2020ApJ...896...40Z


Query : 2020ApJ...896...40Z

2020ApJ...896...40Z - Astrophys. J., 896, 40-40 (2020/June-2)

C IV emission-line properties and uncertainties in black hole mass estimates of z ∼ 3.5 Quasars.

ZUO W., WU X.-B., FAN X., GREEN R., YI W., SCHULZE A., WANG R. and BIAN F.

Abstract (from CDS):

Using a high-luminosity (Lbol ∼ 1047.5-1048.3 erg s–1), high-redshift (3.2 < z < 3.8) quasar sample of 19 quasars with optical and near-infrared spectroscopy, we investigate the reliability of the C IV-based black hole mass estimates (MBH). The median logarithm of the C IV- and Hβ-based MBH ratios is 0.110 dex, with a scatter of 0.647 dex. The C IV-to-Hβ BH mass differences are significantly correlated with the C IV FWHMs, blueshifts, and asymmetries. Corrections of the C IV FWHM using the blueshift and asymmetry reduce the scatter of the mass differences by ∼0.04-0.2 dex. Quasars in our sample accrete at the Eddington ratio REDD > 0.3 and cover a considerable range of blueshifts, with 18/19 of the quasars showing C IV blueshifts (with the median value of 1126 km s–1) and 14/19 of the quasars showing C IV blueshifts larger than 500 km s–1. It suggests that not all quasars with high Eddington ratios show large blueshifts. The Baldwin effect between the C IV rest-frame equivalent width (REW) and the continuum luminosity at 1350 Å is not seen, likely due to the limited luminosity range of our sample. We find a lack of flux in the red wing of the composite spectrum with larger C IV blueshift and detect a higher ratio of [O III] quasars with REW_[O III]_ > 5 Å in the subsample with lower C IV blueshift. It is more likely that they are caused by the combination of the Eddington ratio and the orientation effect.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Black hole physics - Quasars

Simbad objects: 19

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Number of rows : 19
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 SDSS J011521.20+152453.3 QSO 01 15 21.2055079128 +15 24 53.379998460           ~ 18 0
2 QSO J0142+0023 QSO 01 42 14.7480666240 +00 23 24.293809176   19.30 18.70     ~ 53 0
3 QSO J0157-0106 QSO 01 57 41.5697767176 -01 06 29.648080260   19.40 18.71     ~ 49 0
4 QSO J0250-0757 QSO 02 50 21.7688505360 -07 57 49.964002668   19.02 18.63     ~ 38 0
5 LBQS 0256-0000 QSO 02 59 05.6356015320 +00 11 21.964472340   18.50 18.11     ~ 137 0
6 LBQS 0301-0035 QSO 03 03 41.0487601176 -00 23 21.907819248   18.26 17.93 17.6   ~ 121 0
7 LBQS 0302-0019 QSO 03 04 49.8593341368 -00 08 13.534398816   18.08 17.80 17.5   ~ 261 0
8 QSO J0753+4231 QSO 07 53 03.3374580696 +42 31 30.765827964   19.16 18.43     ~ 91 1
9 2MASS J08043064+5420406 QSO 08 04 30.5728111176 +54 20 41.117018820   19.61 18.81     ~ 35 0
10 [VV2006] J080819.7+373047 QSO 08 08 19.6944956640 +37 30 47.337865812   19.91 19.18     ~ 37 0
11 [VV2006] J080956.0+502001 QSO 08 09 56.0316646272 +50 20 00.929017896   19.25 18.69     ~ 36 0
12 SDSS J081855.78+095848.0 QSO 08 18 55.7827140888 +09 58 47.995294728   19.71 18.81     ~ 41 0
13 QSO B0900+42 QSO 09 00 33.5091652824 +42 15 47.031009948   17.63 17.18     ~ 85 0
14 QSO J0942+0422 QSO 09 42 02.0480819568 +04 22 44.548204368   17.78 17.47     ~ 66 0
15 2MASS J11595433+2019212 QSO 11 59 54.3311536560 +20 19 21.135293688   18.55 17.92     ~ 29 0
16 [VV2006] J173352.2+540030 QSO 17 33 52.2311709504 +54 00 30.514515120   18.07 17.60     ~ 61 0
17 [VV2006] J213023.6+122252 QSO 21 30 23.6213100504 +12 22 52.288727736   18.68 18.33     ~ 33 0
18 2MASS J22495608+0002182 QSO 22 49 56.0891963592 +00 02 18.159421020   19.17 18.75     ~ 29 0
19 KODIAQ J230301-093930 QSO 23 03 01.4579957256 -09 39 30.654165780   18.64 18.12     ~ 41 0

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