Published August 1, 2011 | Version v1
Journal article

THE XMM-NEWTON WIDE FIELD SURVEY IN THE COSMOS FIELD: REDSHIFT EVOLUTION OF AGN BIAS AND SUBDOMINANT ROLE OF MERGERS IN TRIGGERING MODERATE-LUMINOSITY AGNs AT REDSHIFTS UP TO 2.2

  • 1. Max-Planck-Institut fuer Plasmaphysik, D-85748 Garching (Germany)
  • 2. Max-Planck-Institute fuer Extraterrestrische Physik, D-85748 Garching (Germany)
  • 3. Center for Space Science Technology, University of Maryland, Baltimore County, Baltimore, MD 21250 (United States)
  • 4. Instituto de Astronomia, Universidad Nacional Autonoma de Mexico, Ensenada (Mexico)
  • 5. INAF-Osservatorio Astronomico di Bologna, 40127 Bologna (Italy)
  • 6. Max-Planck-Institute fuer Astrophysik, D-85748 Garching (Germany)
  • 7. Astronomy Department, University of California, Berkeley, Berkeley CA 94720-7450 (United States)
  • 8. Observatoire de Paris, LERMA, 75014 Paris (France)
  • 9. Institute for the Physics and Mathematics of the Universe, University of Tokyo, Kashiwa-shi, Chiba 277-8583 (Japan)

Description

We present a study of the redshift evolution of the projected correlation function of 593 X-ray selected active galactic nuclei (AGNs) with IAB < 23 and spectroscopic redshifts z < 4, extracted from the 0.5-2 keV X-ray mosaic of the 2.13 deg2 XMM- Cosmic Evolution Survey (COSMOS). We introduce a method to estimate the average bias of the AGN sample and the mass of AGN hosting halos, solving the sample variance using the halo model and taking into account the growth of the structure over time. We find evidence of a redshift evolution of the bias factor for the total population of XMM-COSMOS AGNs from b-bar ( z-bar =0.92)=2.30±0.11 to b-bar ( z-bar =1.94)=4.37±0.27 with an average mass of the hosting dark matter (DM) halos log M0(h-1 Msun) ∼ 13.12 ± 0.12 that remains constant at all z < 2. Splitting our sample into broad optical line AGNs (BL), AGNs without broad optical lines (NL), and X-ray unobscured and obscured AGNs, we observe an increase of the bias with redshift in the range z-bar = 0.7-2.25 and z-bar = 0.6-1.5 which corresponds to a constant halo mass of log M0(h-1 Msun) ∼ 13.28 ± 0.07 and log M0(h-1 Msun) ∼ 13.00 ± 0.06 for BL/X-ray unobscured AGNs and NL/X-ray obscured AGNs, respectively. The theoretical models, which assume a quasar phase triggered by major mergers, cannot reproduce the high bias factors and DM halo masses found for X-ray selected BL AGNs with LBOL ∼ 2 x 1045 erg s-1. Our work extends up to z ∼ 2.2 the z ∼< 1 statement that, for moderate-luminosity X-ray selected BL AGNs, the contribution from major mergers is outnumbered by other processes, possibly secular ones such as tidal disruptions or disk instabilities.

Availability note (English)

Available from http://dx.doi.org/10.1088/0004-637X/736/2/99

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
736
Journal Issue
2
Journal Page Range
[15 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United States
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
43055993
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
CORRELATION FUNCTIONS; GALACTIC EVOLUTION; GALAXY NUCLEI; LUMINOSITY; QUASARS; RED SHIFT
Descriptors DEC
COSMIC RADIO SOURCES; EVOLUTION; FUNCTIONS; OPTICAL PROPERTIES; PHYSICAL PROPERTIES