emissions at multiple wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21...66L</link>
<description>We report multi-wavelength observations of four solar flares on 2014
July 07. We firstly select these flares according to the soft X-ray
(SXR) and extreme ultraviolet (EUV) emissions recorded by the Extreme
Ultraviolet Variability Experiment and Geostationary Orbiting
Environmental Satellites. Then their locations and geometries are
identified from the full-disk images measured by the Atmospheric Imaging
Assembly (AIA), and the time delays among the light curves in different
channels are identified. The electron number densities are estimated
using the differential emission measure method. We find that three of
four flares show strong emissions in SXR channels and high temperature
(&gt;6 MK) EUV wavelengths during the impulsive phase, i.e., AIA 131  and
94 , and then they emit peak radiation subsequently in the middle
temperature (0.6-3 MK) EUV channels. Moreover, they last for a long
time and have smaller electron densities, which are probably driven by
the interaction of hot diffuse flare loops. Only one flare emits
radiation at almost the same time in all the observed wavelengths, lasts
for a relatively short time, and has a larger electron density. It is
also accompanied by a type III radio burst. The bright emission at the
EUV channel could be corresponding to the associated erupting filament.</description>
</item>
<item>
<title> Temporal variation of solar flare index during solar cycles 21 - 24</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RAA....21...53R</link>
<description>The present investigation attempts to quantify the temporal variation of
Solar Flare Index (SFI) with other activity indices during solar cycles
21 - 24 by using different techniques such as linear regression,
correlation, cross-correlation with phase lag-lead, etc. Different Solar
Activity Indices (SAI) considered in this present study are Sunspot
Number (SSN), 10.7 cm Solar Radio Flux (F10.7), Coronal Index (CI) and
MgII Core-to-Wing Ratio (MgII). The maximum cycle amplitude of SFI and
considered SAI has a decreasing trend from solar cycle 22, and cycle 24
is the weakest solar cycle among all other cycles. The SFI with SSN,
F10.7, CI and MgII shows hysteresis during all cycles except for solar
cycle 22 where both paths for ascending and descending phases are
intercepting each other, thereby representing a phase reversal. A
positive hysteresis circulation exists between SFI and considered SAI
during solar cycles 22 and 23, whereas a negative circulation exists in
cycles 21 and 24. SFI has a high positive correlation with coefficient
values of 0.92, 0.94, 0.84 and 0.81 for SSN, F10.7, CI and MgII
respectively. According to cross-correlation analysis, SFI has a phase
lag with considered SAI during an odd-number solar cycle (solar cycles
21 and 23) but no phase lag/lead during an even-numbered solar cycle
(solar cycles 22 and 24). However, the entire smoothed monthly average
SFI data indicate an in-phase relationship with SSN, F10.7 and MgII, and
a one-month phase lag with CI. The presence of those above
characteristics strongly confirms the outcomes of different research
work with various solar indices and the highest correlation exists
between SFI and SSN as well as F10.7 which establishes that SFI may be
considered as one of the prime activity indices to interpret the
characteristics of the Sun's active region as well as for more accurate
short-range or long-range forecasting of solar events.</description>
</item>
<item>
<title> Electron Acceleration during Macroscale Magnetic Reconnection</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PhRvL.126m5101A</link>
<description>The first self-consistent simulations of electron acceleration during
magnetic reconnection in a macroscale system are presented. Consistent
with solar flare observations, the spectra of energetic electrons take
the form of power laws that extend more than two decades in energy. The
drive mechanism for these nonthermal electrons is Fermi reflection in
growing and merging magnetic flux ropes. A strong guide field suppresses
the production of nonthermal electrons by weakening the Fermi drive
mechanism. For a weak guide field the total energy content of nonthermal
electrons dominates that of the hot thermal electrons even though their
number density remains small. Our results are benchmarked with the hard
x-ray, radio, and extreme ultraviolet observations of the X8.2-class
solar flare on September 10, 2017.</description>
</item>
<item>
<title> Low Radio Frequency Observations from the Moon Enabled by NASA Landed Payload Missions</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PSJ.....2...44B</link>
<description>A new era of exploration of the low radio frequency universe from the
Moon will soon be underway with landed payload missions facilitated by
NASA's Commercial Lunar Payload Services (CLPS) program. CLPS landers
are scheduled to deliver two radio science experiments, Radio wave
Observations at the Lunar Surface of the photoElectron Sheath (ROLSES)
to the nearside and Lunar Surface Electromagnetics Experiment (LuSEE) to
the farside, beginning in 2021. These instruments will be pathfinders
for a 10 km diameter interferometric array, Farside Array for Radio
Science Investigations of the Dark ages and Exoplanets (FARSIDE),
composed of 128 pairs of dipole antennas proposed to be delivered to the
lunar surface later in the decade. ROLSES and LuSEE, operating at
frequencies from 100 kHz to a few tens of megahertz, will investigate
the plasma environment above the lunar surface and measure the fidelity
of radio spectra on the surface. Both use electrically short, spiral-
tube deployable antennas and radio spectrometers based upon previous
flight models. ROLSES will measure the photoelectron sheath density to
better understand the charging of the lunar surface via photoionization
and impacts from the solar wind, charged dust, and current anthropogenic
radio frequency interference. LuSEE will measure the local magnetic
field and exo-ionospheric density, interplanetary radio bursts, Jovian
and terrestrial natural radio emission, and the galactic synchrotron
spectrum. FARSIDE, and its precursor risk-reduction six antenna-node
array PRIME, would be the first radio interferometers on the Moon.
FARSIDE would break new ground by imaging radio emission from coronal
mass ejections (CME) beyond 2R&lt;SUB&gt;&lt;/SUB&gt;, monitor auroral radiation
from the B-fields of Uranus and Neptune (not observed since Voyager),
and detect radio emission from stellar CMEs and the magnetic fields of
nearby potentially habitable exoplanets.</description>
</item>
<item>
<title> Study of the truncation strategy in the FPGA of a solar radio digital receiver</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PASJ...73..439Y</link>
<description>Computation resource is the limiting factor in higher operational
accuracy of field-programmable gate arrays (FPGAs) in solar radio
digital receivers. The data truncation strategy which determines the
accuracy of data is then the essential technology in the design of a
receiving system. Based on the solar radio spectrometer (dual channel,
14 bit, 1.25 gigasamples per second) at the Chashan Solar Radio
Observatory (CSO), this paper presents a data truncation strategy which
can realize real-time solar radio observation (35-40 GHz) with high time
and frequency resolution as well as a large dynamic range, and at the
same time saves the computation resource to a large extent. Simulations
of truncations during signal processing are carried out in MATLAB, and
the best truncation mechanisms are deduced for windowing and fast
Fourier transform (FFT). Using the simulation results, the best
truncation strategies have been implemented in the solar radio receiver
at CSO with the result that the best truncation bits for the windowing
operation are [27 : 14], with an error of 2.5  10&lt;SUP&gt;-4&lt;/SUP&gt;, and the
best truncation bits for the FFT output are [20 : 5] with an error of
1.5  10&lt;SUP&gt;-3&lt;/SUP&gt;. Compared with the processing of full-precision
data, occupation of the computation resources in the FPGA can be reduced
significantly. For instance, the lookup table, lookup table RAM, flip
flop, and digital signal processing slices are reduced by 7.36%, 14.65%,
8.38%, and 24.94%, respectively, which guarantees broad-band real-time
solar radio observations (35-40 GHz).</description>
</item>
<item>
<title> How modernized and strengthened GPS signals enhance the system performance during solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021GPSS...25...46Y</link>
<description>A Solar Radio Burst (SRB) is one of the most severe natural hazards
affecting the performance of the global navigation satellite systems
(GNSS). Considering the influence of different threat factors, the GNSS
developers upgrade the systems to amend the accuracy and noise-proof
features of the systems. In particular, GPS gradually replaces "old"
satellites (GPS IIA, GPS IIR-A, GPS IIR-B) with new-generation equipment
(GPS IIR-M, GPS IIF, GPS III) featured by an increase in the emitted
signal power at L2 frequency and by new civilian codes. In this work,
based on examples of the extreme SRB of September 24, 2011, and the
severe SRB of September 6, 2017, we study how such modernization can
improve the GPS system performance during solar flares accompanied by
intense SRB. We recorded SRB-related drops in signal strength (S), which
were 7.5/0 dB-Hz for the S1C, 10/7 dB-Hz for the S2X, 17/8 dB-Hz for the
S2W and 9/7.5 for the S5/S5X in 2011/2017 correspondingly. The drop in
the S2W signal strength for the modernized blocks was comparable in
amplitude to those of the "old" blocks. However, the modernized
IIR-M/IIF blocks were featured by about 5 dB-Hz higher signal strength.
This resulted in a double and triple decrease in loss-of-lock density
for the IIR-M/IIF satellites in 2011 and 2017, respectively, as compared
to IIA/IIR-A during SRBs. Therefore, the increase in the emitted signal
power and new civilian codes potentially enhance the stability of the
GPS operation.</description>
</item>
<item>
<title> Solar Radio Burst Effects on Radio- and Radar-Based Systems</title>
<link>https://ui.adsabs.harvard.edu/abs/2021GMS...262..141G</link>
<description>Radio emission from solar flares can attain such high flux density that
the Sun becomes the dominant source of broadband radio noise in the
terrestrial environment. The effects of this radio noise on wireless
communication and navigation systems can take many forms, depending on
the design and operation of the affected system. These effects can be of
special concern for regional or global systems, since the effects can
occur simultaneously over the entire sunlit hemisphere of Earth. This
chapter reviews the origin of solar radio bursts, the threat they pose
based on statistics of the flux-density distribution of such events vs.
frequency, and some of the effects that have been documented in the
literature. The chapter concludes with a discussion of the potential
impacts on current and future technology and how these impacts can be
mitigated (1) through improved radio monitoring of the Sun in both
circular polarizations to supply meaningful real-time warnings, (2)
through improved scientific understanding of the solar phenomena
underlying the radio bursts, and (3) through improved system design that
takes account of solar radio noise.</description>
</item>
<item>
<title> Possible Evidence of a Termination Shock</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...911....4L</link>
<description>Solar flare termination shocks have been suggested as one of the viable
mechanisms for accelerating electrons and ions to high energies.
