WZ - Sge恒星的静态光曲线性质

黄金时代 Pub Date : 2016-07-01 DOI:10.22323/1.315.0031
D. Kononov, C. Lacy, V. Puzin, V. P. Kozhevnikov, A. Sytov, A. P. Lyaptsev
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引用次数: 0

摘要

本文报道了对WZ Sge亚类变星(cv) V455仙女座变星(V455 Andromedae)的静态光谱和光度观测结果。利用光谱数据,我们计算了系统的时间分辨多普勒断层图,展示了它在不同轨道相位的行为。在层析图中,我们可以看到在一个轨道周期内不同区域的周期性变亮。我们将这种变亮解释为由于盘内的四个锁相激波与盘内形成的特定内部进动密度波的相互作用,由于次级恒星的潮汐影响,这种密度波向上传播到盘的外部区域。当密度波的外层在其岁差运动中到达激波时,局部密度增加,从而放大激波(通过增加$\rho V^{2}/2$)。这导致在冲击中额外的能量释放,可以观察到增亮。层析成像结果和光度数据的分析表明,两个主要来源对系统的光曲线有贡献:“热线”和弓形激波的辐射给了我们两个主要的轨道峰,大约位于轨道相位$\phi=0.25$和$\phi=0.75$;四个激波的放大可能给我们带来在光曲线上随岁差周期移动的四个“超级峰”。当这两种效应重叠时,会改变光曲线的形状,移动峰的最大值,有时会在光曲线中产生两个以上的峰。我们应该强调的是,当我们说“超级驼峰”时,我们指的是在WZ Sge恒星的静止光曲线中观察到的一种效应,而不是通常在爆发中观察到的“经典”超级驼峰。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the nature of quiescent light curves demonstrated by WZ Sge stars
We present the results of simultaneous spectroscopic and photometric observations of the cataclysmic variable star (hereafter CVs) V455 Andromedae, belonging to the WZ Sge sub-class, in quiescence. Using the spectroscopic data we computed time-resolved Doppler tomograms of the system demonstrating its behavior at different orbital phases. In the tomograms one can see the periodic brightening of different regions within one orbital cycle. We interpret this brightening as being due to the interaction of four phase-locked shock waves in the disk with a specific internal precessing density wave that develops inside the disk, because of the tidal influence of the secondary star, and this density wave propagates up to the disk's outer regions. When the outer part of the density wave in its precessional motion reaches a shock wave the local density grows, which amplifies the shock (by increasing $\rho V^{2}/2$). This results in an additional energy release in the shock and can be observed as a brightening. Analysis of the tomographic results and the photometric data shows that two main sources contribute to the light curves of the system: the radiation of the "hot line" and the bow-shock gives us two major orbital humps, located approximately at the orbital phases $\phi=0.25$ and $\phi=0.75$; the amplification of the four shock waves may give us up to four "superhumps" shifting over the light curve with the precessional period. These two effects, when overlapping, change the shape of the light curves, shift the hump maxima, and they sometimes produce more than two humps in the light curve. We should emphasize that when saying "superhumps" we imply an effect that is observed in quiescent light curves of WZ Sge stars, as opposed to "classical" superhumps usually observed in outbursts.
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