The Astrophysical Journal · 2009 · 516 citations · 239 references
Natural SciencesAstronomyPhysicsAstrophysicsRadio AstronomyX-ray AstronomyDark MatterExtragalactic Infrared AstronomyExtragalactic Radio AstronomyExtragalactic X-ray SourcesRedshift SurveysActive Galactic Nuclei ContributionActive Galactic Nuclei Infrared EmissionActive Galactic Nucleus ContributionDark Matter Halo EvolutionGalaxy Color EvolutionGalaxy Evolution In The InfraredObscured Active Galactic NucleiX-ray Surveys
We explore the connection between different classes of active galactic nuclei (AGNs) and the evolution of their host galaxies, by deriving host galaxy properties, clustering, and Eddington ratios of AGNs selected in the radio, Xray, and infrared (IR) wavebands. We study a sample of 585 AGNs at 0.25 <z< 0.8 using redshifts from the AGN and Galaxy Evolution Survey (AGES). We select AGNs with observations in the radio at 1.4 GHz from the Westerbork Synthesis Radio Telescope, X-rays from the Chandra XBootes Survey, and mid-IR from ¨ the Spitzer IRAC Shallow Survey. The radio, X-ray, and IR AGN samples show only modest overlap, indicating that to the flux limits of the survey, they represent largely distinct classes of AGNs. We derive host galaxy colors and luminosities, as well as Eddington ratios, for obscured or optically faint AGNs. We also measure the two-point cross-correlation between AGNs and galaxies on scales of 0.3–10 h−1 Mpc, and derive typical dark matter halo masses. We find that: (1) radio AGNs are mainly found in luminous red sequence galaxies, are strongly clustered (with Mhalo ∼ 3 × 1013 h−1 M), and have very low Eddington ratios λ 10−3; (2) X-ray-selected AGNs are preferentially found in galaxies that lie in the “green valley” of color–magnitude space and are clustered similar to the typical AGES galaxies (Mhalo ∼ 1013 h−1 M), with 10−3 λ 1; (3) IR AGNs reside in slightly bluer, slightly less luminous galaxies than X-ray AGNs, are weakly clustered (Mhalo 1012h−1 M), and have λ > 10−2. We interpret these results in terms of a simple model of AGN and galaxy evolution, whereby a “quasar” phase and the growth of the stellar bulge occurs when a galaxy’s dark matter halo reaches a critical mass between ∼ 1012 and 1013 M. After this event, star formation ceases and AGN accretion shifts from radiatively efficient (optical- and IR-bright) to radiatively inefficient (optically faint, radio-bright) modes. Ke
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The Two Micron All Sky Survey (2MASS)
Michael F. Skrutskie, R. M. Cutri, R. Stiening et al. · The Astronomical Journal · 2006 · 12.2K citations · Full text
SExtractor: Software for source extraction
E. Bertin, S. Arnouts · Astronomy and Astrophysics Supplement Series · 1996 · 11K citations · Full text
The Sloan Digital Sky Survey: Technical Summary
Donald G. York, Jennifer Adelman, John E. Anderson et al. · The Astronomical Journal · 2000 · 10.5K citations · Full text
Natural Sciences, Astronomy, Physics +14