2012ApJ...752...39T


Query : 2012ApJ...752...39T

2012ApJ...752...39T - Astrophys. J., 752, 39 (2012/June-2)

The halo masses and galaxy environments of hyperluminous QSOs at z ≃ 2.7 in the Keck baryonic structure survey.

TRAINOR R.F. and STEIDEL C.C.

Abstract (from CDS):

We present an analysis of the galaxy distribution surrounding 15 of the most luminous ( ≳ 1014 L☉; M1450≃ -30) QSOs in the sky with z ≃ 2.7. Our data are drawn from the Keck Baryonic Structure Survey, which has been optimized to examine the small-scale interplay between galaxies and the intergalactic medium during the peak of the galaxy formation era at z ∼ 2-3. In this work, we use the positions and spectroscopic redshifts of 1558 galaxies that lie within ∼3' (4.2 h–1 comoving Mpc; cMpc) of the hyperluminous QSO (HLQSO) sight line in 1 of 15 independent survey fields, together with new measurements of the HLQSO systemic redshifts. By combining the spatial and redshift distributions, we measure the galaxy-HLQSO cross-correlation function, the galaxy-galaxy autocorrelation function, and the characteristic scale of galaxy overdensities surrounding the sites of exceedingly rare, extremely rapid, black hole accretion. On average, the HLQSOs lie within significant galaxy overdensities, characterized by a velocity dispersion σv≃ 200 km/s and a transverse angular scale of ∼25'' (∼200 physical kpc). We argue that such scales are expected for small groups with log (Mh/M ☉) ≃ 13. The galaxy-HLQSO cross-correlation function has a best-fit correlation length r GQ0= (7.3±1.3) h–1 cMpc, while the galaxy autocorrelation measured from the spectroscopic galaxy sample in the same fields has r GG0= (6.0±0.5) h–1 cMpc. Based on a comparison with simulations evaluated at z ∼ 2.6, these values imply that a typical galaxy lives in a host halo with log (Mh/M☉) = 11.9±0.1, while HLQSOs inhabit host halos of log (Mh/M☉) = 12.3±0.5. In spite of the extremely large black hole masses implied by their observed luminosities [log (MBH/M☉) ≳ 9.7], it appears that HLQSOs do not require environments very different from their much less luminous QSO counterparts. Evidently, the exceedingly low space density of HLQSOs ( ≲ 10–9 c/Mpc3) results from a one-in-a-million event on scales {Lt}1 Mpc, and not from being hosted by rare dark matter halos.

Abstract Copyright: ∼

Journal keyword(s): galaxies: high-redshift - large-scale structure of universe - quasars: general

Simbad objects: 16

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Number of rows : 16
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 PHL 957 QSO 01 03 11.2741573824 +13 16 17.809871484   16.97 16.57     ~ 350 0
2 QSO B0105+1619 QSO 01 08 06.4234637880 +16 35 49.968976200   16.9       ~ 63 0
3 QSO B0142-100A LeQ 01 45 17.3 -09 45 12     16.9     ~ 41 1
4 QSO B0207-0019 QSO 02 09 50.7145927344 -00 05 06.457492608   17.45 17.21     ~ 133 0
5 QSO B0449-1645 QSO 04 52 14.2529886192 -16 40 16.386415284   18.0 17.0 17.8   ~ 48 1
6 QSO J0821+3107 BLL 08 21 07.6135883448 +31 07 51.147374376   17.59 17.28     ~ 72 1
7 CSO 38 QSO 10 11 55.5947671920 +29 41 41.595330804   16.28 16.05     ~ 117 0
8 QSO B1217+4957 QSO 12 19 30.7755423144 +49 40 52.196980584   17.50 17.21     ~ 60 0
9 QSO B1442+2931 QSO 14 44 53.5398146832 +29 19 05.691187272   16.59 16.38     ~ 83 0
10 QSO J1551+1911 QSO 15 51 52.4688797112 +19 11 04.014875400           ~ 66 0
11 QSO B1603+3820 QSO 16 04 55.3999673952 +38 12 01.628642808   16.37 15.99     ~ 60 0
12 QSO B1623+268A QSO 16 25 48.0865431168 +26 44 32.575702092   18.59 18.41     ~ 89 0
13 QSO B1623+269 QSO 16 25 48.7980918960 +26 46 58.784527056   17.77 17.64     ~ 109 0
14 HS 1700+6416 QSO 17 01 00.6194059368 +64 12 09.118892376   16.39 16.17     ~ 382 0
15 LBQS 2206-1958A QSO 22 08 52.0729138920 -19 43 59.866776948   17.49 17.33     ~ 223 0
16 QSO B2343+125 QSO 23 46 28.200 +12 49 00.00     17.5     ~ 143 2

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