American Astronomical Society
Quick Search:Help  
The Astrophysical Journal
Athens/Institutional login
IOP login: Password:   
Create account | Alerts | Contact us
IOP Publishing | AAS Homepage | ApJ Homepage | This Journal | Search | Authors | Referees | Librarians | User Options | Help |

FORMATION OF HIGH-REDSHIFT (z>6) QUASARS DRIVEN BY NUCLEAR STARBURSTS

Nozomu Kawakatu et al 2009 ApJ 706 676-686   doi: 10.1088/0004-637X/706/1/676  Help

   PDF (790 KB) | HTML | References

Nozomu Kawakatu1,3 and Keiichi Wada1,2
1 National Astronomical Observatory of Japan, 2-21-1 Osawa, Mitaka, Tokyo 181-8588, Japan
2 Graduate School of Science and Engineering, Kagoshima University, Kagoshima 890-8580, Japan
3 JSPS Fellow.
E-mail: kawakatu@th.nao.ac.jp and wada@cfca.jp

ABSTRACT. Based on the physical model of a supermassive black hole (SMBH) growth via gas accretion in a circumnuclear disk (CND) proposed by Kawakatu & Wada, we describe the formation of high-z (z>6) quasars (QSOs) whose BH masses are M BH>109 M sun. We derive the necessary conditions to form QSOs at z>6 by only gas accretion: (1) a large mass supply with M sup>1010 M sunfrom host galaxies to CNDs, because the final BH mass is only 1%-10% of the total supplied mass from QSO hosts. (2) High star formation efficiency for a rapid BH growth which is comparable to high-z starburst galaxies such as submillimeter galaxies. We also find that if the BH growth is limited by the Eddington accretion, the final BH mass is greatly suppressed when the period of mass supply from hosts, t sup, is shorter than the Eddington timescale. Thus, the super-Eddington growth is required for the QSO formation while t sup, which is determined by the efficiency of angular momentum transfer, is shorter than ~108 yr. The evolution of the QSO luminosity depends on the redshift z i at which accretion onto a seed BH is initiated. In other words, the brighter QSOs at z>6 favor the late growth of SMBHs (i.e., z i ≈ 10) rather than early growth (i.e., z i ≈ 30). For z i ≈ 10, t sup sime 108 yr is shorter than that of the star formation in the CND. Thus, the gas in the CND can accrete onto a BH more efficiently, compared with the case for z i ≈ 30 (or t sup ≈ 109 yr). Moreover, we predict the observable properties and the evolution of QSOs at z>6. In a QSO phase, there should exist a stellar rich massive CND, whose gas mass is about 10% of the dynamical mass inside ~0.1-1 kpc. On the other hand, in a phase where the BH grows (i.e., a proto-QSO phase), the proto-QSO has a gas-rich massive CND whose gas mass is comparable to the dynamical mass. Compared with the observed properties of the distant QSO SDSS J1148+5251 observed at z = 6.42, we predict that SDSS J1148+5251 corresponds to the scenario of the late growth of SMBH with z i ~ 10, which is accompanied by a massive CNDs with M g ≈ 5 × 1010 M sun and the luminous nuclear starburst L SBat infrared band with L SB ≈ 1047 erg s–1. Moreover, we predict that the progenitor of SDSS J1148+5251 can be the super-Eddington object. These predictions can be verified by ALMA, SPICA, and JWST.

Key words: black hole physics; early universe; galaxies: active; galaxies: nuclei; galaxies: starburst; ISM: structure

Print publication: Issue 1 (2009 November 20)
Received 2009 July 1, accepted for publication 2009 October 9
Published 2009 November 4

Bookmark and Share Post to CiteUlike | Post to Connotea | Post to Bibsonomy

 

Find related articles





Article options

Authors & Referees

Nanotechnology news and resourcesPW launch banner
 
Content finder
  Full Search
  Help


  
Setup information is available for Adobe Acrobat.
EndNote, ProCite ® and Reference Manager ® are registered trademarks of ISI Researchsoft.
Copyright © Institute of Physics and IOP Publishing Limited 2009 - electronic design and all rights in the EJs software.
© The American Astronomical Society ("AAS") - the names of any journals published by AAS and the content of all such journals.
Use of this service is subject to compliance with the terms and conditions of use. In particular, reselling and systematic downloading of files is prohibited.
Help: Cookies | Data Protection.