Quasars at z = 6: The Survival of the Fittest

The Sloan Digital Sky Survey has detected luminous quasars at very high redshift, z > 6. Follow-up observations indicate that at least some of these quasars are powered by supermassive black holes (SMBHs), with masses in excess of 109 M☉. SMBHs, therefore, seem to have already existed when the universe was less than 1 Gyr old and the bulk of galaxy formation had yet to take place. Here we investigate the extent to which accretion and dynamical processes influence the early growth of SMBHs. We assess the impact of (1) black hole mergers, (2) the influence of the merger efficiency, and (3) the negative contribution due to dynamical effects, which can kick black holes out of their host halos (gravitational recoil). We find that if accretion is always limited by the Eddington rate via a thin disk, the maximum allowed radiative efficiency (or spin) to reproduce the luminosity function at z = 6 is ϵ = 0.12 (or = 0.8), against the adverse effect of the gravitational recoil. Dynamical effects unquestionably cannot be neglected in studies of high-redshift SMBHs. If black holes can accrete at a supercritical rate during an early phase, reproducing the observed SMBH mass values is not an issue, even in the case that the recoil velocity is in the upper limit range, as the mass ratios of merging binaries are skewed toward low values, where the gravitational recoil effect is very mild. We propose that SMBH growth at early times is very selective, and efficient only for black holes hosted in high density peak halos.

[1]  Cambridge,et al.  Supermassive black hole formation during the assembly of pre-galactic discs , 2006, astro-ph/0606159.

[2]  M. Colpi,et al.  Laser Interferometer Space Antenna double black holes : dynamics in gaseous nuclear discs , 2006 .

[3]  T. Damour,et al.  Gravitational recoil during binary black hole coalescence using the effective one body approach , 2006, gr-qc/0602117.

[4]  M. Rees,et al.  Formation of supermassive black holes by direct collapse in pre-galactic haloes , 2006, astro-ph/0602363.

[5]  L. Moscardini,et al.  Modelling the quasi-stellar object luminosity and spatial clustering at low redshifts , 2006, astro-ph/0602361.

[6]  M. Colpi,et al.  LISA double black holes: Dynamics in gaseous nuclear discs , 2005, astro-ph/0509813.

[7]  P. Armitage,et al.  Eccentricity of Supermassive Black Hole Binaries Coalescing from Gas-rich Mergers , 2005, astro-ph/0508493.

[8]  C. Will,et al.  Gravitational Recoil of Inspiraling Black Hole Binaries to Second Post-Newtonian Order , 2005, astro-ph/0507692.

[9]  X. Delfosse,et al.  First Results from the Canada-France High-z Quasar Survey: Constraints on the z = 6 Quasar Luminosity Function and the Quasar Contribution to Reionization , 2005, astro-ph/0507183.

[10]  U. California,et al.  The distribution and kinematics of early high-σ peaks in present-day haloes: implications for rare objects and old stellar populations , 2005, astro-ph/0506615.

[11]  M. Rees,et al.  Rapid Growth of High-Redshift Black Holes , 2005, astro-ph/0506040.

[12]  P. Hopkins,et al.  The Evolution of the MBH-σ Relation , 2005, astro-ph/0506038.

[13]  T. D. Matteo,et al.  Energy input from quasars regulates the growth and activity of black holes and their host galaxies , 2005, Nature.

[14]  M. Perna Dynamical evolution of intermediate mass black holes and their observable signatures in the nearby Universe , 2005, astro-ph/0501345.

[15]  S. Shapiro Spin, Accretion, and the Cosmological Growth of Supermassive Black Holes , 2004, astro-ph/0411156.

[16]  M. Rees,et al.  ApJ, in press Preprint typeset using L ATEX style emulateapj v. 04/03/99 THE DISTRIBUTION AND COSMIC EVOLUTION OF MASSIVE BLACK HOLE SPINS , 2004 .

[17]  USA,et al.  ApJ, in press Preprint typeset using L ATEX style emulateapj v. 04/03/99 THE GRAVITATIONAL WAVE SIGNAL FROM MASSIVE BLACK HOLE BINARIES AND ITS CONTRIBUTION TO THE LISA DATA STREAM , 2004 .

[18]  V. Debattista,et al.  The Fate of Supermassive Black Holes and the Evolution of the MBH-σ Relation in Merging Galaxies: The Effect of Gaseous Dissipation , 2004, astro-ph/0407407.

[19]  J. Krolik,et al.  Magnetically Driven Accretion Flows in the Kerr Metric. IV. Dynamical Properties of the Inner Disk , 2004, astro-ph/0409231.

[20]  T. D. Matteo,et al.  Tracing the cosmological assembly of stars and supermassive black holes in galaxies , 2004, astro-ph/0409187.

[21]  Jaiyul Yoo,et al.  Formation of the Black Holes in the Highest Redshift Quasars , 2004, astro-ph/0406217.

