BLACK HOLE MASSES OF INTERMEDIATE-REDSHIFT QUASARS: NEAR-INFRARED SPECTROSCOPY
Journal Article
·
· Astrophysical Journal
- Department of Astronomy, Ohio State University, 140 West 18th Avenue, Columbus, OH 43 210 (United States)
- Department of Astronomy and Astrophysics, Pennsylvania State University, 525 Davey Lab, University Park, PA 16 802 (United States)
- MPI fuer extraterrestrische Physik, Giessenbachstr., D-85 748 Garching (Germany)
We present near-infrared spectra of 10 luminous, intermediate-redshift quasars (z {approx_equal}2; L {sub bol} {approx_equal} 10{sup 47} erg s{sup -1}), observed with SofI at the NTT of ESO/La Silla. With these rest-frame optical spectra we probe the H{beta}-[O III] emission line region. Using the standard scaling relation involving the width of the H{beta} line and the continuum luminosity, we measure black hole (BH) masses in the range of {approx}2 x 10{sup 9}{approx}< M {sub bh} {approx}< 10{sup 10} M {sub sun} for these sources. We also used Sloan Digital Sky Survey spectra to probe Mg II {lambda}2798 and C IV {lambda}1549 emission lines and used these for BH mass measurements as well. The BH mass estimates using C IV {lambda}1549 are on average smaller by about 60% than those based on H{beta}. The massive BHs we observe could not have grown by simple radiatively efficient accretion at the observed accretion rate starting from seeds of up to a thousand solar masses. About 10% of the observed BH mass must have been accumulated by earlier merger events and radiatively inefficient accretion. Radiatively efficient accretion would further grow these BHs to masses of several 10{sup 9} M {sub sun} in 2-3 e-folding times, i.e., in several 10{sup 8} yr. This scenario is consistent with recent models of BH growth. The H{beta}-based Eddington luminosity ratios are in the range of {approx}0.2-0.7, with an average of (L {sub bol}/L {sub edd}) = 0.39 {+-} 0.05. The L {sub bol}/L {sub edd} ratio distribution follows a lognormal distribution which is consistent with prior studies of quasars with comparable luminosity. We also find that the gas metallicity of the broad-line region is super-solar with {approx}3 Z/Z {sub sun}, based on N III]{lambda}1750/O III]{lambda}1663 and N V {lambda}1240/C IV {lambda}1549 emission line ratios. We find no correlation of the gas metallicity with the optical Fe II emission line strength in our small sample, contrary to a recent suggestion.
- OSTI ID:
- 21300622
- Journal Information:
- Astrophysical Journal, Journal Name: Astrophysical Journal Journal Issue: 2 Vol. 696; ISSN ASJOAB; ISSN 0004-637X
- Country of Publication:
- United States
- Language:
- English
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