The SDSS Data Release 5 (DR5)
DR5 is to be described in a paper submitted to ApJS (2006)
Contents
What DR5 contains
The DR5 imaging data cover about 8000 square degrees, and include
information on roughly 215 million objects. The DR5 spectroscopic
data include data from 1278 main survey plates of 640 spectra each,
and cover 5600 square degrees. In addition, DR5
contains 361 "extra" and "special" plates:
- 62 "extra" plate/MJD combinations which are repeat
observations of 53 distinct main survey plates,
- 289 distinct "special" plates, which are observations
of spectroscopic targets, mostly in the southern galactic cap, which
were selected by the collaboration for a series of specialized science
programs (note that some of these plates are outside of the DR5
imaging area),
- and 10 "extraspecial" repeat observations of
"special" plates.
There is a separate page describing the special plates in
DR5.
The DR5 footprint is defined by all non-repeating survey-quality
imaging runs within the a priori defined elliptical survey area in the
Nothern Galactic Cap, and three stripes in the Southern Galactic Cap
obtained prior to 1 July 2005, and the spectroscopy associated with
that area as well as the extra and special plates
obtained before that date. In fact, 34 square degrees of imaging data
in the Nothern Galactic Cap lie outside this ellipse. While the DR5
scans do not repeat a given area of sky, they do overlap to some
extent, and the data in the overlaps are included in earlier releases
as well. The sky coverage of the imaging and spectroscopic data that
make up DR5 are given on the coverage
page. The natural unit of imaging data is a run; the DR5 contains
data from (about) 240 runs in the best database, and (about) 242 runs
in the target database.
A total of 183 square degrees of sky are different runs between target
and best, the majority along the Equatorial Stripe in the Fall sky.
Except for the sky coverage, the pipelines and databases are
identical in DR5, DR4, DR3 and DR2. Thus, DR5 is (very nearly) a proper
superset of DR4, which is a superset of DR3, which is a superset of DR2.
The DR2 included reprocessing of all data included in DR1, and
those data in EDR that pass our data-quality criteria for
the official survey. For details
about what changed from DR3 to DR4, please refer to About DR4 on
the DR4 web site.
There is a table photoAuxAll in the CAS that contains errors and
covariances for the right ascension and declination as well as
galactic coordinates for all objects. See the CAS
Schema Browser entry for photoAuxAll and the astrometry algorithms
description for the calculation of RA, DEC errors.
New for DR5
- Photometric redshifts for galaxies The DR1 Catalog Archive Server had a
table with photometric redshifts for galaxies, including galaxies
fainter than those in the spectroscopic survey. The redshifts
have now been computed and loaded into the database for
DR5; there are now two different tables of photometric redshifts
provided by two different groups within SDSS.
XXX Currently, the only documentation I'm aware of is that in sdss-archive
message 2805 and references therein.
- Coverage masks Detailed coverage masks which
allow large-scale structure resarchers to easily calculate
power spectrum and related quantities, and which allow the
computation of the area covered by statistical samples such as the
quasar sample are now in DR5. XXX: links to sample queries etc
- photoAuxAll XXX Something's new in the photoAuxAll
table, but I don't know what in detail - at least SEGUE targeting
flags will (have?) appear(ed?) there. The schema browser doesn't
report any differences to DR4.
- XXX The runQA bug is now fixed and the proper
colors are used in all quality determinations. (Is that right?)
Not entirely new, but still noteworthy
Stetson and RC3 catalogs are in CAS
There are two tables stetson and RC3 in
the holding photometric catalogs. stetson includes
stellar B, V, R, and I Kron-Cousins photometry with an accuracy of
0.02 mag or better from Stetson
(2000), as downloaded from the Canadian Astronomy Data
Centre photometric standards Web site. RC3 contains
data from the Third
Reference Catalog of Galaxies (de Vaucouleurs et al. 1991). Both
are included in the CAS to allow cross-reference to SDSS data.
Photometric transformations between SDSS and Kron-Cousins systems
There is a long page describing transformations between
SDSS (ugriz) and Kron-Cousins (UBVRcIc) photometry.
Imaging caveats
The following caveats apply unchanged to DR5.