Observational evidence of such shocks, however, remains rare. Using
radio dynamic spectroscopic imaging of a long-duration C1.9 flare
obtained by the Karl G. Jansky Very Large Array (VLA), Chen et al.
suggested that a type of coherent radio bursts, referred to as
"stochastic spike bursts," were radio signatures of nonthermal electrons
interacting with myriad density fluctuations at the front of a flare
termination shock. Here we report another stochastic spike burst event
recorded during the extended energy release phase of a long-duration
M8.4-class eruptive flare on 2012 March 10. VLA radio spectroscopic
imaging of the spikes in 1.0-1.6 GHz shows that, similar to the case of
Chen et al., the burst centroids form an extended, 10-long structure
in the corona. By combining extreme-ultraviolet imaging observations of
the flare from two vantage points with hard X-ray and ultraviolet
observations of the flare ribbon brightenings, we reconstruct the flare
arcade in three dimensions. The results show that the spike source is
located at 60 Mm above the flare arcade, where a diffuse supra-arcade
fan and multitudes of plasma downflows are present. Although the flare
arcade and ribbons seen during the impulsive phase do not allow us to
clearly understand how the observed spike source location is connected
to the flare geometry, the cooling flare arcade observed 2 hr later
suggests that the spikes are located in the above-the-loop-top region,
where a termination shock presumably forms.</description>
</item>
<item>
<title> Quasi-periodic Particle Acceleration in a Solar Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...910..123C</link>
<description>A common feature of electromagnetic emission from solar flares is the
presence of intensity pulsations that vary as a function of time. Known
as quasi-periodic pulsations (QPPs), these variations in flux appear to
include periodic components and characteristic timescales. Here, we
analyze a GOES M3.7 class flare exhibiting pronounced QPPs across a
broad band of wavelengths using imaging and time series analysis. We
identify QPPs in the time series of X-ray, low-frequency radio, and
extreme ultraviolet (EUV) wavelengths using wavelet analysis, and
localize the region of the flare site from which the QPPs originate via
X-ray and EUV imaging. It was found that the pulsations within the 171
, 1600 , soft X-ray, and hard X-ray light curves yielded similar
periods of ${122}_{-22}^{+26}$ &lt;!-- --&gt; s, ${131}_{-27}^{+36}$ &lt;!-- --&gt;
s, ${123}_{-26}^{+11}$ &lt;!-- --&gt; s, and ${137}_{-56}^{+49}$ &lt;!-- --&gt; s,
respectively, indicating a common progenitor. The low-frequency radio
emission at 2.5 MHz contained a longer period of 231 s. Imaging
analysis indicates that the location of the X-ray and EUV pulsations
originates from a hard X-ray footpoint linked to a system of nearby open
magnetic field lines. Our results suggest that intermittent particle
acceleration, likely due to "bursty" magnetic reconnection, is
responsible for the QPPs. The precipitating electrons accelerated toward
the chromosphere produce the X-ray and EUV pulsations, while the
escaping electrons result in low-frequency radio pulses in the form of
type III radio bursts. The modulation of the reconnection process,
resulting in episodic particle acceleration, explains the presence of
these QPPs across the entire spatial range of flaring emission.</description>
</item>
<item>
<title> Narrowband Spikes Observed during the 2013 November 7 Flare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...910..108K</link>
<description>Narrowband spikes have been observed in solar flares for several
decades. However, their exact origin is still discussed. To contribute
to understanding of these spikes, we analyze the narrowband spikes
observed in the 800-2000 MHz range during the impulsive phase of the
2013 November 7 flare. In the radio spectrum, the spikes started with
typical broadband clouds of spikes, and then their distribution in
frequencies changed into unique, very narrow bands having noninteger
frequency ratios. We successfully fitted frequencies of these narrow
spike bands by those, calculating dispersion branches and growth rates
of the Bernstein modes. For comparison, we also analyzed the model where
the narrow bands of spikes are generated at the upper-hybrid
frequencies. Using both models, we estimated the plasma density and
magnetic field in spike sources. Then, the models are discussed, and
arguments in favor of the model with the Bernstein modes are presented.
Analyzing frequency profiles of this spike event by the Fourier method,
we found the power-law spectra with the power-law indices varying in the
-0.8 to -2.75 interval. Because at some times this power-law index was
close to the Kolmogorov spectral index (-5/3), we propose that the
spikes are generated through the Bernstein modes in turbulent plasma
reconnection outflows or directly in the turbulent magnetic reconnection
of solar flares.</description>
</item>
<item>
<title> comparison based on CTIPe model simulations and satellite measurements</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AnGeo..39..341V</link>
<description>The ionospheric total electron content (TEC) provided by the
International GNSS Service (IGS) and the TEC simulated by the Coupled
Thermosphere Ionosphere Plasmasphere Electrodynamics (CTIPe) model have
been used to investigate the delayed ionospheric response against solar
flux and its trend during the years 2011 to 2013. The analysis of the
distinct low-latitude and midlatitude TEC response over 15 E shows a
better correlation of observed TEC and the solar radio flux index F10.7
in the Southern Hemisphere compared to the Northern Hemisphere. Thus, a
significant hemispheric asymmetry is observed. &lt;P /&gt;The ionospheric
delay estimated using model-simulated TEC is in good agreement with the
delay estimated for observed TEC against the flux measured by the Solar
Dynamics Observatory (SDO) extreme ultraviolet (EUV) Variability
Experiment (EVE). The average delay for the observed (modeled) TEC is
17(16) h. The average delay calculated for observed and modeled TEC is 1
and 2 h longer in the Southern Hemisphere compared to the Northern
Hemisphere. &lt;P /&gt;Furthermore, the observed TEC is compared with the
modeled TEC simulated using the SOLAR2000 and EUVAC flux models within
CTIPe over northern and southern hemispheric grid points. The analysis
suggests that TEC simulated using the SOLAR2000 flux model overestimates
the observed TEC, which is not the case when using the EUVAC flux model.</description>
</item>
<item>
<title> LOFAR imaging of the solar corona during the 2015 March 20 solar eclipse</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...648A..43R</link>
<description>The solar corona is a highly-structured plasma which can reach
temperatures of more than 2 MK. At low frequencies (decimetric and
metric wavelengths), scattering and refraction of electromagnetic waves
are thought to considerably increase the imaged radio source sizes (up
to a few arcminutes). However, exactly how source size relates to
scattering due to turbulence is still subject to investigation. The
theoretical predictions relating source broadening to propagation
effects have not been fully confirmed by observations due to the rarity
of high spatial resolution observations of the solar corona at low
frequencies. Here, the LOw Frequency ARray (LOFAR) was used to observe
the solar corona at 120180 MHz using baselines of up to 3.5 km
(corresponding to a resolution of 12') during the partial solar
eclipse of 2015 March 20. A lunar de-occultation technique was used to
achieve higher spatial resolution (0.6') than that attainable via
standard interferometric imaging (2.4'). This provides a means of
studying the contribution of scattering to apparent source size
broadening. It was found that the de-occultation technique reveals a
more structured quiet corona that is not resolved from standard imaging,
implying scattering may be overestimated in this region when using
standard imaging techniques. However, an active region source was
measured to be 4' using both de-occultation and standard imaging. This
may be explained by the increased scattering of radio waves by turbulent
density fluctuations in active regions, which is more severe than in the
quiet Sun.</description>
</item>
<item>
<title> The Potential of Near Real Time Solar Observation at 1.4 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SpWea..1902649F</link>
<description>Soil Moisture and Ocean Salinity (SMOS) is an ESA mission observing
Earth at 1.4 GHz with full polarimetry. SMOS images are affected by a
noise of solar origin produced by the Sun appearing in the antenna's
field of view. In this paper, we study whether this solar signal is of
any use for scientific and space weather observations. We analyze the
response of the SMOS Sun brightness temperature (B&lt;SUB&gt;T&lt;/SUB&gt;) to
thermal and nonthermal solar emissions, and compare them with
observations from ground radio telescopes, GOES X ray flares, and CMEs
from SOHO/LASCO. We find that the SMOS Sun B&lt;SUB&gt;T&lt;/SUB&gt; can detect weak
variations in the solar emission such as the progress of the 11 year
activity cycle, the solar rotation, and the thermal emission from
flares. Solar radio bursts detected by the SMOS Sun B&lt;SUB&gt;T&lt;/SUB&gt; are
generally observed during flares from the visible hemisphere of the Sun
that are associated with a CME. We also find a correlation between the
amount of solar flux released at 1.4 GHz and the speed, angular width,
and kinetic energy of the CMEs. We conclude that the unique capability
of the SMOS mission to perform 24 h near real time observation of the
Sun with full polarimetry makes it a promising instrument for monitoring
solar interferences affecting GNSS, radar, and L band wireless
communications, as well as for early assessment of flares
geoeffectiveness. Nevertheless, the current limitations of the solar
data as byproduct of the SMOS data reduction pipeline make it necessary
to create a dedicated product for solar observations.</description>
</item>
<item>
<title> Mid-term Periodicities in Solar Radio Emission Corresponding to Sunspot Number During Solar Cycle 23</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...43A</link>
<description>We present a systematic time-series analysis of solar radio emission in
nine different frequencies to compare with that of daily sunspot number
(SSN) during Solar Cycle 23 (1996-2009). Owing to the contribution from
quiet-sun emission, the total solar fluxes in microwaves do not decrease
as significantly as the sunspot number does during 2006 to 2009. Lomb-
Scargle (LS) and wavelet analysis techniques are employed to infer the
various periodicities present in the time-series data. False alarm
probability (FAP) levels are estimated by the use of background mean
power spectrum in the global wavelet spectrum. The LS periodogram
contains resolved period peaks, some of which are below FAP levels, for
example a well-known rotational period. These peaks are assessed with
global significance levels of the wavelet analysis. In all the data
sets, the period for solar rotational modulation (26-31 days) is
present. The periodogram for the SSN presents Riger type periods
(130-180 days), mid-term periods (300-400 days) and long-term periods
(430-850 days). These periods in north and south are not similar,
especially long term periods are missing in SSN data of the southern
hemisphere. Corresponding to the SSN periodicities, Riger and near
Riger type of oscillations (130-180 days), quasi-biennial periodicities
in the range of 1.2 to 3 years were detected in the time-series data of
radio frequencies. Several of these detected periods fall in the range
of the periods that are suggested to be connected with magneto-Rossby
wave spherical harmonics. Our analysis found reduced power levels in the
LS periodograms of low frequencies because of the fact that these low
frequency emissions originate higher up in the corona with diminishing
contrast to small scale structures.</description>
</item>
<item>
<title> AIM-E auroral ionosphere model adjustment for the regular E layer</title>
<link>https://ui.adsabs.harvard.edu/abs/2021STP.....7a..41N</link>
<description>The E-Region Auroral Ionosphere Model (AIM-E) was developed to determine
the chemical composition and electron density in the auroral zone at
E-layer heights (90150 km). Solar and magnetic activity input
parameters for AIM-E are the three-hour Ap index and the daily solar
radio flux at a wavelength of 10.7 cm (index F10.7). In this paper, we
compare AIM-E calculations of the electron density for the daytime with
EUV radiation spectrum specified in two different ways: 1) the EUV
spectrum theoretically calculated using the F10.7 index as an input
parameter; 2) using TIMED satellite direct measurements of the EUV
spectrum. We have corrected the EUVAC EUV radiation model to specify a
photoionization source in AIM-E. Calculations of regular E-region
critical frequencies show good agreement with the vertical sounding data
from Russian high-latitude stations. Results we obtained make it
possible to do a quick on-line assessment of the regular E layer, using
the daily index F10.7 as an input parameter.</description>
</item>
<item>
<title> History of Space Weather Research and Operation in Japan and New Emphasis in Southeast Asia</title>
<link>https://ui.adsabs.harvard.edu/abs/2021RaSc...5607162I</link>
<description>Japanese space weather research and operation began in 1896 with
research on radio propagation. LF, MF, and HF radio communication used
to be important before the era of communication satellites; however,
they are affected by ionospheric conditions and solar activity. A center
for the research and development of radio systems was established at
Hiraiso, which is now also a space weather observatory for measuring
solar activity, geomagnetic fields, and ionospheric conditions. The need
for space weather information initially decreased in the communication
satellite age, but since the beginning of the 21st century it has been
increasing again with the growing use of positioning satellite systems.
The role of Southeast Asian countries in space weather research has
become important and the range of activities is also growing. The
contribution of these countries to space weather research and operation
is expected to grow in future.</description>
</item>
<item>
<title> Galactic and cosmological fast radio bursts as scaled-up solar radio bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.501.3155W</link>
<description>Fast radio bursts (FRBs) are bright milliseconds radio transients with
large dispersion measures. Recently, FRB 200428 was detected in temporal
coincidence with a hard X-ray flare from the Galactic magnetar SGR
1935+2154, which supports that at least some FRBs are from magnetar
activity. Interestingly, a portion of X-ray flares from magnetar XTE
J1810-197 and the Sun are also accompanied by radio bursts. Many
features of Galactic FRB 200428 and cosmological FRBs resemble solar
radio bursts. However, a common physical origin among FRBs, magnetar
radio pulses, and solar radio bursts has not yet been established. Here,
we report a universal correlation between X-ray luminosity and radio
luminosity over 20 orders of magnitude among solar type III radio
bursts, XTE J1810-197 and Galactic FRB 200428. This universal
correlation reveals that the energetic electrons that produce the X-ray
flares and those that cause radio emissions have a common origin, which
can give stringent limits on the generation process of radio bursts.
