X-ray variability of SS 433: effects of the supercritical accretion disc

被引:9
|
作者
Atapin, Kirill [1 ]
Fabrika, Sergei [2 ,3 ]
Medvedev, Aleksei [2 ,4 ]
Vinokurov, Alexander [2 ]
机构
[1] Moscow MV Lomonosov State Univ, Sternberg Astron Inst, Moscow 119991, Russia
[2] Special Astrophys Observ, Nizhnii Arkhyz 369167, Russia
[3] Kazan Fed Univ, Kazan 420008, Russia
[4] St Petersburg State Univ, Fac Math & Mech, St Petersburg 198504, Russia
基金
俄罗斯基础研究基金会;
关键词
accretion; accretion discs; stars: individual: SS 433; X-rays: binaries; BLACK-HOLES; OPTICAL VARIABILITY; SS433; SS-433; JETS; RADIATION; DIAGNOSTICS; PARAMETERS; SPECTRUM; FLOWS;
D O I
10.1093/mnras/stu2134
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study a stochastic variability of SS 433 in the 10(-4)-5 x 10(-2) Hz frequency range based on RXTE data, and on simultaneous observations with RXTE and optical telescopes. We find that the cross-correlation functions and power spectra depend drastically on the precession phase of the supercritical accretion disc. When the wind funnel of the disc is maximally open to the observer, a flat part emerges in the power spectrum; a break is observed at the frequency 1.7 x 10(-3) Hz, with a power-law index beta approximate to 1.67 at higher frequencies. The soft emission forming mostly in the jets lags behind the hard and optical emission. When the observer does not see the funnel and jets (the 'edge-on' disc), the power spectrum is described by a single power-law with beta approximate to 1.34 and no correlations between X-ray ranges are detected. We investigated two mechanisms to explain the observed variability at the open disc phase: (1) reflection of radiation at the funnel wall (X-rays and optical) and (2) the gas cooling in the jets (X-rays only). The X-ray variability is determined by the contribution of both mechanisms; however, the contribution of the jets is much higher. We found that the funnel size is (2-2.5) x 10(12) cm, and the opening angle is v(f) similar to 50 degrees. X-ray jets may consist of three fractions with different densities: 8 x 10(13), 3 x 10(13) and 5 x 10(11) cm(-3), with most of the jet's mass falling within the latter fraction. We suppose that revealed flat part in the power spectrum may be related to an abrupt change in the disc structure and viscous time-scale at the spherization radius, because the accretion disc becomes thick at this radius, h/r similar to 1. The extent of the flat spectrum depends on the variation of viscosity at the spherization radius.
引用
收藏
页码:893 / 910
页数:18
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