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The angular clustering of infrared-selected obscured and unobscured quasars
Authors
A. D. Myers
Abazajian
+105 more
Alexander
Alexander
Antonucci
Assef
Bardeen
Beifiori
Blanton
Booth
Brodwin
Brown
Chen
Coil
Coil
Colín
Comastri
Conroy
Croom
Croom
Croton
da Ângela
Decarli
Di Matteo
Donley
Donoso
Eisenstein
Elvis
Fan
Ferrarese
Ferrarese
Fitzpatrick
Geach
Gebhardt
Goulding
Guo
Hamilton
Hartley
Hickox
Hickox
Hickox
Hopkins
Hopkins
J. E. Geach
K. N. Hainline
Kaiser
Kelly
King
Kirkpatrick
Kochanek
Komatsu
Kormendy
Kormendy
Kravtsov
Krumpe
Lacy
Lacy
Landy
Leistedt
Li
Limber
M. A. DiPompeo
Magorrian
Mateos
Mateos
Myers
Myers
Myers
Myers
Padmanabhan
Page
Peacock
Peebles
Peng
Porciani
R. C. Hickox
Richards
Richards
Ross
Ross
Ross
Sanders
Schlegel
Scranton
Setti
Shankar
Shen
Shen
Shen
Sherwin
Sheth
Smith
Stern
Stern
Stoughton
Swanson
Tinker
Tinker
Tinker
Totsuji
Tremaine
Vale
White
White
Woo
Wright
York
Publication date
3 June 2014
Publisher
'Oxford University Press (OUP)'
Doi
View
on
arXiv
Abstract
This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society. ©: 2014 The Author(s). Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.Recent studies of luminous infrared-selected active galactic nuclei (AGN) suggest that the reddest, most obscured objects display a higher angular clustering amplitude, and thus reside in higher mass darkmatter haloes. This is a direct contradiction to the prediction of the simplest unification-by-orientation models of AGN and quasars. However, clustering measurements depend strongly on the 'mask' that removes low-quality data and describes the sky and selection function.We find that applying a robust, conservative mask to WISE-selected quasars yields a weaker but still significant difference in the bias between obscured and unobscured quasars. These findings are consistent with results from previous Spitzer surveys, and removes any scale dependence of the bias. For obscured quasars with =0.99, we measure a bias of bq = 2.67 ± 0.16, corresponding to a halo mass of log(Mh/M⊙h-1) = 13.3 ± 0.1, while for unobscured sources with = 1.04 we find bq = 2.04 ± 0.17 with a halo mass log(Mh/M⊙h-1) = 12.8 ± 0.1. This improved measurement indicates that WISE-selected obscured quasars reside in haloes only a few times more massive than the haloes of their unobscured counterparts, a reduction in the factor of ∼10 larger halo mass as has been previously reported using WISE-selected samples. Additionally, an abundance matching analysis yields lifetimes for both obscured and unobscured quasar phases on the order of a few 100 Myr (∼1 per cent of the Hubble time) - however, the obscured phase lasts roughly twice as long, in tension with many model predictions.Peer reviewe
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