2019ApJ...876..102H


Query : 2019ApJ...876..102H

2019ApJ...876..102H - Astrophys. J., 876, 102-102 (2019/May-2)

Reverberation mapping of the narrow-line Seyfert 1 galaxy I Zwicky 1: black hole mass.

HUANG Y.-K., HU C., ZHAO Y.-L., ZHANG Z.-X., LU K.-X., WANG K., ZHANG Y., DU P., LI Y.-R., BAI J.-M., HO L.C., BIAN W.-H., YUAN Y.-F. and WANG J.-M.

Abstract (from CDS):

We report results of the first reverberation mapping campaign of I Zwicky 1 during 2014-2016, which showed unambiguous reverberations of the broad Hβ line emission in the varying optical continuum. From analysis using several methods, we obtain a reverberation lag of τHβ=37.2–4.9+4.5days. Taking a virial factor of fBLR_=1, we find a black hole mass of M•=9.30–1.38+1.26×106M☉ from the mean spectra. The accretion rate is estimated to be 203.9–65.8+61.0LEddc–2, suggesting a super-Eddington accretor, where LEdd is the Eddington luminosity and c is the speed of light. By decomposing Hubble Space Telescope images, we find that the stellar mass of the bulge of its host galaxy is log(Mbulge/M☉)=10.92±0.07. This leads to a black hole to bulge mass ratio of ∼10–4, which is significantly smaller than that of classical bulges and elliptical galaxies. After subtracting the host contamination from the observed luminosity, we find that I Zw 1 follows the empirical RBLR∝L51001/2 relation.

Abstract Copyright: © 2019. The American Astronomical Society.

Journal keyword(s): galaxies: active - galaxies: individual: I Zw 1 - galaxies: nuclei

VizieR on-line data: <Available at CDS (J/ApJ/876/102): table1.dat>

Simbad objects: 4

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Number of rows : 4
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 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
2 Mrk 142 Sy1 10 25 31.2786898344 +51 40 34.867889004   16.33 16.12     ~ 330 0
3 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
4 Z 195-3 Sy1 15 59 09.6231720696 +35 01 47.561352852   15.69 15.06     ~ 346 0

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