Up: CCD astrometry of faint
The X, Y coordinates of the reference stars on the photographic
plates were measured to
(
at the plate scale)
with a digital Zeiss-Jena Ascorecord measuring machine. Only
one setting was made on the catalogue, secondary and
tertiary reference stars. In the few cases in which the optical
counterpart of the CERS was measurable directly on the long
exposure plate, at least 4 settings were made on it. The
photographic position thus
determined was used to check for
consistency. Plates were measured both in direct and reverse
positions in an effort to cancel possible systematic errors in
the X, Y
values. Six term (const., X, Y, XY, X2, Y2)
quadratic relations were used in the reductions. Third order
terms were not included because the flat field of the Maksutov
Astrograph is almost free of distortions. Also, since all plates
were taken near culmination, refraction third order terms were
not important. The standard deviation of the differences
between
calculated and catalogue values of the Hipparcos stars turned out
to be
in X and
in Y.
All raw CCD frames were first calibrated (overscan, zero
level and flat field corrected) using standard IRAF (version
2.10, NOAO, University of Arizona) tasks. The four CCD images
taken of each CERS were then registered and combined using
algorithms available in the IRAF IMAGES package, to produce the
final image from which the X, Y coordinates of the PSF centroids
of the CERS and the tertiary stars were extracted. This latter
step was carried out by means of the PEAK task within the DAOPHOT
package (Stetson 1987). Although this package was originally
designed for photometric programs, it has proven to be an
excellent tool to compute image positions (Monet 1992; Anguita &
Loyola 1995).
Table 2:
Optical positions in the ICRS system of 15 compact
extragalactic
radio sources

CT stands for Cerro Tololo,
LC stands for Las Campanas,
Phot. indicates a position derived from direct
photography. |
Up: CCD astrometry of faint
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