Moreover, we find similar occurrence frequency distributions of energy,
duration, and waiting time for solar radio bursts, SGR 1935+2154 and
repeating FRB 121102, which also support the tight correlation and the
X-ray flares temporally associated with radio bursts. All of these
distributions can be understood by avalanche models of self-organized
criticality systems. The universal correlation and statistical
similarities indicate that the Galactic FRB 200428 and FRBs seen at
cosmological distances can be treated as scaled-up solar radio bursts.</description>
</item>
<item>
<title> The effects of density inhomogeneities on the radio wave emission in electron beam plasmas</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JPlPh..87b9003Y</link>
<description>Type III radio bursts are radio emissions associated with solar flares.
They are considered to be caused by electron beams travelling from the
solar corona to the solar wind. Magnetic reconnection is a possible
accelerator of electron beams in the course of solar flares since it
causes unstable distribution functions and density inhomogeneities
(cavities). The properties of radio emission by electron beams in an
inhomogeneous environment are still poorly understood. We capture the
nonlinear kinetic plasma processes of the generation of beam-related
radio emissions in inhomogeneous plasmas by utilizing fully kinetic
particle-in-cell code numerical simulations. Our model takes into
account initial electron velocity distribution functions (EVDFs) as they
are supposed to be created by magnetic reconnection. We focus our
analysis on low-density regions with strong magnetic fields. The assumed
EVDFs allow two distinct mechanisms of radio wave emissions: plasma
emission due to wave-wave interactions and so-called electron cyclotron
maser emission (ECME) due to direct wave-particle interactions. We
investigate the effects of density inhomogeneities on the conversion of
free energy from the electron beams into the energy of electrostatic and
electromagnetic waves via plasma emission and ECME, as well as the
frequency shift of electron resonances caused by perpendicular gradients
in the beam EVDFs. Our most important finding is that the number of
harmonics of Langmuir waves increases due to the presence of density
inhomogeneities. The additional harmonics of Langmuir waves are
generated by a coalescence of beam-generated Langmuir waves and their
harmonics.</description>
</item>
<item>
<title> Response of Mars's Topside Ionosphere to Changing Solar Activity and Comparisons to Venus</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JGRA..12628913H</link>
<description>Studying how planetary ionospheres respond to changes in solar
irradiance can inform our understanding of how planetary atmospheres
have reacted to our changing Sun over the course of solar system
history. The response of Mars's main ionospheric peak to changing solar
irradiance has been well studied. Less well understood are the altitudes
above the main peak. We use radio occultation observations by Mars
Global Surveyor and ground based solar radio flux measurements to
quantify the response of Mars's electron densities to changing solar
irradiance at these altitudes. This analysis shows that the electron
densities respond modestly at and just above the main peak, with the
response increasing above or below the peak. We use a one dimensional
photochemical equilibrium model to reproduce the observed electron
densities and investigate the influence of minor ions, changing electron
temperatures, and changing neutral densities and composition on the
resultant electron density. We find that the neutral atmosphere is
primarily responsible for the observed behavior. We also make
comparisons to Venus, which shows a more dramatic increase in its
ionospheric response as a function of altitude. We show that while the
ionospheric responses of Mars and Venus as a function of altitude are
markedly different, recasting the analysis in terms of number of scale
heights above the main peak brings the two planets into closer
agreement, especially at the main peak. The agreement is worse at higher
altitudes and this is attributed to Venus's larger proportion of atomic
oxygen.</description>
</item>
<item>
<title> On the Relationship of the O(&lt;SUP&gt;1&lt;/SUP&gt;D) 630.0 nm Dayglow Emission to the F10.7 cm Solar Flux and the Solar Zenith Angle</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JGRA..12628715S</link>
<description>The Wind Imaging Interferometer (WINDII) Empirical Model, which provides
the characteristics of the O(&lt;SUP&gt;1&lt;/SUP&gt;D) 630.0 nm atomic oxygen
dayglow emission from the upper atmosphere has been reviewed and
updated. It now includes the Integrated Emission Rate, the peak Volume
Emission Rate, the Altitude of that peak and the Full Width at Half
Maximum as functions of the F10.7 cm Solar Radio Flux and the solar
zenith angle (SZA). The model employs 98,617 WINDII observations
obtained between the years 1992 and 1996, and the model and observations
of the Integrated Emission Rate agree well with one another within 2
standard deviations of 588.7 Rayleigh (R) (10&lt;SUP&gt;6&lt;/SUP&gt; photons
cm&lt;SUP&gt;2&lt;/SUP&gt; sec&lt;SUP&gt;1&lt;/SUP&gt;). It is also demonstrated that the
impact of latitude, longitude and day of year, independently of their
contribution to the SZA, is very small. The WINDII Empirical Model is
also shown to agree with results from the TRANSCAR photochemical model.
The dayglow is challenging to measure with ground based instruments, as
the solar scattered light from the daytime sky must be accurately
subtracted from the data. Ground based measurements of the integrated
emission rate have been made by others, with good agreement for
observations from Hyderabad during the 2015 summer and winter, but mixed
agreement with measurements made over Boston in 2003. The latter results
are reviewed and assessed.</description>
</item>
<item>
<title> Mingantu Spectral Radioheliograph for Solar and Space Weather Studies</title>
<link>https://ui.adsabs.harvard.edu/abs/2021FrASS...8...20Y</link>
<description>The Chinese Spectral Radioheliograph (CSRH) covering 400 MHz-15 GHz
frequency range was constructed during 2009-2016 in Mingantu Observing
Station, National Astronomical Observatories, Chinese Academy of
Sciences at Zhengxiangbaiqi, Inner Mongolia of China. CSRH is renamed as
{\it M}ingant{\it U} {\it S}p{\it E}ctral {\it R}adioheliograph (MUSER)
after its accomplishment. Currently, MUSER consists of two arrays
spreading over 3 spiral-shaped arms of $\sim$3 km maximum baseline in
both east-west and north-south directions. MUSER array configuration is
optimized to meet the needs of observing the full-disk Sun over
ultrawide wavebands with high temporal, spatial and spectral resolution
and a high dynamic range of images. MUSER-I covers 400 MHz-2.0 GHz with
40 4.5-m-diameter antennas and MUSER-II covers 2-15 GHz with 60
2-m-diameter antennas. MUSER-I can obtain solar full-disk radio images
in 64 frequency channels with 25 ms cadence and 51.6$^{\prime\prime}$ to
10.3$^{\prime\prime}$ spatial resolution corresponding to the frequency
range from 400 MHz to 2 GHz, whereas MUSER-II can obtain full-disk
images in 520 channels with 206.25 ms cadence and 10.3$^{\prime\prime}$
to 1.3$^{\prime\prime}$ resolution from 2 to 15 GHz. Snapshot image
quality with 25 dB dynamic range can be realized. The extension of MUSER
to lower frequency band covering 30 MHz - 400 MHz with an array of 224
logarithm-periodic dipole antennas (LPDAs) has been approved and will be
constructed during the next 4 years. {MUSER} has the following merits as
a solar dedicated instrument: unique high temporal-spatial-spectral
resolutions simultaneously over a wide frequency range; innovative high-
performance ultrawide-band, dual-polarization feeds for wideband signal
collection; advanced high data-rate, large-scale digital correlation
receiver for multiple-frequency and fast snapshot observations; and
applications of new technologies such as using optical fiber to realize
remote antenna and wide-band analog signal transmission. MUSER opens a
new window to measure the solar magnetic fields, trace the dynamic
evolution of energetic electrons in radio frequencies, which will help
us to better understand the origin of solar activities and the basic
drivers of space weather.</description>
</item>
<item>
<title> Radio astronomical tools for the study of solar energetic particles II.Time-extended acceleration at subrelativistic and relativistic energies</title>
<link>https://ui.adsabs.harvard.edu/abs/2021FrASS...7...93K</link>
<description>Solar energetic particle (SEP) events are commonly separated in two
categories: numerous 'impulsive' events of relatively short duration,
and a few 'gradual' events, where SEP-intensities may stay enhanced over
several days at energies up to several tens of MeV. In some gradual
events the SEP spectrum extends to relativistic energies ($&gt; 1$ GeV),
over shorter durations. The two categories are strongly related to an
idea developed in the 1960s based on radio observations: Type III
bursts, which were addressed in a companion chapter, outline impulsive
acceleration of electrons to subrelativistic energies, while the large
and the relativistic SEP events were ascribed to a second acceleration
process. At radio wavelengths, typical counterparts were bursts emitted
by electrons accelerated at coronal shock waves (type II bursts) and by
electron populations in large-scale closed coronal structures (type IV
bursts). Both burst types are related to coronal mass ejections (CMEs).
Type II bursts from metric to kilometric wavelengths tend to accompany
large SEP events, which is widely considered as a confirmation that CME-
driven shocks accelerate the SEPs. But type II bursts, especially those
related to SEP events, are most often accompanied by type IV bursts,
where the electrons are rather accelerated in the wake of the CME.
Individual event studies suggest that although the CME shock is the most
plausible accelerator of SEPs up to some yet unknown limiting energy,
the relativistic SEP events show time structure that rather points to
coronal acceleration related to type IV bursts. This chapter addresses
the question what type II bursts tell us about coronal shock waves and
how type II and type IV radio bursts are related with relativistic
proton signatures as seen by particle detectors on the Earth and by
their gamma-ray emission in the solar atmosphere, focussing on two
relativistic SEP events, on 2005 Jan 20 and 2017 Sep 10. The importance
of radio emissions as a complement to the upcoming SEP observations from
close to the Sun is underlined.</description>
</item>
<item>
<title> Polar and Equatorial Radii Derived from SST and ALMA</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...910...77M</link>
<description>At subterahertz frequenciesi.e., millimeter and submillimeter
wavelengthsthere is a gap in measurements of the solar radius, as well
as other parameters of the solar atmosphere. As the observational
wavelength changes, the radius varies because the altitude of the
dominant electromagnetic radiation is produced at different heights in
the solar atmosphere. Moreover, radius variations throughout long time
series are indicative of changes in the solar atmosphere that may be
related to the solar cycle. Therefore, the solar radius is an important
parameter for the calibration of solar atmospheric models enabling a
better understanding of the atmospheric structure. In this work, we use
data from the Solar Submillimeter-wave Telescope (SST) and the Atacama
Large Millimeter/submillimeter Array (ALMA) at frequencies of 100, 212,
230, and 405 GHz to measure the equatorial and polar radii of the Sun.
