Caveats and Limitations
While the Chandra Source Catalog (CSC) is capable of supporting many
diverse scientific investigations, users should carefully consider the
limitations of the CSC when assessing the efficacy of the catalog for
their particular line of enquiry.
General
In particular, users of the CSC should be aware that there may be
fundamental and significant selection effects that restrict the source
content of the catalog and which therefore may limit scientific
studies that require an unbiased source sample. The CSC is
constructed from pointed observations obtained using the Chandra X-ray
Observatory; it is not an all-sky catalog, and does not include
sources detected to a uniform depth. Furthermore, the first release
of the catalog includes only point and compact sources, with observed
(i.e., un-deconvolved) spatial extents < ~30 arcsec. Sources larger
than this will not be detected with the current CSC algorithms. In
addition, observations of fields containing highly extended
sources have been excluded from the catalog. In most cases if
the extended emission is
restricted to a single ACIS CCD, then the data from the
remaining CCDs is included in the catalog.
Users of catalog database views (as opposed to an official
catalog release view) should also be aware that the contents of
the database are subject to revision as processing progresses,
and a small fraction
of sources present in the catalog database may not meet all of the
catalog release quality assurance requirements.
Specific Caveats and Limitations applicable through CSC
release 1
-
In release 1.0 of the catalog, the var_flag property in the
Master Sources Table was not correctly populated. This error
is fixed in release 1.0.1. Catalog users who extracted this
property should consider re-running their queries against the
new release.
-
We have identified an error in variability determination for a
subset of sources near chip edges. This will affect sources that
dither across multiple CCDs, where one or more of the CCDs are
off or are otherwise excluded. Events from the off/excluded CCDs
are not included in the source lightcurve nor in any other source
properties; however, the fractional area correction (calculated
with
the dither_region
tool) will still include areas from the off/excluded CCDs when
applying the variability tests. This can lead to a false
variability signal from all three variability
tests (Kuiper, Kolmogorov-Smirnov, and Gregory-Loredo).
This variability will not necessarily be on the dither time
scale, therefore
the dither_warning_flag
may be set to FALSE and thus not serve as an indicator of this
problem. Likewise,
the multi_chip_code
flag may be set to 0 if all but one CCD is
off/excluded. Thus, highly variable sources with a
non-zero edge_code should be treated with caution when assessing variability properties.
-
The background is modeled using a single low spatial frequency
component, with the addition of a high spatial frequency "streak
map" for ACIS observations. The detectability of sources may be
compromised in crowded regions near bright sources (or near bright,
extended emission that has not been excluded) where the
background has a strong spatial dependence. The emission contributes
to the background detection annulus around each source and increases
the background variance, hence reducing the significance of the
source detection. An example of this problem can be seen near the
center of Obsid 6420;
see the science study
"CSC Release 1: Missing
sources in crowded fields" for further details.
-
All position angles recorded in
the Source Observations
Table are defined relative to the tangent plane projection of
the individual observation. The 0 degree position angle reference
is defined to be parallel to the true North direction at the
location of the tangent plane reference point, rather than relative
to local true North.
-
The source position error
ellipse is replaced by a source position error circle in
this release. This limitation will be lifted in a future release of
the catalog.
-
The deconvolved
source extent is determined using a circular
Gaussian parameterization in this release, rather than a rotated
elliptical Gaussian parameterization. This limitation will be
lifted in a future release of the catalog.
-
The mean chip coordinates (chipx, chipy) of a source are computed
without including the effect of the mean dy, dz, dtheta offsets
from the aspect solution. For some observations these offsets are
of order 15 arcsec (~30 ACIS pixels) in both dy and dz, so the mean
chip coordinates may be uncertain by this amount.
Specific Caveats and Limitations for certain ObsIds
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