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XMMCPHOTZ - XMM-Newton COSMOS (XMM-COSMOS) Survey Photometric Redshift Catalog |
HEASARC Archive |
In addition, in this study the authors released revised photometric redshifts for the 1735 optical counterparts of the XMM-detected sources over the entire 2 deg2 of COSMOS, and these are the sources listed in the present table. For 248 sources, their updated photometric redshift differs from the previous release by Delta-z > 0.2. These changes are predominantly due to the inclusion of newly available deep H-band^ photometry (HAB = 24 mag). The authors illustrate once again the importance of a spectroscopic training sample and how an assumption about the nature of a source together, with the number and the depth of the available bands, influences the accuracy of the photometric redshifts determined for AGN. These considerations should be kept in mind when defining the observational strategies of upcoming large surveys targeting AGNs, such as eROSITA at X-ray energies and the Australian Square Kilometre Array Pathfinder Evolutionary Map of the Universe in the radio band.
This table contains the photometric redshifts and related quantities for 1735 XMM-Newton sources over the entire 2 square degrees of the COSMOS field. Notice that in the original as-published paper no positional information was provided. The HEASARC has assumed that the source numbers used in the present catalog are in the same source numbering scheme as used by Cappelluti et al. (2009, A&A, 497, 635, the XMM-Newton Wide-Field Survey in the COSMOS Field Point-like X-ray Source Catalog, available at the HEASARC as the XMMCOSMOS table) and thus obtained the positions and (position-based) names corresponding to these X-ray sources from the latter.
Dissecting Photometric Redshift for Active Galactic Nucleus Using XMM- and Chandra-COSMOS Samples Salvato M., Ilbert O., Hasinger G., Rau A., Civano F., Zamorani G., Brusa M., Elvis M., Vignali C., Aussel H., Comastri A., Fiore F., Le Floc'h E., Mainieri V., Bardelli S., Bolzonella M., Bongiorno A., Capak P., Caputi K., Cappelluti N., Carollo C. M., Contini T., Garilli B., Iovino A., Fotopoulou S., Fruscione A., Gilli R., Halliday C., Kneib J.-P., Kakazu Y., Kartaltepe J. S., Koekemoer A. M., Kovac K., Ideue Y., Ikeda H., Impey C. D., Le Fevre O., Lamareille F., Lanzuisi G., Le Borgne J.-F., Le Brun V., Lilly S., Maier C., Manohar S., Masters D., McCracken H., Messias H., Mignoli M., Mobasher B., Nagao T., Pello R., Puccetti S., Perez-Montero E., Renzini A., Sargent M., Sanders D. B., Scodeggio M., Scoville N., Shopbell P., Silvermann J., Taniguchi Y., Tasca L., Tresse L., Trump J. R., Zucca E. <Astrophys. J., 742, 61 (2011)> =2011ApJ...742...61S
Source_Number
A unique identification number for each source in the catalog
from Brusa et al. (2010, ApJ, 716, 348, available at the HEASARC as the
XMMCOSMOID table). This source numbering scheme is also used by Cappelluti et
al. (2009, A&A, 497, 635, the XMM-Newton COSMOS Survey X-Ray Point Source
Catalog, available at the HEASARC as the XMMCOSMOS table) from which the
positions and (position-based) names corresponding to these sources .
Name
The XMM-Newton source name, following the standard IAU position-based
convention, with the prefix "XMMU" for "XMM-Newton X-ray Observatory,
Unregistered" and the J2000.0 source coordinates (taken from the XMMCOSMOS
table).
RA
The Right Ascension of the XMM-Newton source in the selected equinox.
This was given in J2000.0 coordinates to a precision of 1 microdegree (3.6 mas)
in the XMMCOSMOS table.
Dec
The Declination of the XMM-Newton source in the selected equinox. This
was given in J2000.0 coordinates to a precision of 1 microdegree (3.6 mas) in
the XMMCOSMOS table.
LII
The Galactic Longitude of the XMM-Newton source.
BII
The Galactic Latitude of the XMM-Newton source.
Ilbert_Source_Number
The optical identifier of the source as reported in the
optical photometric catalog "cosmos_phot_20081101" available on the COSMOS
webpage http://irsa.ipac.caltech.edu/data/COSMOS/tables/photometry/ and/or in
the photo-z catalog (Ilbert et al. 2009, ApJ, 690, 1236). A null value
for this parameter indicates that the XMM-Newton source has no counterpart in
these catalogs.
Phot_Redshift
The photometric redshift of the source. The authors found 53 candidate stars
in this sample of which 32 had been already spectroscopically confirmed. A
redshift of 0.000 has been assigned in such cases and no information on the
PDFz, best fit template, and variability is given.
Phot_Redshift_Min
The lower limit to the value of the photometric redshift. The authors found
53 candidate stars in this sample of which 32 had been already
spectroscopically confirmed. A minimum redshift of 0.000 has been assigned in
such cases and no information on the PDFz, best fit template, and
variability is given.
Phot_Redshift_Max
The upper limit to the value of the photometric redshift. The authors found
53 candidate stars in this sample of which 32 had been already
spectroscopically confirmed. A maximum redshift of 0.000 has been assigned in
such cases and no information on the PDFz, best fit template, and
variability is given.
Redshift_Pdf
The redshift probability distribution function PDFz.
No value is provided for objects classified as stars.
Best_Fit_Template
The best-fit template to the spectral energy distribution
(SED) using the codes 1-30 as described in Table 2 of Salvato et al. (2009,
ApJ, 690, 1250) and adding 100 to the codes 1-31 in the Ilbert et al. (2009,
ApJ, 690, 1236) library. No value is provided for objects classified as stars.
Morph_Class
The source morphological classification (Leauthard et al. 2007,
ApJS, 172, 219) where values of 1 or 3 indicate extended structure and 2 or
4 indicate point-like sources. Null values represented by -999 in the
original table have been replaced by nulls in this HEASARC representation.
Variability
The variability parameter VAR as defined in equation (1) of
Salvato et al. (2009, ApJ, 690, 1250). This describes the deviation of the
optical photometry from a reference epoch (2006, the time of
quasi-simultaneous optical and Spitzer/IRAC observations). See Section 3 of
the reference paper for more details.