论文标题

HMXB CEN X-3的X射线变异性:不均匀增生流动的证据

X-ray variability of the HMXB Cen X-3: evidence for inhomogeneous accretion flows

论文作者

Sanjurjo-Ferrín, Graciela, Torrejón, Jose Miguel, Postnov, Konstantin, Oskinova, Lida, Rodes-Roca, Jose Joaquín, Bernabeu, Guillermo

论文摘要

CEN X-3是一种紧凑的高质量X射线二元,可能由Roche Lobe溢出提供动力。我们提出了两个尖的XMM-Newton观测值的相位分辨X射线光谱和定时分析。第一个发生在源的正常状态下,当它具有亮度$ l _ {\ rm x} \ sim 10^{36} $ erg s $^{ - 1} $时。该观察结果涵盖了轨道阶段$ ϕ = 0.00-0.37 $,即从日食出口。出口灯罩是高度结构化的,显示出独特的间隔。我们认为不同的间隔对应于不同发射结构的出现。 LightCurve分析使我们能够估算紧凑型星周围的这种结构的大小,其中最明显的是Roche Lobe Radius的顺序,其大小$ \ sim 0.3r _ {*} $。在出口期间,随着X射线连续体的增长,来自高度离子化物质的Fe发射线的等效宽度降低。另一方面,Fe K $α$线的等效宽度从接近中性的Fe加强。由于积聚流的X射线照明,这条线很可能形成。当源X射线更明亮并覆盖轨道阶段$ ϕ = 0.36-0.80 $时,进行了第二个观察结果。高状态下的X射线照明显示倾角。这些倾角不是由吸收引起的,而是由于积聚流中的不稳定性引起的。典型的倾角持续时间约为1000 〜s,比归因于大型供体恒星的易变恒星风的时间尺度要长得多,但与积聚磁盘内半径处的粘性时间尺度相似。

Cen X-3 is a compact high mass X-ray binary likely powered by Roche lobe overflow. We present a phase-resolved X-ray spectral and timing analysis of two pointed XMM-Newton observations. The first one took place during a normal state of the source, when it has a luminosity $L_{\rm X}\sim 10^{36}$ erg s$^{-1}$. This observation covered orbital phases $ϕ= 0.00-0.37$, i.e. the egress from the eclipse. The egress lightcurve is highly structured, showing distinctive intervals. We argue that different intervals correspond to the emergence of different emitting structures. The lightcurve analysis enables us to estimate the size of such structures around the compact star, the most conspicuous of which has a size $\sim 0.3R_{*}$, of the order of the Roche lobe radius. During the egress, the equivalent width of Fe emission lines, from highly ionized species, decreases as the X-ray continuum grows. On the other hand, the equivalent width of the Fe K$α$ line, from near neutral Fe, strengthens. This line is likely formed due to the X-ray illumination of the accretion stream. The second observation was taken when the source was 10 times X-ray brighter and covered the orbital phases $ϕ= 0.36-0.80$. The X-ray lightcurve in the high state shows dips. These dips are not caused by absorption but can be due to instabilities in the accretion stream. The typical dip duration, of about 1000~s, is much longer than the timescale attributed to the accretion of the clumpy stellar wind of the massive donor star, but is similar to the viscous timescale at the inner radius of the accretion disk.

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