Source Astrometry
Guest observers obtain coordinates for
their sources from the Kepler Input Catalog
(KIC). The source of the astrometry depends
on which catalog (or catalogs) contain data for that source. The
order for the choice of astrometric values is described in the
release notes for the Kepler Input Catalog. Those catalogs are
listed here, with an estimate of their positional accuracy.
1. Kepler Stellar Classification
Program; 50 milliarcseconds, data obtained closer to the
Kepler epoch, minimizing proper motion offsets
2.
Hipparcos; 10 milliarcseconds
3.
Tycho-2; for V brighter than 8.0; 20 milliarcseconds
4.
UCAC2; 40 milliarcseconds
5.
2MASS; 70 milliarcseconds
6.
USNO-B1.0; 200 milliarcseconds
The values listed in the KIC arise from the
first catalog in the above list that contains a measure for
that source. The source catalogs should be consulted for a
detailed discussion of astrometric accuracy. The Kepler Project
required positions to be accurate to 200 milliarcseconds, and
proper motions to 20 millarseconds per year.
Observed Astrometry
Observers will generally want to know where
their sources lie within the assigned target aperture. Image
centroids are calculated as part of the calibration pipeline,
within the Photometric Analysis (PA)
module. PA computes flux-weighted mean centroids for all stars, which
are tabulated in the light curve files, expressed as row and column pixels
values. These data provide an image centroid time series, and
enable observers to assess target placement during the observing sequence.
On each channel, a set of bright (but not
saturated), relatively isolated stars are chosen to provide a reference
grid for astrometry. Photometry for this set of reference stars
is processed within the Photometer Performance Assessment (PPA)
pipeline module to provide metrics of the photometric and
astrometric stability of the instrument. Image centroids for these
stars are used to create a "plate" solution specific for each
CCD channel. This solution is then interpolated to convert detector
coordinates (row, column) to celestial coordinates (RA, Dec).
In the currently released data (Q0-Q3),
both public and proprietary Guest Observer data, the derived
celestial coordinates are not provided in the light curve tables.
Analysis of centroid motion is not encumbered by the lack of this
calibration; both significant and more subtle motions can be
discerned in the centroid time series (detailed in the paper
mentioned below). In particular, the flux-weighted centroid will
respond to photometric variability when two or more stars are present
within the aperture. The centroid will appear to move in a systematic
manner as one star varys in brightness; the resulting motion time
series can be used to help identify false positive transit signatures.
We anticipate that astrometric coordinates will be included within
Pipeline Version 7.0, approximately coincident with the first Cycle 2
data release.
FFIs:   The full frame images
were designated as engineering data by the Project, and no astrometric
calibration was initally intended. MAST developed an astrometric solution
for the 8 Golden full-frame images, using the public astrometry.net tool,
developed by Blanton, Hogg, Lang, Mierle & Rowies. These 8 FFIs were taken
under ideal pointing and thermal stability at the start of the mission,
and are avaiable
here. Subsequent FFIs do not yet contain astrometry. Plans for the
possible astrometric calibration of all FFIs is under review.
Astrometric Science with Kepler
The high signal-to-noise ratios
achieved with Kepler permit a high level of astrometric accuracy,
despite the large pixel scale and large field of view. In principle
the Kepler data can be used to determine parallaxes and proper motion
for tens of thousands of stars, and explore more subtle motions,
hinting at planetary companions. The Kepler Project
is working towards understanding the astrometric precision of the
data, and its potential applications. Based on analysis of
the Q0+Q1 data, Monet provides an estimate of Kepler's astrometric
precision of ~4 milliarcseconds over a single 30 minute observation
(1 long cadence). Additional details are provided in an
initial
report
on astrometric results from Kepler.
The abtract from this paper (Monet etal 2010):
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