2007ApJ...668.1145Q


Query : 2007ApJ...668.1145Q

2007ApJ...668.1145Q - Astrophys. J., 668, 1145-1153 (2007/October-3)

Disk evaporation-fed corona: structure and evaporation features with magnetic field.

QIAN L., LIU B.F. and WU X.-B.

Abstract (from CDS):

The disk-corona evaporation model naturally accounts for many observational phenomena in black hole X-ray binaries, such as the truncation of an accretion disk and the spectral state transitions. On the other hand, magnetic fields are known to play an important role in transporting angular momentum and producing viscosity in accretion flows. In this work, we explicitly take the magnetic field in the accretion disk corona into consideration and numerically calculate the coronal structure on the basis of our two-temperature evaporation code. We show that the magnetic field influences the coronal structure through its contribution to the pressure, energy, and radiative cooling in the corona and by decreasing the vertical heat conduction. We find that the maximum evaporation rate stays more or less constant (∼3% of the Eddington rate) when the strength of the magnetic field changes, but that the radius corresponding to the maximum evaporation rate decreases with increasing magnetic field. This suggests that spectral state transitions always occur at a few percent of the Eddington accretion rate, while the inner edge of the thin disk can be at ∼100RS or even less in the hard state before the transition to the soft state. These results alleviate the problem of previous evaporation models' predicting too large a truncation radius and are in better agreement with the observational results for several black hole X-ray binaries, although discrepancies remain.

Abstract Copyright: ∼

Journal keyword(s): Accretion, Accretion Disks - Black Hole Physics - Conduction - Magnetic Fields - X-Rays: Binaries

Simbad objects: 11

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Number of rows : 11
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 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 722 0
2 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
3 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 734 1
4 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
5 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
6 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
7 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
8 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
9 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
10 V* QZ Vul HXB 20 02 49.5220407111 +25 14 10.631666444           K3V-K6V 432 0
11 INTREF 1012 LXB 20 12 37.7592785736 +38 11 00.770922096     21.33     ~ 78 0

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