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arXiv 1905.01262astro-ph.HE
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天鹅座X-1系统III中聚焦风的钱德拉X射线光谱学。在低/硬状态下浸渍

Chandra X-ray spectroscopy of the focused wind in the Cygnus X-1 system III. Dipping in the low/hard state

Maria Hirsch, Natalie Hell, Victoria Grinberg, Ralf Ballhausen, Michael A. Nowak, Katja Pottschmidt, Norbert S. Schulz, Thomas Dauser, Manfred Hanke, Timothy R.… 展开作者

Maria Hirsch, Natalie Hell, Victoria Grinberg, Ralf Ballhausen, Michael A. Nowak, Katja Pottschmidt, Norbert S. Schulz, Thomas Dauser, Manfred Hanke, Timothy R. Kallman, Gregory V. Brown, Jörn Wilms

摘要:

利用钱德拉高能透射光栅对天鹅座黑洞双星Cyg X-1/HDE 226868进行了三次不同轨道相位的观测。在这个系统中,为吸积提供动力的恒星风的特征是温度和密度的不均匀性,包括嵌入光电离气体中的更冷、更致密的物质的结构或“团块”。当这些团块通过我们的视线时,光变曲线上出现吸收下降。我们通过光谱的变化,在各个浸渍阶段的团块的特性。在四个不同柱深度的水平中比较硅和硫吸收线区域(1.6-2.7 keV $\equiv$ 7.7-4.6 keV)揭示了较低电离级的存在,即,更冷或更致密的材料,在更深的浸渍阶段。线的多普勒速度在每次观测中大致一致,随各自的轨道相位而变化。这与由不同的电离物质组成的结构的图像是一致的,其中面向黑洞的物质壳层屏蔽了电离辐射的内壳和后壳。然而,与星风的玩具模型相比,多普勒速度的变化并不能让我们确定系统中团块区域的确切位置。这一结果,以及观察到的线的不对称形状,指向一个复杂的风结构的图片。

英文摘要:

We present an analysis of three Chandra High Energy Transmission Gratings observations of the black hole binary Cyg X-1/HDE 226868 at different orbital phases. The stellar wind that is powering the accretion in this system is characterized by temperature and density inhomogeneities including structures, or "clumps", of colder, more dense material embedded in the photoionized gas. As these clumps pass our line of sight, absorption dips appear in the light curve. We characterize the properties of the clumps through spectral changes during various dip stages. Comparing the silicon and sulfur absorption line regions (1.6-2.7 keV $\equiv$ 7.7-4.6 Å) in four levels of varying column depth reveals the presence of lower ionization stages, i.e., colder or denser material, in the deeper dip phases. The Doppler velocities of the lines are roughly consistent within each observation, varying with the respective orbital phase. This is consistent with the picture of a structure that consists of differently ionized material, in which shells of material facing the black hole shield the inner and back shells from the ionizing radiation. The variation of the Doppler velocities compared to a toy model of the stellar wind, however, does not allow us to pin down an exact location of the clump region in the system. This result, as well as the asymmetric shape of the observed lines, point at a picture of a complex wind structure.

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