The Sloan Digital Sky Survey Reverberation Mapping Project: The Black Hole Mass−-Stellar Mass Relations at 0.2≲z≲0.80.2\lesssim z\lesssim 0.8

preprint2023arXivOpen access

Abstract

We measure the correlation between black-hole mass MBHM_{\rm BH} and host stellar mass M∗M_* for a sample of 38 broad-line quasars at 0.2≲z≲0.80.2\lesssim z\lesssim 0.8 (median redshift zmed=0.5z_{\rm med}=0.5). The black-hole masses are derived from a dedicated reverberation mapping program for distant quasars, and the stellar masses are estimated from two-band optical+IR HST imaging. Most of these quasars are well centered within ≲1\lesssim 1kpc from the host galaxy centroid, with only a few cases in merging/disturbed systems showing larger spatial offsets. Our sample spans two orders of magnitude in stellar mass (∼109−1011 M⊙\sim 10^9-10^{11}\,M_\odot) and black-hole mass (∼107−109 M⊙\sim 10^7-10^9\,M_\odot), and reveals a significant correlation between the two quantities. We find a best-fit intrinsic (i.e., selection effects corrected) MBH−M∗,hostM_{\rm BH}-M_{\rm *,host} relation of log⁡(MBH/M⊙)=7.01−0.33+0.23+1.74−0.64+0.64log⁡(M∗,host/1010M⊙)\log (M_{\rm BH}/M_{\rm \odot})=7.01_{-0.33}^{+0.23} + 1.74_{-0.64}^{+0.64}\log (M_{\rm *,host}/10^{10}M_{\rm \odot}), with an intrinsic scatter of 0.47−0.17+0.240.47_{-0.17}^{+0.24}dex. Decomposing our quasar hosts into bulges and disks, there is a similar MBH−M∗,bulgeM_{\rm BH}-M_{\rm *,bulge} relation with a slightly larger scatter, likely caused by systematic uncertainties in the bulge-disk decomposition. The MBH−M∗,hostM_{\rm BH}-M_{\rm *,host} relation at zmed=0.5z_{\rm med}=0.5 is similar to that in local quiescent galaxies, with negligible evolution over the redshift range probed by our sample. With direct black-hole masses from reverberation mapping and a large dynamical range of the sample, selection biases do not appear to affect our conclusions significantly. Our results, along with other samples in the literature, suggest that the locally-measured black-hole mass−-host stellar mass relation is already in place at z∼1z\sim 1.

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