The XMM-Newton wide-field survey in the COSMOS field: III. optical identification and multiwavelength properties of a large sample of X-ray selected sources
M. Brusa, G. Zamorani, A. Comastri, G. Hasinger, N. Cappelluti, F. Civano, A. Finoguenov, V. Mainieri, M. Salvato, C. Vignali, M. Elvis, F. Fiore, R. Gilli, C. D. Impey, S. J. Lilly, M. Mignoli, J. Silverman, J. Trump, C. M. Urry, R. Bender, P. Capak, J. P. Huchra, J. P. Kneib, A. Koekemoer, A. Leauthaud, I. Lehmann, R. Massey, I. Matute, P. J. McCarthy, H. J. McCracken, J. Rhodes, N. Z. Scoville, Y. Taniguchi, D. Thompson
Abstract
[ABRIGED] We present the optical identification of a sample of 695 X-ray sources detected in the first 1.3 deg2 of the XMM-COSMOS survey, down to a 0.5-2 keV (2-10 keV) limiting flux of ~10-15 erg cm-2 s-1 (~5x10-15 erg cm-2 s-1). We were able to associate a candidate optical counterpart to ~90% (626) of the X-ray sources, while for the remaining ~10% of the sources we were not able to provide a unique optical association due to the faintness of the possible optical counterparts (IAB>25) or to the presence of multiple optical sources within the XMM-Newton error circles. We also cross-correlated the candidate optical counterparts with the Subaru multicolor and ACS catalogs and with the Magellan/IMACS, zCOSMOS and literature spectroscopic data; the spectroscopic sample comprises 248 objects (~40% of the full sample). Our analysis reveals that for ~80% of the counterparts there is a very good agreement between the spectroscopic classification, the morphological parameters as derived from ACS data, and the optical to near infrared colors. About 20% of the sources show an apparent mismatch between the morphological and spectroscopic classifications. All the ``extended'' BL AGN lie at redshift <1.5, while the redshift distribution of the full BL AGN population peaks at z~1.5. Our analysis also suggests that the Type 2/Type 1 ratio decreases towards high luminosities, in qualitative agreement with the results from X-ray spectral analysis and the most recent modeling of the X-ray luminosity function evolution.
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