2022MNRAS.513.4361M


Query : 2022MNRAS.513.4361M

2022MNRAS.513.4361M - Mon. Not. R. Astron. Soc., 513, 4361-4379 (2022/July-1)

High-density disc reflection spectroscopy of low-mass active galactic nuclei.

MALLICK L., FABIAN A.C., GARCIA J.A., TOMSICK J.A., PARKER M.L., DAUSER T., WILKINS D.R., DE MARCO B., STEINER J.F., CONNORS R.M.T., MASTROSERIO G., MARKOWITZ A.G., PINTO C., ALSTON W.N., LOHFINK A.M. and GANDHI P.

Abstract (from CDS):

The standard alpha-disc model predicts an anticorrelation between the density of the inner accretion disc and the black hole mass times square of the accretion rate, as seen in higher mass (MBH > 106 M☉) active galactic nuclei (AGNs). In this work, we test the predictions of the alpha-disc model and study the properties of the inner accretion flow for the low-mass end (MBH ≃ 105–6 M☉) of AGNs. We utilize a new high-density disc reflection model where the density parameter varies from ne = 1015 to 1020 cm–3 and apply it to the broad-band X-ray (0.3-10 keV) spectra of the low-mass AGN sample. The sources span a wide range of Eddington fractions and are consistent with being sub-Eddington or near-Eddington. The X-ray spectra reveal a soft X-ray excess below ∼1.5 keV which is well modelled by high-density reflection from an ionized accretion disc of density ne ∼ 1018 cm–3 on average. The results suggest a radiation pressure-dominated disc with an average of 70 per cent fraction of the disc power transferred to the corona, consistent with that observed in higher mass AGNs. We show that the disc density higher than 1015 cm–3 can result from the radiation pressure compression when the disc surface does not hold a strong magnetic pressure gradient. We find tentative evidence for a drop in black hole spin at low-mass regimes.

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

Journal keyword(s): accretion, accretion discs - black hole physics - relativistic processes - galaxies: active - galaxies: nuclei - X-rays: galaxies

Simbad objects: 16

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Number of rows : 16
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 2MASS J01071195+1408449 Sy1 01 07 12.0268679880 +14 08 44.981850408   19.30 18.83     ~ 53 0
2 SDSS J022849.51-090153.8 Sy1 02 28 49.5160665072 -09 01 53.804543988   18.37 17.88     ~ 24 0
3 MCG-02-07-024 Sy1 02 30 05.5225590096 -08 59 53.207139372   14.74 14.29 13.981 13.585 ~ 332 0
4 MCG-05-13-017 Sy2 05 19 35.8118941104 -32 39 27.923120568   13.81 13.37 12.73   ~ 274 1
5 2MASS J09405720+0324012 Sy1 09 40 57.1978090608 +03 24 01.259433720   18.44 17.86     ~ 36 0
6 2MASX J10234843+0405536 Sy1 10 23 48.4350539699 +04 05 53.905121235   17.30 16.70     ~ 21 0
7 2MASX J11400874+0307114 Sy1 11 40 08.7172457952 +03 07 11.399104884   19.03 18.48     ~ 60 1
8 POX 52 Sy2 12 02 56.93256 -20 56 02.9580           ~ 178 0
9 2MASS J13473822+4743021 Sy1 13 47 38.2359565560 +47 43 01.977094632   16.89 16.47     ~ 22 0
10 2MASS J13572448+6525057 Sy1 13 57 24.5204418120 +65 25 05.952508176   18.91 18.58     ~ 49 0
11 Z 47-107 Sy1 14 34 50.6282462496 +03 38 42.520770600   15.84 15.28     ~ 61 0
12 2MASX J15415087+3100368 Sy1 15 41 50.8573995816 +31 00 37.323477720   16.36 15.85     ~ 17 0
13 Z 195-3 Sy1 15 59 09.6231720696 +35 01 47.561352852   15.69 15.06     ~ 346 0
14 Z 196-64 Sy1 16 26 36.4008193656 +35 02 42.072346392   15.83 15.42     ~ 46 0
15 2MASS J16315959+2437403 Sy1 16 31 59.5942119768 +24 37 40.240873740   18.61 17.92     ~ 29 0
16 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0

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