The radii measured with extensive data from the SST agree with the
radius-versus-frequency trend present in the literature. The radii
derived from ALMA maps at 230 GHz also agree with the radius-versus-
frequency trend, whereas the 100 GHz radii are slightly above the values
reported by other authors. In addition, we analyze the equatorial and
polar radius behavior over the years by determining the correlation
coefficient between solar activity and subterahertz radius time series
at 212 and 405 GHz (SST). The variations of the SST-derived radii over
13 yr are correlated to the solar activity when considering equatorial
regions of the solar atmosphere and anticorrelated when considering
polar regions. The ALMA-derived radius time series for 100 and 230 GHz
show very similar behaviors with those of SST.</description>
</item>
<item>
<title> Multiwavelength Observations of the Formation and Eruption of a Complex Filament</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...910...40Z</link>
<description>We present an analysis of the formation and eruption of a filament and
fast coronal mass ejection associated with a flare that occurred in
active region 11429 using observations in the ultraviolet, extreme
ultraviolet, X-ray, and radio wavelength bands. Precursor activity began
as an interaction between two filaments, F1 and F2, that are identified
as having twisted magnetic flux ropes (MFRs). Transient brightenings in
all wavelengths are observed as a result of this interaction, likely the
result of magnetic reconnection between the two filaments. This
interaction results in a reconfiguration of the two filaments into a
long overlying filament and a shorter low-lying filament. The upper
filament subsequently undergoes a partial confined eruption. Plasma
flows originating near the east footpoint of F1 lead to an extension of
the upper filament into the filament channel to the west, resulting in a
new active region filament (ARF). This new filament begins a slow rise
and expansion. During its slowly rising phase, the MFR in which the
filament is embedded becomes visible, with both the filament and flux
rope rising and expanding simultaneously. The twist of the magnetic rope
is determined as four turns. The erupting configuration changes from a
twisted arch shape to a reversed  shape within 75 s at the beginning
of the fast-rise phase, representing a transformation from twist to
writhe. The observations provide a clear example of filament formation
via the tether-cutting reconnection of two nearby filaments. A helical
kink instability may be the trigger of the ARF eruption.</description>
</item>
<item>
<title> PIC Simulation of Double Plasma Resonance and Zebra Pattern of Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...909L...5L</link>
<description>The latest study has reported that plasma emission can be generated by
energetic electrons of Dory-Guest-Harris distribution via the electron
cyclotron maser instability (ECMI) in plasmas characterized by a large
ratio of plasma oscillation frequency to electron gyro-frequency
(&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;). In our study, on the basis of the ECMI-
plasma emission mechanism, we examine the double plasma resonance (DPR)
effect and the corresponding plasma emission at both harmonic (H) and
fundamental (F) bands using particle-in-cell simulations with various
&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;. This allows us to directly simulate the
feature of the zebra pattern (ZP) observed in solar radio bursts for the
first time. We find that (1) the simulations reproduce the DPR effect
nicely for the upper hybrid and Z modes, as seen from their variation of
intensity and linear growth rate with &lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;, (2)
the intensity of the H emission is stronger than that of the F emission
by 2 orders of magnitude and varies periodically with increasing
&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt;, while the F emission is too weak to be
significant (therefore, we suggest that it is the H emission accounting
for solar ZPs), (3) the peak-valley contrast of the total intensity of H
is 4, and the peak lies around integer values of
&lt;SUB&gt;pe&lt;/SUB&gt;/&lt;SUB&gt;ce&lt;/SUB&gt; (=10 and 11) for the present parameter
setup. We also evaluate the effect of energy of energetic electrons on
the characteristics of ECMI-excited waves and plasma radiation. The
study provides novel insight on the physical origin of ZPs of solar
radio bursts.</description>
</item>
<item>
<title> Insights on Magnetic Field Dynamics during a Microflare</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...909L...1M</link>
<description>A solar type-I noise storm is produced by accelerated particle beams
generated at active regions undergoing magnetic field restructuring.
Their intensity varies by orders of magnitude within subsecond and sub-
MHz scales. But the morphological evolution of these sources is not
studied at these scales due to the lack of required imaging cadence and
fidelity in meterwave bands. Using data from the Murchison Widefield
Array, this work explores the coevolution of size, sky-orientation, and
intensity of a noise storm source associated with a weak microflare.
This work presents the discovery of two correlated modes of evolution in
the source parameters: a sausage like "S" mode where the source
intensity and size show an anticorrelated evolution; and a torsional
like "T" mode where the source size and sky-orientation show a
correlated evolution. A flare mediated mode conversion is observed from
"T" to "S" for the first time in these sources. These results support
the idea of build up of magnetic stress energy in braided active region
loops, which later become unstable causing flares and particle
acceleration until they relax to a minimally braided state. The
discovered mode conversion can be a future diagnostic for such events.</description>
</item>
<item>
<title> The Source Size, Duration, and Position</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...909..195Z</link>
<description>The observed features of the radio source indicate that the waves of
solar radio bursts are convoluted with complex propagation effects. In
this work, we perform ray-tracing simulations on radio wave transport in
the corona and interplanetary region with anisotropic electron density
fluctuations. For the first time, the variation of the apparent source
size, burst duration, and source position for the fundamental emission
and harmonic emission at the frequency of 35 MHz are simulated as a
function of the anisotropic parameter  and the angular scattering rate
coefficient  = &lt;SUP&gt;2&lt;/SUP&gt;/h&lt;SUB&gt;0&lt;/SUB&gt;, where &lt;SUP&gt;2&lt;/SUP&gt; =
n&lt;SUP&gt;2&lt;/SUP&gt;/n&lt;SUP&gt;2&lt;/SUP&gt; is the density fluctuation level and
h&lt;SUB&gt;0&lt;/SUB&gt; is its correlation length near the wave excitation site.
It is found that isotropic fluctuations produce a much larger decay time
than a highly anisotropic fluctuation for fundamental emission. By
comparing the observed duration and source size with the simulation
results in the parameter space, we can estimate the scattering
coefficient and the anisotropic parameter  = 8.9  10&lt;SUP&gt;-5&lt;/SUP&gt;
km&lt;SUP&gt;-1&lt;/SUP&gt; and  = 0.719 with a point pulse source assumption.
Position offsets due to wave scattering and refraction can produce the
co-spatial of the fundamental and harmonic waves in the observation of
some type III radio bursts. The visual speed due to the wave propagation
effect can reach 1.5c for  = 2.4  10&lt;SUP&gt;-4&lt;/SUP&gt; km&lt;SUP&gt;-1&lt;/SUP&gt; and
 = 0.2 for the fundamental emission in the sky plane, accompanied with
large expansion rate of the source size. The direction of the visual
speed is mostly identical to the direction of the offset, thus, for the
observation aimed at obtaining the source position, the source centroid
at the starting time is closer to the wave excitation site.</description>
</item>
<item>
<title> Harmonic Electron Cyclotron Maser Emission Excited by Energetic Electrons Traveling inside a Coronal Loop</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...909....3Y</link>
<description>A complete understanding of solar radio bursts requires developing
numerical techniques that can connect large-scale activities with
kinetic plasma processes. As a starting point, this study presents a
numerical scheme combining three different techniques: (1) extrapolation
of the magnetic field overlying a specific active region in order to
derive the background field, (2) guiding-center simulation of the
dynamics of millions of particles within a selected loop to reveal the
integral velocity distribution function (VDF) around certain sections of
the loop, and (3) particle-in-cell simulation of kinetic instabilities
driven by energetic electrons initiated by the obtained distributions.
Scattering effects at various levels (weak, moderate, and strong) due to
wave turbulence-particle interaction are considered using prescribed
timescales of scattering. It was found that the obtained VDFs contain
strip-like and loss-cone features with positive gradient, and both
features are capable of driving electron cyclotron maser emission, which
is a viable radiation mechanism for some solar radio bursts, in
particular, solar radio spikes. The strip-like feature is important in
driving the harmonic X mode, while the loss-cone feature can be
important in driving the fundamental X mode. In the weak-scattering
case, the rate of energy conversion from energetic electrons to X2 can
reach up to $\sim 2.9\times {10}^{-3}\,{E}_{{k}_{0}}$ , where
${E}_{{k}_{0}}$ is the initial kinetic energy of energetic electrons.
The study demonstrates a novel way of exciting the X2 mode in the corona
during solar flares and provides new sight into how escaping radiation
can be generated within a coronal loop.</description>
</item>
<item>
<title> LOFAR Observations of a Jet-driven Piston Shock in the Low Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...909....2M</link>
<description>The Sun produces highly dynamic and eruptive events that can drive
shocks through the corona. These shocks can accelerate electrons, which
result in plasma emission in the form of a type II radio burst. Despite
the large number of type II radio burst observations, the precise origin
of coronal shocks is still subject to investigation. Here, we present a
well-observed solar eruptive event that occurred on 2015 October 16,
focusing on a jet observed in the extreme ultraviolet by the Atmospheric
Imaging Assembly (SDO/AIA), a streamer observed in white light by the
Large Angle and Spectrometric Coronagraph (SOHO/LASCO), and a metric
type II radio burst observed by the LOw Frequency Array (LOFAR). LOFAR
interferometrically imaged the fundamental and harmonic sources of a
type II radio burst and revealed that the sources did not appear to be
cospatial, as would be expected from the plasma emission mechanism. We
correct for the separation between the fundamental and harmonic using a
model that accounts for scattering of radio waves by electron density
fluctuations in a turbulent plasma. This allows us to show the type II
radio sources were located 0.5R&lt;SUB&gt;&lt;/SUB&gt; above the jet and
propagated at a speed of 1000 km s&lt;SUP&gt;-1&lt;/SUP&gt;, which was
significantly faster than the jet speed of 200 km s&lt;SUP&gt;-1&lt;/SUP&gt;. This
suggests that the type II burst was generated by a piston shock driven
by the jet in the low corona.</description>
</item>
<item>
<title> Multi-wavelength analysis of CME-driven shock and Type II solar radio burst band-splitting</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ap&amp;SS.366...31L</link>
<description>It is now well established that Coronal Mass Ejections (CMEs) may
produce shocks in near Sun and interplanetary medium. A Type-II radio
burst is characterized by shock and associated emission with very slow
frequency drift rate (0.1 MHz/sec). A CME driven shock and their
velocity, acceleration/deceleration signature can be observed by a Type-
II solar radio burst which drifts with the shock speed and is split in
bands of plasma radio emission. These emissions can be seen in radio
spectrographs as split bands both in fundamental and harmonic
frequencies close to a ratio of 1:2. In this paper, we present an
analysis of a CME associated with a band splitting Type-II radio burst
observed using multi-instruments in multi-wavelengths. We observed the
CME event that occurred in 02 May 2013 (05:24 UT) and is associated with
an M1.1 class solar flare from the active region NOAA 11731 located at
N10W23 on the solar disk. We use the widely accepted Newkirk coronal
density model to estimate the height in the solar atmosphere to compare
our results. We conclude that the speed of CME is high enough to produce
a Type-II solar radio burst. The analysis of this paper also involved an
estimation of the coronal ambient magnetic field and its comparison with
the empirical active region magnetic field model (Dulk and McLean in
Sol. Phys. 57:279, 1978). This shows the good results. Observations
provide sufficient evidence that the unusual patch signature in Type-II
solar radio burst is due to the CMECME interaction.</description>
</item>
<item>
<title> Short-term periodicities in the downward longwave radiation and their associations with cosmic ray and solar interplanetary data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..67.1672M</link>
<description>In this study downward longwave (LW) atmospheric radiation data for the
period of 2014-2020 were used to search for short-term periodicities
using fast Fourier transform (FFT). Several local peaks in the power
spectrum density were found and established. The time series exhibits a
series of significant peaks (exceeding the 95% confidence limit), such
as at 273 days, 227 days, 200 days, 178 days, 157 days, 110 days, 120
days, 87 days, 73 days, 53-56 days, 35-30 days, 25-27 days, 21 days, 13
days, and 9-10 days. &lt;P /&gt;Moreover, cosmic ray data from KACST muon
detector and the Oulu neutron monitor, as well as the data for the solar
radio flux at 10.7 cm (F10.7 cm), Dst index, and solar wind speed for
the same period as the LW data, were used to look for common cyclic
variations and periodicities matching those found in the LW radiation.