Overestimation of sky levels in the vicinity of bright
objects
A study of weak lensing in the SDSS imaging data (Mandelbaum
et al. 2005) found a systematic, 5% decrease in the number
density of faint objects within 90′′ of bright
(r < 18) galaxies. This was found to be due to a
systematic overestimation of the sky levels in the vicinity of bright
objects, which of course will affect all the measured photometric
quantities of faint objects, including the classification as stars and
galaxies. The brighter the object, the larger the overestimation of
sky; indeed, restricting to foreground galaxies brighter than
r = 16, the number density of fainter galaxies is 10% below
the mean. The effect is due to the way in which the sky levels are
estimated in the SDSS; they can be biased upward by the faint outer
isophotes of a bright galaxy (see the EDR paper [Stoughton
et al. 2002]; see also the discussion in Strauss
et al. 2002). Closer than 40′′ to the bright objects,
the intrinsic clustering of galaxies makes it difficult to assess the
problem. This problem is most relevant for applications that involve
correlating positions of bright objects with faint ones, yielding a
spurious anti-correlation on the affected scales. We are currently
investigating changes to the imaging pipeline to address this problem.
Red leak to the u filter and very red objects
The u filter has a natural red leak around 7100 Å
which is supposed to be blocked by an interference coating. However,
under the vacuum in the camera, the wavelength cutoff of the
interference coating has shifted redward (see the discussion in the
EDR paper), allowing some of this red leak through. The extent of
this contamination is different for each camera column. It is not
completely clear if the effect is deterministic; there is some
evidence that it is variable from one run to another with very similar
conditions in a given camera column. Roughly speaking, however, this
is a 0.02 magnitude effect in the u magnitudes for mid-K
stars (and galaxies of similar color), increasing to 0.06 magnitude
for M0 stars (r-i ~ 0.5), 0.2 magnitude at r-i ~
1.2, and 0.3 magnitude at r-i = 1.5. There is a large
dispersion in the red leak for the redder stars, caused by three
effects:
- The differences in the detailed red
leak response from column to column, beating with the complex red
spectra of these objects.
- The almost certain time variability of the red leak.
- The red-leak images on the u chips are out of focus and are
not centered at the same place as the u image because of
lateral color in the optics and differential refraction - this means
that the fraction of the red-leak flux recovered by the PSF fitting
depends on the amount of centroid displacement.
To make matters even more complicated, this is a detector
effect. This means that it is not the real i and
z which drive the excess, but the instrumental colors
(i.e., including the effects of atmospheric extinction), so the leak
is worse at high airmass, when the true ultraviolet flux is heavily
absorbed but the infrared flux is relatively unaffected. Given these
complications, we cannot recommend a specific correction to the
u-band magnitudes of red stars, and warn the user of these
data about over-interpreting results on colors involving the
u band for stars later than K.
Bias in sky determination
There is a slight and only recently recognized downward bias in the
determination of the sky level in the photometry, at the level of
roughly 0.1 DN per pixel. This is apparent if one compares
large-aperture and PSF photometry of faint stars; the bias is of order
29 mag arcsec-2 in r. This, together with
scattered light problems in the u band, can cause of order
10% errors in the u band Petrosian fluxes of large
galaxies.
Zeropoint of the photometric system
The SDSS photometry is intended to be on the AB system (Oke
& Gunn 1983), by which a magnitude 0 object should have the
same counts as a source of Fnu =
3631 Jy. However, this is known not to be exactly true, such that the
photometric zeropoints are slightly off the AB standard. We continue
to work to pin down these shifts. Our present estimate, based on
comparison to the STIS standards of Bohlin,
Dickinson, & Calzetti~(2001) and confirmed by SDSS photometry and
spectroscopy of fainter hot white dwarfs, is that the u
band zeropoint is in error by 0.04 mag, uAB =
uSDSS - 0.04 mag, and that g, r, and
i are close to AB. These statements are certainly not
precise to better than 0.01 mag; in addition, they depend critically
on the system response of the SDSS 2.5-meter, which was measured by
Doi et al. (2004, in preparation). The z band zeropoint is
not as certain at this time, but there is mild evidence that it may be
shifted by about 0.02 mag in the sense zAB =
zSDSS + 0.02 mag. The large shift in the
u band was expected because the adopted magnitude of the
SDSS standard BD+17 in Fukugita
et al.(1996) was computed at zero airmass, thereby making the
assumed u response bluer than that of the USNO system
response.
