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The script inherits some limitations from ASTROM
, and some
from CCDPACK's findoff
.
The limitations due to ASTROM
are as follows (quoted from
SUN/5, sect. 5):
ASTROM
aims to deliver results better than 1 arcsec
from typical Schmidt plate measurements, and better than
0.1 arcsec from carefully measured JKT and AAT plates
etc. Astrometric specialists will,
nonetheless, be aware of a number of shortcomings, including
the following:
- The fit is limited to a 6-coefficient linear model
plus cubic distortion and plate tilt. Colour effects --
arising for example from chromatic aberrations in the
camera optics -- are not allowed for, no magnitude or
image shape terms are included in the model, and the
refraction cannot be adjusted automatically.
- The zonal distortions of the reference catalogues are
neglected.
- There is no provision for the simultaneous fitting
of more than one plate. This prevents an extended area
being modelled via overlapping plates, and the
determination of proper motion and parallax from plates
taken at different epochs.
- Only rudimentary error information is produced.
Despite these limitations, which stem mainly from the need
for simplicity of use, the accuracy of the result tends in
practice to be dominated by the quality of the input data
rather than by ASTROM
itself.Further, ASTROM
requires that at least 10 reference stars
are available. Since autoastrom
obtains its reference stars
from well-stocked catalogues, this is not a problem in
practice.
The restrictions arising from findoff
are similarly slight,
and should not be a problem if the initial astrometry is
good enough. It's not at present completely clear
exactly what `good enough' means.
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Autoastrometry for Mosaics
Starlink User Note 242
Norman Gray
24 August 2001. Release v0-5-8. Last updated 25 August 2003