Accretion disk models and their X-ray reflection signatures. I. Local spectra

被引:104
作者
Nayakshin, S [1 ]
Kallman, TR [1 ]
机构
[1] NASA, Goddard Space Flight Ctr, High Energy Phys Lab, Greenbelt, MD 20771 USA
关键词
accretion; accretion disks; line : formation; radiation mechanisms : nonthermal; radiative transfer; X-rays : general;
D O I
10.1086/318250
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
X-ray illumination of accretion disks is an invaluable diagnostic of the structure of these disks because of the associated iron K alpha emission. Here we point out that the resulting reflected spectra depend very sensitively on the geometry of the X-ray source and that this fact can be efficiently used to test these models observationally. In particular, we discuss three different accretion disk geometries : the "lamppost model," accretion disks with magnetic flares, and the model with a full corona overlaying a cold thin disk. We show that in the case of the lamppost model, unless the X-ray luminosity of the central source is larger than that of the cold disk by a factor of 10 or more, a significant fraction of iron in the ionized skin of the disk is in the hydrogen and helium-like ions. Because these ions have large fluorescence yields, the resulting reflected spectra look strongly ionized, with equivalent width (EW) of the line increasing with X-ray luminosity L-X up to the maximum of similar to 500 eV. This situation contrasts to the magnetic flare model, where the large X-ray flux near flares completely ionizes the skin of the disk and thus the resulting spectra appear to be that from a neutral material. The line EW in this model anti-correlates with X-ray luminosity and becomes arbitrarily small when L-X is a good fraction of the Eddington luminosity. Finally, in the full corona case, due to the additional pressure and weight of the corona, the gas pressure (and its density) below the corona is always large enough to make the gas very cool and effectively neutral. No highly ionized skin forms in such a model. If the corona is Thomson thin, then EW of the line does not depend on the accretion disk or corona luminosities for the full corona model.
引用
收藏
页码:406 / 418
页数:13
相关论文
共 59 条
[1]  
BASKO MM, 1974, ASTRON ASTROPHYS, V31, P249
[2]   EVAPORATIVE WINDS IN X-RAY BINARIES [J].
BASKO, MM ;
HATCHETT, S ;
MCCRAY, R ;
SUNYAEV, RA .
ASTROPHYSICAL JOURNAL, 1977, 215 (01) :276-284
[3]   COMPTON HEATED WINDS AND CORONAE ABOVE ACCRETION DISKS .1. DYNAMICS [J].
BEGELMAN, MC ;
MCKEE, CF ;
SHIELDS, GA .
ASTROPHYSICAL JOURNAL, 1983, 271 (01) :70-88
[4]   Polarization change due to fast winds from accretion disks [J].
Beloborodov, AM .
ASTROPHYSICAL JOURNAL, 1998, 496 (02) :L105-L108
[5]   Electron-positron outflows from gamma-ray emitting accretion discs [J].
Beloborodov, AM .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1999, 305 (01) :181-189
[6]   Concave accretion discs and X-ray reprocessing [J].
Blackman, EG .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1999, 306 (03) :L25-L30
[7]   ACCRETION FLOWS IN GALACTIC X-RAY SOURCES .1. OPTICALLY THIN SPHERICALLY SYMMETRIC MODEL [J].
BUFF, J ;
MCCRAY, R .
ASTROPHYSICAL JOURNAL, 1974, 189 (01) :147-155
[8]   WEAK SOFT-X-RAY EXCESSES NEED NOT RESULT FROM THE HIGH-FREQUENCY TAIL OF THE OPTICAL ULTRAVIOLET BUMP IN ACTIVE GALACTIC NUCLEI [J].
CZERNY, B ;
ZYCKI, PT .
ASTROPHYSICAL JOURNAL, 1994, 431 (01) :L5-L8
[9]   AN IONIZED ACCRETION DISK IN CYGNUS X-1 [J].
DONE, C ;
MULCHAEY, JS ;
MUSHOTZKY, RF ;
ARNAUD, KA .
ASTROPHYSICAL JOURNAL, 1992, 395 (01) :275-288
[10]   Observational signatures of X-ray-irradiated accretion disks [J].
Done, C ;
Nayakshin, S .
ASTROPHYSICAL JOURNAL, 2001, 546 (01) :419-428