2022MNRAS.515..491M


Query : 2022MNRAS.515..491M

2022MNRAS.515..491M - Mon. Not. R. Astron. Soc., 515, 491-506 (2022/September-1)

Systematically smaller single-epoch quasar black hole masses using a radius-luminosity relationship corrected for spectral bias.

MAITHIL J., BROTHERTON M.S., SHEMMER O., DU P., WANG J.-M., MYERS A.D., McLANE J.N., DIX C. and MATTHEWS B.M.

Abstract (from CDS):

Determining black hole masses and accretion rates with better accuracy and precision is crucial for understanding quasars as a population. These are fundamental physical properties that underpin models of active galactic nuclei. A primary technique to measure the black hole mass employs the reverberation mapping of low-redshift quasars, which is then extended via the radius-luminosity relationship for the broad-line region to estimate masses based on single-epoch spectra. An updated radius-luminosity relationship incorporates the flux ratio of optical Fe II to H β ($\equiv \mathcal {R}_{\rm Fe}$) to correct for a bias in which more highly accreting systems have smaller line-emitting regions than previously realized. In this work, we demonstrate and quantify the effect of using this Fe-corrected radius-luminosity relationship on mass estimation by employing archival data sets possessing rest-frame optical spectra over a wide range of redshifts. We find that failure to use an Fe-corrected radius predictor results in overestimated single-epoch black hole masses for the most highly accreting quasars. Their accretion rate measures (LBol/LEdd and $\dot{\mathscr{M}}$ ) are similarly underestimated. The strongest Fe-emitting quasars belong to two classes: high-z quasars with rest-frame optical spectra, which, given their extremely high luminosities, require high accretion rates, and their low-z analogues, which, given their low black holes masses, must have high accretion rates to meet survey flux limits. These classes have mass corrections downward of about a factor of two, on average. These results strengthen the association of the dominant Eigenvector 1 parameter $\mathcal {R}_{\rm Fe}$ with the accretion process.

Abstract Copyright: © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): galaxies: active - quasars: supermassive black holes

Simbad objects: 17

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Number of rows : 17
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 [VV2000] J040114.0-395132 QSO 04 01 14.0652420192 -39 51 32.682179196     17.00     ~ 16 0
2 QSO J0810+0936 QSO 08 10 11.9752125648 +09 36 48.261391164   19.74 19.15     ~ 13 0
3 US 1279 QSO 08 35 25.9788747456 +43 52 11.221368240   17.96 17.74     ~ 38 0
4 2MASS J09215364+0336525 Sy1 09 21 53.6394201864 +03 36 52.689432672   18.62 18.32     ~ 24 0
5 2MASSI J0935316+354101 Sy1 09 35 31.6122905856 +35 41 01.069495044   17.86 17.57     ~ 28 0
6 US 952 Sy1 09 47 04.5209282352 +47 21 42.905723688   18.48 18.16     ~ 64 0
7 2MASSI J0949277+314110 Sy1 09 49 27.6779121024 +31 41 09.962326932   17.09 16.63     ~ 28 1
8 2MASS J10443175+0708414 Sy1 10 44 31.7708539416 +07 08 41.048330964   17.73 17.57     ~ 27 0
9 [VV2000] J105528.8+312411 QSO 10 55 28.8008393520 +31 24 11.247287040   17.80 17.41     ~ 28 0
10 2MASS J13060187+5803200 Sy1 13 06 01.8667932024 +58 03 19.903339440   17.50 17.33     ~ 43 0
11 2MASS J13154947+0620478 QSO 13 15 49.4698194720 +06 20 47.885693460   16.8 17.58 16.7   ~ 15 0
12 LBQS 1313-0138 Sy1 13 16 09.7809609000 -01 54 03.878056872   18.24 18.11     ~ 32 0
13 2MASS J14032583+4430139 Sy1 14 03 25.8299114496 +44 30 14.114192400   18.81 18.64     ~ 24 0
14 SDSS J151036.74+510854.5 LM* 15 10 36.7448136552 +51 08 54.676291524   19.10 18.39     M0 18 0
15 [VV2000] J152350.4+391405 QSO 15 23 50.4253011504 +39 14 05.230614516   17.50 17.24     ~ 41 0
16 SDSS J224028.85-010649.9 Sy1 22 40 28.8594641352 -01 06 49.906688760   17.50 17.17     ~ 31 0
17 [VV2000] J235534.6-395355 QSO 23 55 34.5981536112 -39 53 55.263106284     16.30     ~ 17 0

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