Leaving the innermost stable circular orbit: the inner edge of a black-hole accretion disk at various luminosities

被引:72
作者
Abramowicz, M. A. [1 ,2 ,6 ]
Jaroszynski, M. [3 ]
Kato, S.
Lasota, J-P [4 ,5 ]
Rozanska, A. [2 ]
Sadowski, A. [2 ]
机构
[1] Gothenburg Univ, Dept Phys, S-41296 Gothenburg, Sweden
[2] Polish Acad Sci, N Copernicus Astron Ctr, PL-00716 Warsaw, Poland
[3] Univ Warsaw Observ, PL-00478 Warsaw, Poland
[4] UPMC Univ Paris 06, CNRS, Inst Astrophys Paris, UMR 7095, F-75014 Paris, France
[5] Jagiellonian Univ Observ, PL-30244 Krakow, Poland
[6] Silesian Univ Opava, Fac Philosophy & Sci, Inst Phys, Opava 74601, Czech Republic
关键词
black hole physics; accretion; accretion disks; ADVECTION-DOMINATED ACCRETION; POWER SPECTRA; STRESS; SPIN; FLOW; SIMULATIONS; VARIABILITY; RADIATION; THICKNESS; EMISSION;
D O I
10.1051/0004-6361/201014467
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The "radiation inner edge" of an accretion disk is defined as the inner boundary of the region from which most of the luminosity emerges. Similarly, the "reflection edge" is the smallest radius capable of producing a significant X-ray reflection of the fluorescent iron line. For black hole accretion disks with very sub-Eddington luminosities these and all other "inner edges" coexist at the innermost stable circular orbit (ISCO). Thus, in this case, one may rightly consider ISCO as the unique inner edge of the black hole accretion disk. However, even at moderate luminosities, there is no such unique inner edge because differently defined edges are located at different places. Several of them are significantly closer to the black hole than ISCO. These differences grow with the increasing luminosity. For nearly Eddington luminosities, they are so huge that the notion of the inner edge loses all practical significance.
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页数:12
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