2011MNRAS.414.2186J


Query : 2011MNRAS.414.2186J

2011MNRAS.414.2186J - Mon. Not. R. Astron. Soc., 414, 2186-2194 (2011/July-1)

On different types of instabilities in black hole accretion discs: implications for X-ray binaries and active galactic nuclei.

JANIUK A. and CZERNY B.

Abstract (from CDS):

We discuss two important instability mechanisms that may lead to the limit-cycle oscillations of the luminosity of the accretion discs around compact objects: ionization instability and radiation pressure instability. Ionization instability is well established as a mechanism of X-ray novae eruptions in black hole binary systems, but its applicability to active galactic nuclei (AGN) is still problematic. Radiation pressure theory has still a very weak observational background in any of these sources. In this paper, we attempt to confront the parameter space of these instabilities with the observational data. At the basis of this simple survey of sources properties, we argue that the radiation pressure instability is likely to be present in several Galactic sources with the Eddington ratios being above 0.15 and in AGN with the Eddington ratio above 0.025. Our results favour the parametrization of the viscosity through the geometrical mean of the radiation and gas pressure in both Galactic sources and AGN. More examples of the quasi-regular outbursts in the time-scales of 100 s in Galactic sources and hundreds of years in AGN are needed to formulate firm conclusions. We also show that the disc sizes in the X-ray novae are consistent with the ionization instability. This instability may also considerably influence the lifetime cycle and overall complexity in the supermassive black hole environment.

Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): galaxies: active - galaxies: evolution - X-rays: binaries

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 CXOM31 J004253.1+411422 ULX 00 42 53.15 +41 14 22.9           ~ 27 0
2 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184 13.00 13.50 13.2     M4.5V 651 1
3 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544 10.60 11.40 11.2     K3V-K7V 1113 0
4 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 715 1
5 NGC 4395 Sy2 12 25 48.8633109888 +33 32 48.700168152 10.84 10.54 10.11 9.98   ~ 1177 1
6 V* BW Cir HXB 13 58 09.700 -64 44 05.80 17.90 18.00 16.9     ~ 238 1
7 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760     11.96     ~ 494 1
8 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000   17.95 16.6     K3III 1173 0
9 X Nor X-1 LXB 16 34 01.610 -47 23 34.80           ~ 517 0
10 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60     11.89     K4V 398 0
11 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1887 1
12 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 251 0
13 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2079 0
14 AX J1733.9-3112 LXB 17 33 32.00 -31 13 00.0           ~ 52 0
15 3FHL J1746.2-2852 LXB 17 44 33.09 -28 44 27.0           ~ 532 0
16 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 745 0
17 2MAXI J1753-013 LXB 17 53 28.2898766424 -01 27 06.256555272 15.30 16.73 16.46 16.15 15.64 ~ 364 0
18 XTE J1818-245 LXB 18 18 24.430 -24 32 17.96           ~ 37 0
19 V* V344 Lyr CV* 18 44 39.1748179896 +43 22 28.051269960           sdB 104 0
20 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2628 0
21 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4337 0
22 V* QZ Vul HXB 20 02 49.58 +25 14 11.3   19.64 18.2     K3V-K6V 421 0
23 V* V404 Cyg HXB 20 24 03.8254458776 +33 52 01.962185735           G9/K0III/V 1277 0

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