Holes in the imaging data
About 0.3% of the DR5 imaging footprint area
(about 10/square degree) for DR5 are marked as
holes. These are indicated in the CAS by setting
quality=5 (HOLE) in the tsField file and
field table and given in the list of quality holes, which
contains further details about the holes and quality flags, including
a information about a table in the CAS which allows
one to query for quality information about each field of data.
Problems with one u chip
The u chip in the third column of the camera is read out
on two amplifiers. On occasion, electronic problems on this chip
caused one of the two amplifiers to fail, meaning that half the chip
has no detected objects on it. This was a problem for only two of the
105 imaging runs included in DR5: run 2190, which includes a total of
360 frames in two separate contiguous pieces on strip 12N (centered
roughly at delta = +5 degrees in the North Galactic Cap; NGC), and run
2189, which includes 76 frames on stripe 36N near the northern
boundary of the contiguous area in the NGC. The relevant frames are
flagged as bad in the quality flag; in addition,
individual objects in this region have the u band flagged
as NOTCHECKED_CENTER (or, for objects which straddle the
boundary between the two amplifiers, LOCAL_EDGE ). Richards
et al (2002) describe how the quasar selection algorithm handles
such data; the net effect is that no quasars are selected by the
ugri branch of the algorithm for these data.
Spectroscopy caveats
Zero equivalent width of emission lines, especially H alpha
There is a bug in the line-measurement code that has been in use
since DR3 which gives some emission lines an equivalent width of zero,
even though there is a significant line detection. The aim of the
change introducing the bug had been to determine the equivalent width
by integrating the spectrum, instead of using the parameters of a
fitted Gaussian. The Gauss-fit equivalent width can be recovered from the
fit parameters using the usual expression EW = 2.5066 * sigma *
height / continuum .
Main survey spectra which are not marked sciencePrimary =
1 in CAS
Due to a bug in the pipelines, there are no tsTargets*.fits files for
plates 1617-1620, 1623, and 1652. As a consequence, the objects from
this plates do not have entries in the target and
targetInfo tables in the CAS. Hence they are not marked
sciencePrimary = 1 and do not appear in the default
specObj and specPhoto views, which provide a
filtered set of unique science spectra and form the basis of all
query interfaces. Use the specObjAll and and
specPhotoAll tables to access spectra from these plate
in the CAS.
Note about galactic extinction correction
The EDR and DR1 data nominally corrected for galactic extinction.
The spectrophotometry since DR2 is vastly improved compared to DR1,
but the final calibrated spectra in DR2 and beyond are not
corrected for foreground Galactic reddening (a relatively small
effect; the median E(B-V) over the survey is 0.034). Users
of spectra should note that the fractional improvement in
spectrophotometry from DR1 to DR2 and beyond was much greater than the
extinction correction itself. As the SDSS includes a substantial
number of spectra of galactic stars, a decision has been taken
not to apply any extinction correction to spectra,
since it would only be appropriate for extragalactic objects, but to
report the observational result of the SDSS, namely, the spectrum
including galactic extinction.
Problematic plates
A small number of plates suffered from a variety of minor problems
affecting the quality of the spectrophotometry (but not of
redshifts). See the list under Plates with
problematic spectrophotometry on the data products page for
spectra.
Mismatches between the spectroscopic and imaging data
For various reasons, a small fraction of the spectroscopic objects
do not have a counterpart in the best object catalogs. In
addition, the DR5 does not contain photometric information for some of
the special plates, and
the retrieval of photometric data from the CAS database requires
special care for objects from the special plates. See the caveat
about mismatches
between spectra and images on the data products page for
spectra.
Advanced features not yet available in DR5
There are a number of advanced features or data products that are
not yet available in DR5, but will be in the near future.
Last modified: Mon Apr 10 21:23:29 BST 2006
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