Broadband spectrum of Cygnus X-1 in two spectral states with BeppoSAX

被引:104
作者
Frontera, F
Palazzi, E
Zdziarski, AA
Haardt, F
Perola, GC
Chiapetti, L
Cusumano, G
Dal Fiume, D
Del Sordo, S
Orlandini, M
Parmar, AN
Piro, L
Santangelo, A
Segreto, A
Treves, A
Trifoglio, M
机构
[1] Univ Ferrara, Dipartmento Fis, I-44100 Ferrara, Italy
[2] CNR, Ist Tecnol & Studio Radiaz Extraterr, I-40129 Bologna, Italy
[3] Univ Insubria, I-22100 Como, Italy
[4] N Copernicus Astron Ctr, PL-00716 Warsaw, Poland
[5] Univ Roma Tre, Dipartimento Fis E Amaldi, I-00146 Rome, Italy
[6] CNR, Ist Fis Cosm G Occhialini, I-20133 Milan, Italy
[7] CNR, Ist Fis Cosm & Applicaz Informat, I-90146 Palermo, Italy
[8] European Space Agcy, Dept Space Sci, Div Astrophys, NL-2200 AG Noordwijk, Netherlands
[9] CNR, Ist Astrofis Spaziale, I-00133 Rome, Italy
关键词
accretion; accretion disks; binaries : general; black hole physics; stars : individual (Cygnus X-1); X-rays : stars;
D O I
10.1086/318304
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We report on the 0.5-200 keV spectral properties of Cyg X-1 observed at different epochs with the Narrow Field Instruments of the BeppoSAX satellite. The source was in its soft state during the first observation of 1996 June. In the second observation of 1996 September, the source had parameters characteristic to its hard state. A soft X-ray excess, a broad Fe K alpha line and Compton reflection are clearly detected in both states. The soft-state broadband continuum is well modeled by a disk blackbody (accounting for the soft excess) and Compton upscattering of the disk photons by a hybrid, thermal/nonthermal plasma, probably forming a corona above the disk (also giving rise to the Compton-reflection component). In the hard state, the primary hard X-ray spectrum can be well modeled by Compton upscattering of a weak blackbody emission by a thermal plasma at a temperature of similar to 60 keV. The soft excess is then explained by thermal Comptonization of the same blackbody emission by another hot plasma cloud characterized by a low value of its Compton parameter. Finally, we find the characteristic ratio of the bolometric flux in the soft state to that in the hard state to be about 3. This value is much more compatible with theories of state transitions than the previously reported (and likely underestimated) value of 1.5.
引用
收藏
页码:1027 / 1037
页数:11
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