Black hole masses and enrichment of z ∼ 6 SDSS quasars

被引:196
作者
Kurk, Jaron D. [1 ]
Walter, Fabian
Fan, Xiaohui
Jiang, Linhua
Riechers, Dominik A.
Rix, Hans-Walter
Pentericci, Laura
Strauss, Michael A.
Carilli, Chris
Wagner, Stefan
机构
[1] Max Planck Inst Astron, D-69117 Heidelberg, Germany
[2] Univ Arizona, Steward Observ, Tucson, AZ 85721 USA
[3] Osserv Astron Roma, I-00040 Monte Porzio Catone, Italy
[4] Princeton Univ, Dept Astrophys Sci, Princeton, NJ 08544 USA
[5] Natl Radio Astron Observ, Socorro, NM 87801 USA
[6] Landessternwarte Heidelberg, D-69117 Heidelberg, Germany
关键词
galaxies : evolution; galaxies : formation; galaxies : fundamental parameters galaxies; high-redshift; quasars; individual; (J000552.34-000655.8; J083643.85+005453.3; J130608.26+035626.3; J103027.10+052455.0; J141111.29+121737.4);
D O I
10.1086/521596
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present sensitive near-infrared spectroscopic observations for a sample of five z similar to 6 quasars. These quasars are among the most distant, currently known quasars in the universe. The spectra have been obtained using ISAAC at the VLT and include the C IV, Mg II, and Fe II lines. We measure the Fe II/Mg II line ratio, as an observational proxy for the Fe/alpha-element ratio. We derive a ratio of 2: 7 +/- 0: 8 for our sample, which is similar to that found for lower redshift quasars; i. e., we provide additional evidence for the lack of evolution in the Fe II/Mg II line ratio of quasars up to the highest redshifts. This result demonstrates that star formation must have commenced at z >= 8 in the quasar hosts. The line widths of the Mg II andCiv lines give two estimates for the black hole masses. A third estimate is given by assuming that the quasars emit at their Eddington luminosity. The derived masses using these three methods agree well, implying that the quasars are not likely to be strongly lensed. We derive central black hole masses of (0.3-5.2) x 10(9) M circle dot. We use the difference between the redshift of Mg II (a proxy for the systemic redshift of the quasar) and the onset of the Gunn-Peterson trough to derive the extent of the ionized Stromgren spheres around our target quasars. The derived physical radii are about 5 Mpc. Using a simple ionization model, the emission of the central quasars would need of order 10(6)-10(8) yr to create these cavities. As the e- folding timescale for the central accreting black hole is on the order of a few times 107 yr, it can grow by one e- folding or less within this time span.
引用
收藏
页码:32 / 44
页数:13
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