This was done to investigate the possible effect of the solar activity
parameters on LW radiation. Several common periodicities were observed
in the spectra of all the variables considered, such as 227 days,
154-157 days, 25-27 days, and 21 days. Some of the periodicities found
in the LW radiation spectrum can be attributed to the modulation of the
cosmic ray intensity by solar activity. Others are attributed to the
disturbances in the interplanetary magnetic field. Based on the spectral
results, we suggest that the solar signals may directly or indirectly
affect the variations of the downward longwave radiation, which in turn
may affect climate change.</description>
</item>
<item>
<title> Moving solar radio bursts and their association with coronal mass ejections</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...647L..12M</link>
<description>Context. Solar eruptions, such as coronal mass ejections (CMEs), are
often accompanied by accelerated electrons that can in turn emit
radiation at radio wavelengths. This radiation is observed as solar
radio bursts. The main types of bursts associated with CMEs are type II
and type IV bursts that can sometimes show movement in the direction of
the CME expansion, either radially or laterally. However, the
propagation of radio bursts with respect to CMEs has only been studied
for individual events. &lt;BR /&gt; Aims: Here, we perform a statistical study
of 64 moving bursts with the aim to determine how often CMEs are
accompanied by moving radio bursts. This is done in order to ascertain
the usefulness of using radio images in estimating the early CME
expansion. &lt;BR /&gt; Methods: Using radio imaging from the Nanay
Radioheliograph (NRH), we constructed a list of moving radio bursts,
defined as bursts that move across the plane of sky at a single
frequency. We define their association with CMEs and the properties of
associated CMEs using white-light coronagraph observations. We also
determine their connection to classical type II and type IV radio burst
categorisation. &lt;BR /&gt; Results: We find that just over a quarter of type
II and half of type IV bursts that occurred during the NRH observing
windows in Solar Cycle 24 are accompanied by moving radio emission. All
but one of the moving radio bursts are associated with white-light CMEs
and the majority of moving bursts (90%) are associated with wide CMEs (&gt;
60 in width). In particular, all but one of the moving bursts
corresponding to type IIs are associated with wide CMEs; however, and
unexpectedly, the majority of type II moving bursts are associated with
slow white-light CMEs (&lt; 500 km s&lt;SUP&gt;1&lt;/SUP&gt;). On the other hand, the
majority of moving type IV bursts are associated with fast CMEs (&gt; 500
km s&lt;SUP&gt;1&lt;/SUP&gt;). &lt;BR /&gt; Conclusions: The observations presented here
show that moving radio sources are almost exclusively associated with
CMEs. The majority of events are also associated with wide CMEs,
indicating that strong lateral expansion during the early stages of the
eruption may play a key role in the occurrence of the radio emission
observed.</description>
</item>
<item>
<title> Spectroscopic observations of a flare-related coronal jet</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...647A.113Z</link>
<description>Context. Coronal jets are ubiquitous in active regions and coronal
holes. &lt;BR /&gt; Aims: In this paper, we study a coronal jet related to a
C3.4 circular-ribbon flare in the active region 12434 on 2015 October
16. &lt;BR /&gt; Methods: The flare and jet were observed in ultraviolet and
extreme ultraviolet wavelengths by the Atmospheric Imaging Assembly on
board the Solar Dynamics Observatory (SDO). The line-of-sight
magnetograms of the photosphere were observed by the Helioseismic and
Magnetic Imager on board SDO. The whole event was covered by the
Interface Region Imaging Spectrograph during its imaging and
spectroscopic observations. Soft X-ray fluxes of the flare were recorded
by the GOES spacecraft. Hard X-ray (HXR) fluxes at 450 keV were
obtained from observations of RHESSI and Fermi. Radio dynamic spectra of
the flare were recorded by the ground-based stations belonging to the
e-Callisto network. &lt;BR /&gt; Results: Two minifilaments were located under
a 3D fan-spine structure before flare. The flare was generated by the
eruption of one filament. The kinetic evolution of the jet was divided
into two phases: a slow rise phase at a speed of 131 km s&lt;SUP&gt;1&lt;/SUP&gt;
and a fast rise phase at a speed of 363 km s&lt;SUP&gt;1&lt;/SUP&gt; in the plane-
of-sky. The slow rise phase may correspond to the impulsive reconnection
at the breakout current sheet. The fast rise phase may correspond to
magnetic reconnection at the flare current sheet. The transition between
the two phases occurred at 09:00:40 UT. The blueshifted Doppler
velocities of the jet in the Si IV 1402.80  line range from 34 to 120
km s&lt;SUP&gt;1&lt;/SUP&gt;. The accelerated high-energy electrons are composed of
three groups. Those propagating upward along the open field generate
type III radio bursts, while those propagating downward produce HXR
emissions and drive chromospheric condensation observed in the Si IV
line. The electrons trapped in the rising filament generate a microwave
burst lasting for 40 s. Bidirectional outflows at the base of jet are
manifested by significant line broadenings of the Si IV line. The
blueshifted Doppler velocities of outflows range from 13 to 101 km
s&lt;SUP&gt;1&lt;/SUP&gt;. The redshifted Doppler velocities of outflows range from
17 to 170 km s&lt;SUP&gt;1&lt;/SUP&gt;. &lt;BR /&gt; Conclusions: Our multiwavelength
observations of the flare-related jet are in favor of the breakout jet
model and are important for understanding the acceleration and transport
of nonthermal electrons. &lt;P /&gt;Movies are available at &lt;A href="https://w
ww.aanda.org/10.1051/0004-6361/202038924/olm"&gt;https://www.aanda.org&lt;/A&gt;</description>
</item>
<item>
<title> 3D Quasilinear Effects</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...42M</link>
<description>A conventional model for the generation of Langmuir waves in Type-III
radio bursts is based on a one-dimensional (1D) version of the
quasilinear equations. In this model a wave with phase velocity
v&lt;SUB&gt;&lt;/SUB&gt; resonates with an electron with velocity v =v&lt;SUB&gt;&lt;/SUB&gt;,
causing the waves to grow at a rate d F (v )/d v &gt;0 , where F (v ) is
the 1D-distribution function. The backreaction on the electrons drives
the electrons towards a plateau distribution: d F (v )/d v 0 . In the
3D-generalization, none of these features apply: waves with phase speed
v&lt;SUB&gt;&lt;/SUB&gt; can resonate with electrons with speed v &lt;v&lt;SUB&gt;&lt;/SUB&gt;,
depending on the angle between the wave normal and the electron
velocity, wave growth occurs only if the distribution function is both
an increasing function of v and also has an anisotropic pitch-angle
distribution, and the backreaction involves diffusion in both speed v
and in pitch-angle  . In this article we discuss implications of the
generalization from 1D to 3D on models for Type-III bursts. An effect
that is absent in 1D, but may be important in 3D, is scattering of
Langmuir waves by turbulence in the ambient plasma. Pitch-angle
scattering by the scattered Langmuir waves may play an important role in
the evolution of the Type-III beam.</description>
</item>
<item>
<title> An Observational Revisit of Stationary Type IV Solar Radio Bursts</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...38L</link>
<description>Stationary type IV solar radio bursts (IVSs) are broadband continuum
emission observed at decimetric-decametric wavelength without apparent
source motions. They are closely associated with solar flares and/or
coronal mass ejections. Earlier studies on IVSs suffered from limited
number of events, frequency coverage and available channels, and spatial
resolution. Here we present an analysis on 34 IVSs using two-dimensional
imaging data provided by Nanay Radioheliograh (NRH) at 10 frequencies
from 150 to 445 MHz. The events are recorded from 2010 to 2014. We focus
on general properties including the spatial dispersion of sources with
frequency, brightness temperature (T&lt;SUB&gt;B&lt;/SUB&gt;) and corresponding
spectra, and polarization. Main findings are: (i) In the majority of
events (23/34) regular and systematic source dispersion with frequency
can be clearly recognized. (ii) In most (31/34) events the maximum
brightness temperature (T&lt;SUB&gt;BM&lt;/SUB&gt;&lt;SUP&gt;E&lt;/SUP&gt;) exceeds
10&lt;SUP&gt;8&lt;/SUP&gt;K, and exceeds 10&lt;SUP&gt;9&lt;/SUP&gt;K in 23 events. The histogram
distribution of T&lt;SUB&gt;BM&lt;/SUB&gt;&lt;SUP&gt;f&lt;/SUP&gt;, i.e. the maximum brightness
temperature of a source at certain frequency (f ) of a specific event
(referred to as event-f source, there are 247 such sources in total)
exhibits a clear declining trend with increasing frequencies. The
dominant type of T&lt;SUB&gt;B&lt;/SUB&gt; spectra is power-law like with a negative
index. (iii) In most events (30/34) the sense of polarization remains
unchanged and the number of events with right and left-handed
polarization are comparable. In 57% of all 247 event-f sources the level
of polarization does not change considerably, in about 39% sources the
level of polarization exhibits significant variation yet with a fixed
sense, and in only 4% the sense of polarization changes. These results
provide strong constraints on radiation mechanism of IVSs.</description>
</item>
<item>
<title> Intense L-Band Solar Radio Bursts Detection Based on GNSS Carrier-To-Noise Ratio Decrease over Multi-Satellite and Multi-Station</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Senso..21.1405Y</link>
<description>Not Available</description>
</item>
<item>
<title> origins and radio-wave propagation effects</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PhDT.........1C</link>
<description>Solar eruptive events are associated with radio emissions that appear as
impulsive increases in intensity, known as solar radio bursts.
Turbulence in the solar corona impacts the propagation of radio waves,
obscuring the intrinsic emission properties. Here, anisotropic
scattering on small-scale density fluctuations is investigated using
novel 3D radio-wave propagation simulations. Several observed radio
properties are simultaneously reproduced for the first time, verifying
the necessity to consider anisotropic scattering. The sub-second
evolution of fine radio burst properties at a single frequency is also
investigated, enabled by conducting observations that utilise the
unprecedented imaging capabilities of the LOw-Frequency ARray (LOFAR).
The fundamental and harmonic sources of a Type IIIb burst are
quantitatively compared, demonstrating that harmonic emissions arise
from an intrinsic source with a finite size and finite emission
duration. Drift-pair burst observations are successfully described by
the radio echo hypothesis. It is shown that the radio echo, which
produces the second Drift-pair component, is detected only when the
anisotropy is strong. A dependence of the observed properties on the
source's intrinsic location and on the assumed emission-to-plasma
frequency ratio is inferred. Moreover, the subbands of a split-band Type
II burst are simultaneously imaged for the first time. Despite the large
separations observed between subband sources, it is shown that once
scattering is quantitatively accounted for, the sources become co-
spatial. Corrections on the observed source locations also allude to
lower coronal densities. Additionally, the first observation of a Type
II burst that transitions between a stationary and drifting statetermed
as a transitioning Type II burstis reported. The radio emissions are
related to a jet eruption that drives a streamer-puff CME. Overall,
state-of-the-art simulations and radio observations are combined and
compared. The importance of accounting for radio-wave propagation
effectsprimarily anisotropic scatteringand the consequence of
neglecting to do so on any subsequent interpretations is illustrated.</description>
</item>
<item>
<title> The Delayed Ionospheric Response to the 27 day Solar Rotation Period Analyzed With GOLD and IGS TEC Data</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JGRA..12628861S</link>
<description>The delayed ionospheric response is analyzed for two well defined 27 day
solar rotation periods in the year 2019 with solar radio flux index
F10.7 and Global scale Observations of the Limb and Disk (GOLD) data,
like solar extreme ultraviolet (EUV) flux proxy, O/N&lt;SUB&gt;2&lt;/SUB&gt; column
density ratio and peak electron density, as well as International Global
Navigation Satellite System Service rapid high rate total electron
content (TEC) map data. Although the correlation between GOLD solar EUV
flux proxy and TEC is similar to the correlation between F10.7 and TEC,
it is shown that the estimated delays based on GOLD data are in much
better agreement with recent studies using EUV measurements compared to
the delays based on F10.7 data. The GOLD peak electron density
correlates well with TEC and allows insight to a local time interval
when the ionosphere is not controlled by solar activity changes (17:00
LT to 21:00 LT). The present study investigates the impact of the solar
activity (F10.7, GOLD EUV flux proxy) and O/N&lt;SUB&gt;2&lt;/SUB&gt; column density
ratio on the ionospheric delay for two representative solar rotation
periods. The capabilities of GOLD data for future research on the
ionospheric response to the 27 day solar rotation period are
demonstrated and discussed. These results are crucial information for
precise ionospheric models and forecasts.</description>
</item>
<item>
<title> The Impact of Solar Flux Proxies and Indices</title>
<link>https://ui.adsabs.harvard.edu/abs/2021JGRA..12628466G</link>
<description>We present a new high resolution empirical model for the ionospheric
total electron content (TEC). TEC data are obtained from the global
navigation satellite system (GNSS) receivers with a 1  1 spatial
resolution and 5 min temporal resolution. The linear regression model is
developed at 45N, 0E for the years 2000-2019 with 30 min temporal
resolution, unprecedented for typical empirical ionospheric models. The
model describes dependency of TEC on solar flux, season, geomagnetic
activity, and local time. Parameters describing solar and geomagnetic
activity are evaluated. In particular, several options for solar flux
input to the model are compared, including the 10.7 cm solar radio flux
(F&lt;SUB&gt;10.7&lt;/SUB&gt;), the Mg II core to wing ratio, and formulations of
the solar extreme ultraviolet flux (EUV). Ultimately, the extreme
ultraviolet flux presented by the Flare Irradiance Spectral Model,
integrated from 0.05 to 105.05 nm, best represents the solar flux input
to the model. TEC time delays to this solar parameter on the order of
several days as well as seasonal modulation of the solar flux terms are
included. The Ap&lt;SUB&gt;3&lt;/SUB&gt; index and its history are used to reflect
the influence of geomagnetic activity. The root mean squared error of
the model (relative to the mean TEC observed in the 30 min window) is
1.9539 TECu. A validation of this model for the first 3 months of 2020
shows excellent agreement with data. The new model shows significant
improvement over the International Reference Ionosphere 2016 (IRI 2016)
when the two are compared during 2008 and 2012.</description>
</item>
<item>
<title> Radio astronomical tools for the study of solar energetic particles I. Correlations and diagnostics of impulsive acceleration and particle propagation</title>
<link>https://ui.adsabs.harvard.edu/abs/2021FrASS...7..105K</link>
<description>Solar energetic particles (SEPs) are sporadically ejected from the Sun
during flares and coronal mass ejections. They are of major
astrophysical interest, because the proximity of the Sun allows for
detailed multi-messenger studies. They affect space weather due to
interactions with electronics, with the Earth's atmosphere, and with
humans if they leave the protective shield of the magnetosphere of the
Earth. Since early studies in the 1950s, starting with particle
detectors on the ground, SEP events have been related to radio
bursts.Two subjects are addressed in this chapter: attempts to establish
quantitative correlations between SEPs and microwave bursts produced by
gyro synchrotron radiation of mildly relativistic electrons, and the
information derived from type III radio bursts on impulsive processes of
particle acceleration and the coronal and interplanetary propagation.