[22]  Z. Haiman Constraints from Gravitational Recoil on the Growth of Supermassive Black Holes at High Redshift , 2004, astro-ph/0404196.

[23]  P. Madau,et al.  The Effect of Gravitational-Wave Recoil on the Demography of Massive Black Holes , 2004, astro-ph/0403295.

[24]  A. Merloni The anti‐hierarchical growth of supermassive black holes , 2004, astro-ph/0402495.

[25]  E. al.,et al.  Down-sizing in galaxy formation at z~1 , 2004, astro-ph/0402276.

[26]  D. Holz,et al.  How Black Holes Get Their Kicks: Gravitational Radiation Recoil Revisited , 2004, astro-ph/0402056.

[27]  D. Holz,et al.  Consequences of Gravitational Radiation Recoil , 2004, astro-ph/0402057.

[28]  R. Maiolino,et al.  Local supermassive black holes, relics of active galactic nuclei and the X-ray background , 2003, astro-ph/0311619.

[29]  A. University,et al.  Massive black hole seeds from low angular momentum material , 2003, astro-ph/0311487.

[30]  D. Mardones,et al.  The Role of Gas in the Merging of Massive Black Holes in Galactic Nuclei. II. Black Hole Merging in a Nuclear Gas Disk , 2003, astro-ph/0406304.

[31]  M. Rees,et al.  Early Reionization by Miniquasars , 2003, astro-ph/0310223.

[32]  S. Shapiro,et al.  Black Hole Spin Evolution , 2003, astro-ph/0310886.

[33]  L. Ho,et al.  Iron Emission in the z = 6.4 Quasar SDSS J114816.64+525150.3 , 2003, astro-ph/0308005.

[34]  China.,et al.  Double—double radio galaxies: remnants of merged supermassive binary black holes , 2003, astro-ph/0310045.

[35]  W. Brandt,et al.  Very High Redshift X-Ray-selected Active Galactic Nuclei in the Chandra Deep Field-North , 2003, astro-ph/0301232.

[36]  A. Loeb,et al.  Formation of the First Supermassive Black Holes , 2002, astro-ph/0212400.

[37]  Piero Madau,et al.  The Assembly and Merging History of Supermassive Black Holes in Hierarchical Models of Galaxy Formation , 2002, astro-ph/0207276.

[38]  D. Richstone,et al.  The Cosmic Density of Massive Black Holes from Galaxy Velocity Dispersions , 2002, astro-ph/0210573.

[39]  S. Tremaine,et al.  The Slope of the Black Hole Mass versus Velocity Dispersion Correlation , 2002, astro-ph/0203468.

[40]  L. Ferrarese Beyond the Bulge: A Fundamental Relation between Supermassive Black Holes and Dark Matter Halos , 2002, astro-ph/0203469.

[41]  S. Tremaine,et al.  Observational constraints on growth of massive black holes , 2002, astro-ph/0203082.

[42]  Z. Haiman,et al.  Second-Generation Objects in the Universe: Radiative Cooling and Collapse of Halos with Virial Temperatures above 104 K , 2001, astro-ph/0108071.

[43]  V. Narayanan,et al.  A Survey of z > 5.8 Quasars in the Sloan Digital Sky Survey. I. Discovery of Three New Quasars and the Spatial Density of Luminous Quasars at z ∼ 6 , 2001, astro-ph/0108063.

[44]  Martin J. Rees,et al.  ApJ, in press Preprint typeset using L ATEX style emulateapj v. 04/03/99 MASSIVE BLACK HOLES AS POPULATION III REMNANTS , 2001 .

[45]  F. Nakamura,et al.  On the Initial Mass Function of Population III Stars , 2000, astro-ph/0010464.

[46]  M. Rees,et al.  Early Metal Enrichment of the Intergalactic Medium by Pregalactic Outflows , 2000, astro-ph/0010158.

[47]  H. Rix,et al.  Binary Black Hole Mergers from Planet-like Migrations , 1999, The Astrophysical journal.

[48]  R. Nichol,et al.  High-Redshift Quasars Found in Sloan Digital Sky Survey Commissioning Data , 1999, astro-ph/0103228.

[49]  S. White,et al.  A Universal Density Profile from Hierarchical Clustering , 1996, astro-ph/9611107.

[50]  L. Hernquist,et al.  Gasdynamics and starbursts in major mergers , 1995, astro-ph/9512099.

[51]  L. Hernquist,et al.  Ultraluminous starbursts in major mergers , 1994, astro-ph/9405039.

[52]  M. Fitchett The influence of gravitational wave momentum losses on the centre of mass motion of a Newtonian binary system , 1983 .

[53]  D. Meier,et al.  Thick accretion disks - Self-similar, supercritical models , 1982 .

[54]  M. Rees,et al.  Massive black hole binaries in active galactic nuclei , 1980, Nature.

[55]  M. Begelman Can a spherically accreting black hole radiate very near the Eddington limit , 1979 .

[56]  F. Hoyle,et al.  On the Mechanism of Accretion by Stars , 1944 .