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  • The XMM-Newton Wide-field S...
    Brusa, M; Civano, F; Comastri, A; Miyaji, T; Salvato, M; Zamorani, G; Cappelluti, N; Fiore, F; Hasinger, G; Mainieri, V; Merloni, A; Bongiorno, A; Capak, P; Elvis, M; Gilli, R; Hao, H; Jahnke, K; Koekemoer, A. M; Ilbert, O; Le Floc'h, E; Lusso, E; Mignoli, M; Schinnerer, E; Silverman, J. D; Treister, E; Trump, J. D; Vignali, C; Zamojski, M; Aldcroft, T; Aussel, H; Bardelli, S; Bolzonella, M; Cappi, A; Caputi, K; Contini, T; Finoguenov, A; Fruscione, A; Garilli, B; Impey, C. D; Iovino, A; Iwasawa, K; Kampczyk, P; Kartaltepe, J; Kneib, J. P; Knobel, C; Kovac, K; Lamareille, F; Leborgne, J.-F; Le Brun, V; Le Fevre, O; Lilly, S. J; Maier, C; McCracken, H. J; Pello, R; Peng, Y.-J; Perez-Montero, E; de Ravel, L; Sanders, D; Scodeggio, M; Scoville, N. Z; Tanaka, M; Taniguchi, Y; Tasca, L; de la Torre, S; Tresse, L; Vergani, D; Zucca, E

    The Astrophysical journal, 06/2010, Letnik: 716, Številka: 1
    Journal Article

    We report the final optical identifications of the medium-depth ({approx}60 ks), contiguous (2 deg{sup 2}) XMM-Newton survey of the COSMOS field. XMM-Newton has detected {approx}1800 X-ray sources down to limiting fluxes of {approx}5 x 10{sup -16}, {approx}3 x 10{sup -15}, and {approx}7 x 10{sup -15} erg cm{sup -2} s{sup -1} in the 0.5-2 keV, 2-10 keV, and 5-10 keV bands, respectively ({approx}1 x 10{sup -15}, {approx}6 x 10{sup -15}, and {approx}1 x 10{sup -14} erg cm{sup -2} s{sup -1}, in the three bands, respectively, over 50% of the area). The work is complemented by an extensive collection of multiwavelength data from 24 {mu}m to UV, available from the COSMOS survey, for each of the X-ray sources, including spectroscopic redshifts for {approx}>50% of the sample, and high-quality photometric redshifts for the rest. The XMM and multiwavelength flux limits are well matched: 1760 (98%) of the X-ray sources have optical counterparts, 1711 ({approx}95%) have IRAC counterparts, and 1394 ({approx}78%) have MIPS 24 {mu}m detections. Thanks to the redshift completeness (almost 100%) we were able to constrain the high-luminosity tail of the X-ray luminosity function confirming that the peak of the number density of log L{sub X} > 44.5 active galactic nuclei (AGNs) is at z {approx} 2. Spectroscopically identified obscured and unobscured AGNs, as well as normal and star-forming galaxies, present well-defined optical and infrared properties. We devised a robust method to identify a sample of {approx}150 high-redshift (z > 1), obscured AGN candidates for which optical spectroscopy is not available. We were able to determine that the fraction of the obscured AGN population at the highest (L{sub X} > 10{sup 44} erg s{sup -1}) X-ray luminosity is {approx}15%-30% when selection effects are taken into account, providing an important observational constraint for X-ray background synthesis. We studied in detail the optical spectrum and the overall spectral energy distribution of a prototypical Type 2 QSO, caught in a stage transitioning from being starburst dominated to AGN dominated, which was possible to isolate only thanks to the combination of X-ray and infrared observations.