论文标题

恒星风在CYG X-1的硬状态下的X射线光谱定时贡献

The X-ray spectral-timing contribution of the stellar wind in the hard state of Cyg X-1

论文作者

Lai, E. V., De Marco, B., Zdziarski, A. A., Belloni, T. M., Mondal, S., Uttley, P., Grinberg, V., Wilms, J., Różańska, A.

论文摘要

来自高质量X射线二进制的伴侣恒星的块状恒星风会导致可变,部分吸收X射线源的发射。我们从7.22 d-d-long的“ Cyg X-1 X-1硬状态观察”(Chocbox)监测活动中研究了XMM-Newton的观察,以限制源头秀中的恒星风对来源的X射线X射线频谱的影响。我们发现这些特性在风的存在下会发生显着变化。特别是,最长的采样时间尺度(对应于$ν\ sim $ 0.1-1 Hz的时间频率)揭示了分数可变性功率的增强,而在最短的采样时间表($ν\ sim $ 1-10 Hz)中,可变性抑制了可变性。此外,我们观察到软带和硬带光曲线之间原本高相干性以及硬X射线固定在X射线连续体固有的幅度的降低(高达$ \ sim $ 1.8)。观察到的低频可变性功率的增加可以通过风柱密度的变化来解释,这是由于中间团块的运动的结果。在这种情况下(并假设$ v _ {\ infty} = 2400 \ {\ rm km \ s^{ - 1}} $)的终端速度,我们获得了$ l \ sim $ 0.5-1.5 $ \ times 10^{ - 4} r _ 4} r _ {r _ {r a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a a} $平均平均平均水平。另一方面,我们建议以高频的行为是由于在光学较厚的介质中散射,这可能是由于恒星风与盘边缘的碰撞而形成的。

The clumpy stellar wind from the companion star in high mass X-ray binaries causes variable, partial absorption of the emission from the X-ray source. We studied XMM-Newton observations from the 7.22 d-long "Cyg X-1 Hard state Observations of a Complete Binary Orbit in X-rays" (CHOCBOX) monitoring campaign, in order to constrain the effects of the stellar wind on the short-timescale X-ray spectral-timing properties of the source. We find these properties to change significantly in the presence of the wind. In particular, the longest sampled timescales (corresponding to temporal frequencies of $ν\sim$ 0.1-1 Hz) reveal an enhancement of the fractional variability power, while on the shortest sampled timescales ($ν\sim$ 1-10 Hz) the variability is suppressed. In addition, we observe a reduction (by up to a factor of $\sim$ 1.8) of the otherwise high coherence between soft and hard band light curves, as well as of the amplitude of the hard X-ray lags intrinsic to the X-ray continuum. The observed increase of low frequency variability power can be explained in terms of variations of the wind column density as a consequence of motions of the intervening clumps. In this scenario (and assuming a terminal velocity of $v_{\infty}=2400\ {\rm km\ s^{-1}}$), we obtain an estimate of $l \sim$ 0.5-1.5 $\times 10^{-4} R_{\ast}$ for the average radial size of a clump. On the other hand, we suggest the behaviour at high frequencies to be due to scattering in an optically thicker medium, possibly formed by collision of the stellar wind with the edge of the disc.

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