Type III radio bursts produced by electron beams on open magnetic field
lines have a wide range of applications, including the identification of
acceleration regions, the identification of confined particle
acceleration with coronal signatures, but no SEPs, and the paths that
the electrons, and energetic charged particles in general, take to
travel from the low corona to the Heliosphere in case they escape.
Simple scenarios of coronal particle acceleration are confirmed in
relatively simple and short events. But the comparison with particle
transport models shows that longer and delayed acceleration episodes
exist especially in large SEP events. They will be discussed in a
companion chapter.</description>
</item>
<item>
<title> First Results from Joint Microwave and Hard X-Ray Imaging Spectroscopy</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...908L..55C</link>
<description>Nonthermal sources located above bright flare arcades, referred to as
the "above-the-loop-top" sources, have been often suggested as the
primary electron acceleration site in major solar flares. The X8.2 limb
flare on 2017 September 10 features such an above-the-loop-top source,
which was observed in both microwaves and hard X-rays (HXRs) by the
Expanded Owens Valley Solar Array and the Reuven Ramaty High Energy
Solar Spectroscopic Imager, respectively. By combining the microwave and
HXR imaging spectroscopy observations with multifilter extreme
ultraviolet and soft X-ray imaging data, we derive the coronal magnetic
field and energetic electron distribution of the source over a broad
energy range from &lt;10 keV up to MeV during the early impulsive phase of
the flare. The source has a strong magnetic field of over 800 G. The
best-fit electron distribution consists of a thermal "core" from 25 MK
plasma. A nonthermal power-law "tail" joins the thermal core at 16 keV
with a spectral index of 3.6, which breaks down at above 160 keV to
&gt;6.0. Temporally resolved analysis suggests that the electron
distribution above the break energy rapidly hardens with the spectral
index decreasing from &gt;20 to 6.0 within 20 s, or less than 10 Alfvn
crossing times in the source. These results provide strong support for
the above-the-loop-top source as the primary site where an ongoing bulk
acceleration of energetic electrons is taking place very early in the
flare energy release.</description>
</item>
<item>
<title> Diagnosing a Solar Flaring Core with Bidirectional Quasi-periodic Fast Propagating Magnetoacoustic Waves</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...908L..37M</link>
<description>Quasi-periodic fast propagating (QFP) waves are often excited by solar
flares, and could be trapped in the coronal structure with low Alfvn
speed, so they could be used as a tool for diagnosing both the flaring
core and magnetic waveguide. As the periodicity of a QFP wave could
originate from a periodic source or be dispersively waveguided, it is a
key parameter for diagnosing the flaring core and waveguide. In this
paper, we study two QFP waves excited by a Geostationary Operational
Environmental Satellite-class C1.3 solar flare occurring at active
region NOAA 12734 on 2019 March 8. Two QFP waves were guided by two
oppositely oriented coronal funnels. The periods of two QFP waves were
identical and were roughly equal to the period of the oscillatory signal
in the X-ray and 17 GHz radio emission released by the flaring core. It
is very likely that the two QFP waves could be periodically excited by
the flaring core. Many features of this QFP wave event are consistent
with the magnetic tuning fork model. We also investigated the
seismological application with QFP waves, and found that the magnetic
field inferred with magnetohydrodynamic seismology was consistent with
that obtained in the magnetic extrapolation model. Our study suggests
that the QFP wave is a good tool for diagnosing both the flaring core
and the magnetic waveguide.</description>
</item>
<item>
<title> Harmonic Radio Emission in Randomly Inhomogeneous Plasma</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...908..126T</link>
<description>In the present paper, we describe a theoretical model of the generation
of harmonic emissions of type III solar radio bursts. The goal of our
study is to fully take into account the most efficient physical
processes involved in the generation of harmonic electromagnetic
emission via nonlinear coupling of Langmuir waves in randomly
inhomogeneous plasma of solar wind ( $l+{l}^{{\prime} }\to t$ ). We
revisit the conventional mechanism of coalescence of primarily generated
and back-scattered Langmuir waves in quasihomogeneous plasma.
Additionally, we propose and investigate another mechanism that
generates harmonic emission only in a strongly inhomogeneous plasma: the
nonlinear coupling of incident and reflected Langmuir waves inside
localized regions with enhanced plasma density (clumps), in the close
vicinity of the reflection point. Both mechanisms imply the presence of
strong density fluctuations in plasma. We use the results of a
probabilistic model of beam-plasma interaction and evaluate the
efficiency of energy transfer from Langmuir waves to harmonic emission.
We infer that harmonic emissions from a quasihomogeneous plasma are
significantly more intense than found in previous studies. The
efficiency of Langmuir wave conversion into electromagnetic harmonic
emission is expected to be higher at large heliospheric distances for
the mechanism operating in quasihomogeneous plasma and at small
heliocentric distances for the one operating in inhomogeneous plasma.
The evaluation of emission intensity in quasihomogeneous plasma may also
be applied for type II solar radio bursts. The radiation pattern in both
cases is quadrupolar, and we show that emission from density clumps may
efficiently contribute to the visibility of harmonic radio emission.</description>
</item>
<item>
<title> A statistical study of solar radio Type III bursts and space weather implication</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..67.1425N</link>
<description>Solar radio bursts (SRBs) are the signatures of various phenomenon that
happen in the solar corona and interplanetary medium (IPM). In this
article, we have studied occurrence of Type III bursts and their
association with the Sunspot number. This study confirms that occurrence
of Type III bursts correlate well with Sunspot number. Further, using
the data obtained using e-CALLISTO network, we have investigated drift
rates of isolated Type III bursts and duration of the group of Type III
bursts. Since Type II, Type III and Type IV bursts are signatures of
solar flares and/or CMEs, we can use the radio observations to predict
space weather hazards. In this article, we have discussed two events
that have caused near Earth radio blackouts. Since e-CALLISTO comprises
more than 152 stations at different longitudes, we can use it to monitor
the radio emissions from the solar corona 24 h a day. Such observations
play a crucial role in monitoring and predicting space weather hazards
within few minutes to hours of time.</description>
</item>
<item>
<title> Spatial quasi-periodic variations of the plasma density and magnetic field in zebra radio sources</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...646A.179K</link>
<description>Context. Radio bursts and their fine structures are an integral part of
solar flares. Fine structures in particular are used for diagnostics of
solar flare processes. The so-called zebras belong to the most important
of such fine structures. &lt;BR /&gt; Aims: We analyze seven zebra events in
order to search for spatial variations in the plasma density and
magnetic field in zebra-stripe sources. &lt;BR /&gt; Methods: We used an
improved method for estimating the gyroharmonic numbers of zebra-stripe
frequencies. We compared observed zebra-stripe frequencies with those
calculated in the zebra model. The differences in these frequencies vary
and thus show spatial variations in the plasma density and magnetic
field. &lt;BR /&gt; Results: In six out of seven analyzed zebras, we found a
rather high correlation coefficient (about 0.7 and higher) between
spatial variations in the density and magnetic field and a strictly
periodic function. These density and magnetic field variations are
explained by the torsional or sausage magnetoacoustic waves in the loop
in which zebra-stripe sources are located. We present the wavelengths of
these waves in dependence on the zebra frequency and estimate their
periods.</description>
</item>
<item>
<title> Properties of High-Frequency Type II Radio Bursts and Their Relation to the Associated Coronal Mass Ejections</title>
<link>https://ui.adsabs.harvard.edu/abs/2021SoPh..296...27U</link>
<description>Solar radio bursts are often early indicators of space weather events
such as coronal mass ejections (CMEs). In this study, we determined the
properties of a sample of 40 high-starting-frequency ( 150 MHz) type II
radio bursts and the characteristics of the associated CMEs such as
width, location and speed during 2010-2016. The high starting frequency
implies shock formation closer to the solar surface, which has important
ramifications for the analysis of particle acceleration near the Sun. We
found the CME heliocentric distances at the onset time of metric type II
bursts range from 1.16 to 1.90 solar radii (Rs). The study was also
extended to 128 metric type II bursts to include lower-starting-
frequency events for further analysis. The projected CME heights range
from 1.15 to 2.85 Rs. The lower starting frequency correspond to shocks
forming at larger heights. A weak correlation was found between the
type-II starting frequency and CME heights, which is consistent with the
density decline in the inner corona. The analysis confirmed a good
correlation between the drift rate and the starting frequency of type II
bursts (correlation coefficient  0.8). Taking into account the radial
variation of CMEs speeds from the inner corona to the interplanetary
medium, we observed the deviations from the universal drift-rate
spectrum of type II bursts and confirmed the previous results relating
type II bursts to CMEs.</description>
</item>
<item>
<title> A New Universality Class Pertaining to Quantum Critical Systems</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PhDT........16F</link>
<description>Waves and oscillations are important solar phenomena not only because
they can propagate and dissipate energy in the chromosphere, but also
because they carry information about the structure of the atmosphere in
which they propagate. Among these phenomena, the one of the most
interesting ones occurs in the sunspot umbra. In this area, continuously
propagating magnetohydrodynamic (MHD) waves generated from below the
photosphere create the famous 3-minute sunspot umbral oscillations that
affect the line profile of spectral lines due to temperature, density,
and velocity changes of the plasma in the region. In the past decades,
numerous observations and models have been carried out about the nature
of the 3-minute oscillation and its relation with the coronal heating
problem, but the lack of direct observations of the temperature
variation in the chromosphere has made it hard to answer these
questions.The need for a better understanding of the fine structure of
the 3-minute oscillation and its time evolution in sunspots has
intensified with the development of better observing tools. Among modern
observatories, the Atacama Large Millimeter/submillimeter Array (ALMA)
opens up a new era of solar radio observation due to its high spatial
and temporal resolution and image quality. When combined with other
cutting-edge instruments, such as the Goode Solar Telescope (GST) at the
Big Bear Solar Observatory (BBSO), the Atmospheric Imaging Assembly
(AIA) on board the Solar Dynamics Observatory, and Interface Region
Imaging Spectrograph (IRIS), ALMA can provide unique electron
temperature diagnostics that clarify the behavior of the solar
chromosphere's response to propagating waves.In this dissertation, a
study is carried out about sunspot oscillations and wave propagation in
NOAA active region 12470 using an approximately 1 hr long dataset
acquired on 2015 December 17 by the instruments listed above. The
discovery of 3-minute sunspot oscillations seen in the mm-wave band is
reported for the first time. The 2 s cadence of ALMA images makes it
possible to well resolve the typical 3-minute period sunspot oscillation
in the chromosphere. Fourier analysis is applied to the ALMA band 3 and
GST H data sets to obtain the power spectra as well as phase
information of the oscillations. The properties of the wave propagation
are analyzed by combining multiple wavelengths that probe physical
parameters of the solar atmosphere at different heights.The
chromospheric radiation is synthesized in 1-D using a radiation transfer
code which uses the Solar Irradiance Physical Modeling (SRPM) as an
input. A good correlation of the phase relationship between the observed
and modeled oscillations of H and temperature fluctuations has been
found and it is consistent with the result from a possible physical
model for impulse-driven acoustic waves propagating in the
gravitationally stratified medium. An asymmetry in the time profile of
the temperature fluctuations discovered in the ALMA data is found to
require a nonlinear wave solution, which is applied to several
atmospheric models in an attempt to match the asymmetry and the absolute
brightness temperature of the simulations to the observations. The
asymmetry is successfully reproduced using the nonlinear wave scenario,
although the absolute brightness of the simulated atmosphere remains
lower than observed. These results demonstrate the capability of ALMA mm
observations to provide new insight into what is needed for improving
such atmospheric models in the future.</description>
</item>
<item>
<title> Radio Diagnostics of Particles and Plasma in the Solar Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PhDT........15C</link>
<description>Radio diagnostics, in addition to their capabilities in exploring
intense, impulsive bursts, also provide a high sensitivity to much
weaker events, which may not show any substantial signature in other
wavelengths. &lt;P /&gt;The initial case study examines a complex event
consisting of multiple radio sources/bursts associated with a fast
coronal mass ejection (CME) and an M 2.1 class solar flare
(SOL2015-09-20). 'First-light' data from the Owens Valley Radio
Observatory-Long Wavelength Array is put in context with observations
from Large Angle and Spectrometric Coronagraph onboard the Solar and
Heliospheric Observatory, along with the WAVES radio spectrograph
onboard WIND, the Expanded Owens Valley Solar Array, and the Air Force
Radio Solar Telescope Network. One burst source exhibiting an outward
motion is focused upon indicating movement associated with the core of
the CME and is classified as type IVm burst. The source height,
smoothness of the emission in frequency and time, along with a lower
density in the region, indicate the likelihood of gyrosynchrotron as the
underlying mechanism over plasma emission. Spectral fitting techniques
are used to estimate the physical conditions during the outward movement
of the source. &lt;P /&gt;The second study investigates whether energy bursts
from small breaks in stressed magnetic fields (nanoflares) can
accelerate particles like full-sized flares, and if so, how efficiently?
