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arXiv 2304.02422astro-ph.HE
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天鹅座 X-3 的 RXTE/ASM 光变曲线背后的秘密

Secrets behind the RXTE/ASM light curve of Cyg X-3

Osmi Vilhu, Karri Koljonen, Diana Hannikainen

AI总结:

本文提出启发式反馈模型,将天鹅座 X-3 中 EUV 辐照对 Wolf-Rayet 伴星星风的抑制与 X 射线源耦合,解释其 RXTE/ASM 不规则光变可由小幅吸积变化经正/负反馈放大形成。

摘要:

在星风供食的 X 射线双星中,主星由辐射驱动的星风会因致密次星的极紫外(EUV)辐照而受到抑制,从而导致吸积率升高。这会在释放的吸积功率与致密星光度之间产生反馈。我们研究了独特的大质量 X 射线双星天鹅座 X-3(Cygnus X-3)中释放的吸积功率与致密星 X 射线光度之间的反馈过程。我们假设一部分星风供食功率围绕源光度发生小幅度变化。我们提出了一个简单的启发式模型,将 EUV 辐照对(来自 Wolf-Rayet 伴星的)恒星星风的影响与 X 射线源本身耦合起来。所得光度时间轮廓模拟了输入变化的轮廓,但振幅更大。输入变化最重要的特征是其改变符号并开始产生正反馈或负反馈时的转折时间。由光谱建模得到的热辐射光度是所得反馈光度的时间平均值。我们证明,天鹅座 X-3 的 X 射线光变曲线的不规则行为可能源于 X 射线源的小幅度变化及其与伴星星风的反馈。这种变化可能产生于吸积流,和/或由喷流或吸积盘星风中的动能损失造成。为了使模拟光变曲线具有与观测相似的性质,我们必须将最大吸积半径限制在一个变化的水平,并假设光变曲线上升和下降阶段具有可变的时间尺度。

英文摘要:

In wind-fed X-ray binaries, the radiatively driven wind of the primary star can be suppressed by the EUV irradiation of the compact secondary star, leading to an increased accretion rate. This causes feedback between the released accretion power and the luminosity of the compact star. We investigate the feedback process between the released accretion power and the X-ray luminosity of the compact star in the unique high-mass X-ray binary Cygnus X-3. We assume that a part of the wind-fed power experiences a small amplitude variability around the source luminosity. We propose a simple heuristic model to couple the influence of EUV irradiation on the stellar wind (from the Wolf-Rayet companion star) with the X-ray source itself. The resulting time profile of luminosity mimics that of the input variability, albeit with a larger amplitude. The most important property of the input variability are turnover times when it changes its sign and starts to have either positive or negative feedback. The bolometric luminosity derived by spectral modeling is the time average of the resulting feedback luminosity. We demonstrate that the erratic behavior of the X-ray light curve of Cygnus X-3 may have its origin in the small amplitude variability of the X-ray source and feedback with the companion wind. This variability could arise in the accretion flow and/or due to the loss of kinetic energy in a jet or an accretion disk wind. In order to produce similar properties of the simulated light curve as observed, we have to restrict the largest accretion radius to a changing level, and assume variable timescales for the rise and decline phases of the light curve.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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