2013MNRAS.428.1382K


Query : 2013MNRAS.428.1382K

2013MNRAS.428.1382K - Mon. Not. R. Astron. Soc., 428, 1382-1394 (2013/January-2)

Clustering, bias and the accretion mode of X-ray-selected AGN.

KOUTOULIDIS L., PLIONIS M., GEORGANTOPOULOS I. and FANIDAKIS N.

Abstract (from CDS):

We present the spatial clustering properties of 1466 X-ray-selected active galactic nuclei (AGN) compiled from the Chandra Deep Field (CDF) North and South, extended CDF-S, COSMOS and All-wavelength Extended Groth strip International Survey (AEGIS) fields in the 0.5-8 keV band. The X-ray sources span the redshift interval 0 < z < 3 and have a median value of {bar}z=0.976. We employ the projected two-point correlation function to infer the spatial clustering and find a clustering length of r0 = 7.2±0.6h-1 Mpc and a slope of γ = 1.48 ±0.12, which corresponds to a bias of b({bar}z)=2.26 ±0.16. Using two different halo bias models, we consistently estimate an average dark-matter host halo mass of Mh ≃ 1.3(± 0.3)x1013h-1M☉. The X-ray AGN bias and the corresponding dark-matter host halo mass are significantly higher than the corresponding values of optically selected AGN (at the same redshifts). The redshift evolution of the X-ray-selected AGN bias indicates, in agreement with other recent studies, that a unique dark-matter halo mass does not fit well the bias at all the different redshifts probed. Furthermore, we investigate if there is a dependence of the clustering strength on X-ray luminosity. To this end we consider only 650 sources around z ∼ 1 and we apply a procedure to disentangle the dependence of clustering on redshift. We find indications for a positive dependence of the clustering length on X-ray luminosity, in the sense that the more luminous sources have a larger clustering length and hence a higher dark-matter halo mass. In detail we find for an average luminosity difference of δ log10Lx ≃ 1 a halo mass difference of a factor of ∼ 3.

These findings appear to be consistent with a galaxy formation model where the gas accreted on to the supermassive black hole in intermediate-luminosity AGN comes mostly from the hot-halo atmosphere around the host galaxy.


Abstract Copyright: © 2012 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2012)

Journal keyword(s): galaxies: active - X-rays: galaxies - large scale structure of Universe - dark matter

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
2 NAME Extended Chandra Deep Field South reg 03 32 30.0 -27 48 20           ~ 862 0
3 NAME COSMOS Field reg 10 00 28.60 +02 12 21.0           ~ 3639 0
4 NAME Chandra Deep Field-North reg 12 36.8 +62 13           ~ 686 0
5 NAME Extended Groth Strip reg 14 19 +52.8           ~ 1023 0

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