Since nanoflares may produce numerous 'mildly energetic' particles, at
those energies, the emission in X-ray will be dominated by the thermal
component. Type III radio bursts generated by propagating energetic
electrons are best suited for the purpose. A model is created to
simulate type III emission that may be produced by thousands of
nanoflares occurring per second and the novel time-lag technique used to
detect the motion of particles. The technique indeed detects the
signature of type IIIs despite the numerous overlapping bursts and added
noise that is expected in a radio instrument. Based on the findings of
the model and associated testing, data from the Very Large Array, Low
Frequency Array, and Long Wavelength Array are currently being looked at
for signatures of such bursts in the corona. A similar test is performed
on data from the FIELDS instrument onboard Parker Solar Probe to look
for signatures of particle acceleration in the solar wind from small-
scale reconnection events.</description>
</item>
<item>
<title> POEM AHAA  PODHOA XAPAKTEPCTK EPBX VA 25-DO KA COHEHO AKTBHOCT, OPEEX COCTOH CCTEM OCVEPPOEM AHAA  PODHOA XAPAKTEPCTK EPBX VA 25-DO KA COHEHO AKTBHOCT, OPEEX COCTOH CCTEM OCVEPProblems of Analysis and Forecast of Characteristics of the First Phase 25 Cycle of Solar Activity, Determining States of Biosphere Systems</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PTSUS...4...45V</link>
<description>The paper considers the results of the analysis and prediction of the
dynamics of so-lar activity from the series of the solar radio flux
density at a frequency of 2.8 GHz and the relative Wolf numbers,
proposed by the leading analytical groups, as well as by the authors of
this publication. The typological characteristics of the upcoming
situations of socio-economic development of Russia are indicated.</description>
</item>
<item>
<title> Analysis of Solar Research Activities Published in North Korean Journals</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PKAS...36...37K</link>
<description>We have analyzed 42 research papers regarding on the solar astronomy
written by North Korea scientists to investigate the current status of
astronomical activities in North Korea. The papers are surveyed from the
'Bulletin of Astronomy', the 'Physics', the 'Bulletin of Academy of
Science', and the 'Natural Science' in North Korea, and SCI journals. In
addition, we refer to the presentation material announced in the 2015
IAU by director of Pyongyang Astronomical Observatory (PAO) and the 2013
OAD/IAU reports. We have analyzed the papers statistically according to
three criteria such as research subject, research field, and research
members. The main research subjects are the sunspot (28%), observation
system (21%), and space environments (19%). The research fields are
distributed with data analysis (50%), numerical method (29%), and
instrument development (21%). There have been 25 and 9 researchers in
the solar astronomy and space environment, respectively since 1995.
North Korea's solar research activities were also investigated in three
area: instrument, solar physics, and international research linkage. PAO
has operated two of sunspot telescope and solar horizontal telescope for
spectroscopy and polarimetry, but there is no specific information on
solar radio telescopes. North Korea has cooperated in solar research
with Europe and China. We expect that the results of this study will be
used as useful resource in supporting astronomical cooperation between
South and North Korea in the future..</description>
</item>
<item>
<title> External triggering of O-star formation by a cloud-cloud collision</title>
<link>https://ui.adsabs.harvard.edu/abs/2021PASJ...73S.338K</link>
<description>We have performed a multi-wavelength study of the mid-infrared bubble
S44 to investigate the origin of isolated high-mass star(s) and the
star-formation process around the bubble formed by the H II region. We
report on the results of new CO observations (&lt;SUP&gt;12&lt;/SUP&gt;CO,
&lt;SUP&gt;13&lt;/SUP&gt;CO J = 1-0, and &lt;SUP&gt;12&lt;/SUP&gt;CO J = 3-2) toward the
isolated bubble S44 using the NANTEN2, Mopra, and ASTE radio telescopes.
We found two velocity components at -84 km s&lt;SUP&gt;-1&lt;/SUP&gt; and -79 km
s&lt;SUP&gt;-1&lt;/SUP&gt; in the direction of the bubble. These two clouds are
likely to be physically associated with the bubble, because of the
enhanced &lt;SUP&gt;12&lt;/SUP&gt;CO J = 3-2/1-0 intensity ratio from a ring-like
structure affected by ultraviolet radiation from embedded high-mass
star(s) and of the morphological correspondence between the 8 m
emission and the CO distribution. Assuming a single object, we estimate
a spectral type of the embedded star inside the bubble to be O8.5-9
$({\sim}20\,M_{\odot})$ from the radio-continuum free-free emission. We
hypothesize that the two clouds collided with each other 3 Myr ago,
triggering the formation of the isolated high-mass star in S44, as also
occurred in RCW 120 and RCW 79. We argue that this scenario can explain
the origin of the isolated O-star inside the bubble.</description>
</item>
<item>
<title> Connection of the Intensity of the Flux of SCR Protons with the Velocity of the CME and with the Fading of the Radio Emission of the Sun in the Decameter Range</title>
<link>https://ui.adsabs.harvard.edu/abs/2021OAP....34...76I</link>
<description>The relationship between SCR and CME and with fading of the continuum of
noise storms and type IV radio bursts in the decameter range is
investigated. I was shown earlier that about 60% of CMEs associated with
solar proton events are accompanied by deep fading of the solar radio
emission in the decameter range, which coincides in time with CME
registration. It has also been shown that fading is characterized by
fading depth, the frequency bandwidth in which the fading occurs, as
well as the duration of the fading and the frequency at which the
maximum fading depth is observed. Further detailed studies have shown
that for proton events accompanied by fading of the solar radio emission
in the decameter range, the relationship between the intensity of the
SCR proton flux and the CME velocity is much worse than for events
without fading of the solar radio emission in the decameter range.
However, it was found that for such events, the relationship between the
flux of SCR protons and the CME velocity significantly increases if we
take into account the fading depth of the solar radio emission in the
decameter range. Earlier in (Isaeva, 2019), the results of a study of
the relationship between the intensity of fading of the continuum of
noise storms with the parameters of X-ray bursts, with the CME velocity
and the velocity of coronal shock waves, as well as with the intensity
of the SCR proton flux were presented. This paper presents the results
of studying the relationship between the intensity of the SCR proton
flux with the parameters of type II and IV radio bursts, as well as with
the CME velocity and with the velocity of coronal shock waves, depending
on the intensity of fading of the solar radio emission in the decameter
range at a frequency of 27 MHz. The frequency of 27 MHz was chosen
because in the region of this frequency the maximum fading depth of the
solar radio emission in the decameter range is observed.</description>
</item>
<item>
<title> Spectral signature of solar active region in millimetre and submillimetre wavelengths</title>
<link>https://ui.adsabs.harvard.edu/abs/2021MNRAS.500.1964V</link>
<description>Active regions were observed with different instruments covering the
spectral band from 17 to 405 GHz. The observations were made with the
Nobeyama Radioheliograph (17 GHz), the Atacama Large Millimetre Array
(107 and 238 GHz), and the Solar Submillimeter Telescope (212 and 405
GHz). A procedure was developed that allows the comparison between
observations taken with telescopes of different operational
characteristics and mainly of different spatial resolution. The
brightness temperature and density flux spectra of several active
regions corresponding to a different phase of its lifetime were
obtained. The flux density invariably increases in all cases from 107 to
405 GHz and the mean spectral index is 2 showing that the dominant
emission mechanism at submillimeter frequencies is still thermal. We
show that Solar Submillimeter Telescope (SST) and Atacama Large
Millimeter/submillimeter Array (ALMA) observations are compatible within
the uncertainties, a result of great interest for future joint
observations.</description>
</item>
<item>
<title> Performance Comparison of Power Divider and Fiber Splitter in the Fiber-Based Frequency Transmission System of Solar Radio Observation</title>
<link>https://ui.adsabs.harvard.edu/abs/2021IEEEA...924925L</link>
<description>Time-frequency synchronization plays an important role in the
construction of solar radio telescopes (such as heliograph and
interferometry). In the development of a synchronization system, time-
frequency signal is divided and transmitted to each antenna in an array,
therefore, the performance of the signal splitting devices determines
the quantity of the data. To address this situation, we designed a
frequency transmitting system, and conducted a test to compare the phase
difference among outputs (10 MHz - 1.4 GHz), and the deterioration of
the frequency stability (10 MHz  1GHz) brought by different splitting
devices (fiber splitter and power divider). The following results had
been obtained: 1) Phase difference introduced by both fiber splitter and
power divider can be restricted in a range of 4, and the fiber
splitter is rather stable, which indicate that a better imaging effect
of heliograph can be achieved when using fiber splitters. 2) Frequency
stability deterioration get better (worse) with increasing temperature
for fiber splitter (power divider) in the testing frequency range for a
short-time sampling (100 ms), and for a long-time sampling (10 min), the
frequency stability of different devices is determined by both
temperature and signal frequency. By estimating the SNR, the performance
of optical splitter is found to be slightly better than power splitter.
This article provides a basis for the selection and compensation of
frequency transfer system components for integrated aperture heliograph,
and provide a feasible solution of the construction of low-cost
radioheliograph.</description>
</item>
<item>
<title> Radio Measurements of the Magnetic field in the Solar Chromosphere and the Corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021FrASS...7...77A</link>
<description>The structure of the upper solar atmosphere, on all observable scales,
is intimately governed by the magnetic field. The same holds for a
variety of solar phenomena that constitute solar activity, from tiny
transient brightening to huge Coronal Mass Ejections. Due to inherent
difficulties in measuring magnetic field effects on atoms (Zeeman and
Hanle effects) in the corona, radio methods sensitive to electrons are
of primary importance in obtaining quantitative information about its
magnetic field. In this review we explore these methods and point out
their advantages and limitations. After a brief presentation of the
magneto-ionic theory of wave propagation in cold, collisionless plasmas,
we discuss how the magnetic field affects the radio emission produced by
incoherent emission mechanisms (free-free, gyroresonance and
gyrosynchrotron processes) and give examples of measurements of magnetic
filed parameters in the quiet sun, active regions and radio CMEs. We
proceed by discussing how the inversion of the sense of circular
polarization can be used to measure the field above active regions.
Subsequently we pass to coherent emission mechanisms and present results
of measurements from fiber bursts, zebra patterns and type II burst
emission. We close this review with a discussion of the variation of the
magnetic field, deduced by radio measurement, from the low corona up to
10 solar radii and with some thoughts about future work.</description>
</item>
<item>
<title> Imaging Spectroscopy of CME-associated Solar Radio Bursts using OVRO-LWA</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...906..132C</link>
<description>We present the first results of a solar radio event observed with the
Owens Valley Radio Observatory Long Wavelength Array at metric
wavelengths. We examine a complex event consisting of multiple radio
sources/bursts associated with a fast coronal mass ejection (CME) and an
M2.1 GOES soft X-ray flare from 2015 September 20. Images of 9 s cadence
are used to analyze the event over a 120 minute period, and solar
emission is observed out to a distance of 3.5 R&lt;SUB&gt;&lt;/SUB&gt;, with an
instantaneous bandwidth covering 22 MHz within the frequency range of
40-70 MHz. We present our results from the investigation of the radio
event, focusing particularly on one burst source that exhibits outward
motion, which we classify as a moving type IV burst. We image the event
at multiple frequencies and use the source centroids to obtain the
velocity for the outward motion. Spatial and temporal comparison with
observations of the CME in white light from the C2 coronagraph of the
Large Angle and Spectrometric COronagraph, indicates an association of
the outward motion with the core of the CME. By performing graduated-
cylindrical-shell reconstruction of the CME, we constrain the density in
the volume. The electron plasma frequency obtained from the density
estimates do not allow us to completely dismiss plasma emission as the
underlying mechanism. However, based on source height and smoothness of
the emission in frequency and time, we argue that gyrosynchrotron is the
more plausible mechanism. We use gyrosynchrotron spectral-fitting
techniques to estimate the evolving physical conditions during the
outward motion of this burst source.</description>
</item>
<item>
<title> ALMA and IRIS Observations of the Solar Chromosphere. II. Structure and Dynamics of Chromospheric Plages</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...906...83C</link>
<description>We propose and employ a novel empirical method for determining
chromospheric plage regions, which seems to better isolate a plage from
its surrounding regions than other methods commonly used. We caution
that isolating a plage from its immediate surroundings must be done with
care in order to successfully mitigate statistical biases that, for
instance, can impact quantitative comparisons between different
chromospheric observables. Using this methodology, our analysis suggests
that  = 1.25 mm free-free emission in plage regions observed with the
Atacama Large Millimeter/submillimeter Array (ALMA)/Band6 may not form
in the low chromosphere as previously thought, but rather in the upper
chromospheric parts of dynamic plage features (such as spicules and
other bright structures), i.e., near geometric heights of transition-
region temperatures. We investigate the high degree of similarity
between chromospheric plage features observed in ALMA/Band6 (at 1.25 mm
wavelengths) and the Interface Region Imaging Spectrograph (IRIS)/Si IV
at 1393 . We also show that IRIS/Mg II h and k are not as well
correlated with ALMA/Band6 as was previously thought, and we discuss
discrepancies with previous works. Lastly, we report indications of
chromospheric heating due to propagating shocks supported by the
ALMA/Band6 observations.</description>
</item>
<item>
<title> ALMA and IRIS Observations of the Solar Chromosphere. I. An On-disk Type II Spicule</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...906...82C</link>
<description>We present observations of the solar chromosphere obtained
simultaneously with the Atacama Large Millimeter/submillimeter Array
(ALMA) and the Interface Region Imaging Spectrograph. The observatories
targeted a chromospheric plage region of which the spatial distribution
(split between strongly and weakly magnetized regions) allowed the study
of linear-like structures in isolation, free of contamination from
background emission. Using these observations in conjunction with a
radiative magnetohydrodynamic 2.5D model covering the upper convection
zone all the way to the corona that considers nonequilibrium ionization
effects, we report the detection of an on-disk chromospheric spicule
with ALMA and confirm its multithermal nature.</description>
</item>
<item>
<title> On the Occurrence of Type IV Solar Radio Bursts in Solar Cycle 24 and Their Association with Coronal Mass Ejections</title>
<link>https://ui.adsabs.harvard.edu/abs/2021ApJ...906...79K</link>
<description>Solar activities, in particular coronal mass ejections (CMEs), are often
accompanied by bursts of radiation at meter wavelengths. Some of these
bursts have a long duration and extend over a wide frequency band,
namely, type IV radio bursts. However, the association of type IV bursts
with CMEs is still not well understood. In this article, we perform the
first statistical study of type IV solar radio bursts in solar cycle 24.
Our study includes a total of 446 type IV radio bursts that occurred
during this cycle. Our results show that a clear majority, 81% of type
IV bursts, were accompanied by CMEs, based on a temporal association
with white-light CME observations. However, we found that only 2.2% of
the CMEs are accompanied by type IV radio bursts. We categorized the
type IV bursts as moving or stationary based on their spectral
characteristics and found that only 18% of the total type IV bursts in
this study were moving type IV bursts. Our study suggests that type IV
bursts can occur with both "Fast" (500 km s&lt;SUP&gt;-1&lt;/SUP&gt;) and "Slow"
(&lt;500 km s&lt;SUP&gt;-1&lt;/SUP&gt;), and also both "Wide" (60) and "Narrow"
(&lt;60), CMEs. However, the moving type IV bursts in our study were
mostly associated with "Fast" and "Wide" CMEs (52%), similar to type II
radio bursts. Contrary to type II bursts, stationary type IV bursts have
a more uniform association with all CME types.</description>
</item>
<item>
<title> Ionospheric TEC prediction using Long Short-Term Memory deep learning network</title>
<link>https://ui.adsabs.harvard.edu/abs/2021Ap&amp;SS.366....3W</link>
<description>In this paper, the prediction model for ionospheric total electron
content (TEC) based on Long Short-Term Memory (LSTM) deep learning
network and its performance are discussed. The input parameters of the
model are previous values of daily TEC, solar radio flux at 10.7 cm
parameter of 81 day moving average (F107_81\oline), sunspot number
(SSN), geomagnetic Kp index, and disturbance storm time (Dst) index, and
the outputs are TEC values for the target day. TEC data from January 1,
2001 to December 31, 2016 were used in this study. The dataset almost
covers most of the years of the last two solar cycles (23, 24), and it
is separated as 81.3% for training, 6.2% for validation, and 12.5% for
testing. At BJFS IGS station (39.61 N, 115.89 E), LSTM yielded good
TEC estimates with an RMSE of 4.07 TECU in 2001, it was 33% and 48%
lower than the RMSE observed in TEC prediction using BP and IRI-2016
models, respectively. In the year of low solar activity (2016), the RMSE
predicted by LSTM was 1.78 TECU, it provided 30% and 54% lower RMSE for
TEC prediction than for BP and IRI-2016 models. Under the condition of
magnetic storm, the LSTM TEC predictions are more consistent with the
corresponding IGS Global Ionospheric Maps (GIMs) TEC than TEC
predictions by BP and IRI-2016 models. LSTM can better grasp the
influence of different external conditions on TEC. Seventeen grid points
along 120 E meridian in latitude range from 80 S to 80 N were
selected to further study the performance of LSTM model in different
latitude. Results show that the prediction accuracy of LSTM is better
than that of BP at different latitudes, especially at low latitudes. The
performances of the two models are highly correlated with latitude and
solar activity, and are both better than that of IRI-2016.</description>
</item>
<item>
<title> Study of ionospheric D region changes during solar flares using MF radar measurements</title>
<link>https://ui.adsabs.harvard.edu/abs/2021AdSpR..67..715Q</link>
<description>During solar flares, the X-ray radiation suddenly increases, resulting
in an increase in the electron density of the atmospheric D region and a
strong absorption of short-wave radio waves. Based on Langfang medium
frequency (MF) radar, this paper analyzed the variation characteristics
of D region in the lower ionosphere from 62 km to 82 km. The analysis
focused on multiple C-level and M-level solar flare events before and
after the large-scale flare event at 11:53 (UT) on September 6, 2017.
The results show that it is difficult to detect the electron density
over 70 km in Langfang during solar flares, but the electron density
value can be obtained as low as 62 km, and the stronger the flare
intensity, the lower the detectable electron density height. Besides,
the equal electron density height, the received power of X and O waves
will also be significantly reduced during the flares, and the reduction
of equal electron density height has a weak linear relationship with
flare intensity.</description>
</item>
<item>
<title> Radio observations of solar active regions at 7.36 and 37 GHz</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;AT...32..241K</link>
<description>We present solar radio observations that were made semi-simultaneously
with two Nordic-Baltic radio telescopes observing at two different
frequency bands, 7.36 GHz and 37 GHz. The two radio telescopes are the
Aalto University Metahovi radio telescope located in Kylmala, Finland,
and the Ventspils International Radio-Astronomy Center (VIRAC) radio
telescope located in Irbene, Latvia. The observations presented here
were made between autumn 2017 and autumn 2018. We use them to study the
active solar regions that are seen in the radio intensity maps at both
frequencies. We find that the location of the maximum intensity is
different for the two frequency bands, and that their peak intensities
do not correlate. Based on these findings we propose a simplified
scenario for how the radio sources can form at centimetre and millimetre
wavelengths.</description>
</item>
<item>
<title> LOFAR observations of radio burst source sizes and scattering in the solar corona</title>
<link>https://ui.adsabs.harvard.edu/abs/2021A&amp;A...645A..11M</link>
<description>Low frequency radio wave scattering and refraction can have a dramatic
effect on the observed size and position of radio sources in the solar
corona. The scattering and refraction is thought to be due to
fluctuations in electron density caused by turbulence. Hence,
determining the true radio source size can provide information on the
turbulence in coronal plasma. However, the lack of high spatial
resolution radio interferometric observations at low frequencies, such
as with the LOw Frequency ARray (LOFAR), has made it difficult to
determine the true radio source size and level of radio wave scattering.
Here we directly fit the visibilities of a LOFAR observation of a Type
IIIb radio burst with an elliptical Gaussian to determine its source
size and position. This circumvents the need to image the source and
then de-convolve LOFAR's point spread function, which can introduce
spurious effects to the source size and shape. For a burst at 34.76 MHz,
we find full width at half maximum (FWHM) heights along the major and
minor axes to be 18.8'  0.1' and 10.2'  0.1', respectively, at a plane
of sky heliocentric distance of 1.75 R&lt;SUB&gt;&lt;/SUB&gt;. Our results suggest
that the level of density fluctuations in the solar corona is the main
cause of the scattering of radio waves, resulting in large source sizes.
However, the magnitude of  may be smaller than what has been previously
derived in observations of radio wave scattering in tied-array images.</description>
</item>

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