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Emission lines and shock waves in RR Lyrae stars

机译:RR天琴星的发射线和冲击波

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Context. Emission lines observed in radially pulsating stars are thought to be produced by atoms de-exciting after being excited by a shock wave that is traveling into and then compressing, heating, and accelerating the atmospheric gas. Aims. With the help of recent observations, we examine the origin of all the different types of emission lines of hydrogen and helium that appear during a pulsation cycle. Methods. To analyze the physical origin of emission lines, we used the different models of atmospheric dynamics of RR Lyrae stars that have been calculated so far. Results. In contrast to a recent explanation, we propose that the redshifted emission component of Hα, which occurs near the pulsation phase 0.3, is produced by the main shock. In this case, the emission is the natural consequence of the large extension of the expanding atmosphere. Therefore, this (weak) emission should only be observed in RR Lyrae stars for which the main shock will propagate far enough from the photosphere. It appears as a P-Cygni type profile. We estimate the shock front velocity during the shock propagation in the atmosphere and show that it decreases by 40% when the Hα?emitting-shock passes from the photospheric level to the upper atmosphere. The Hα?P-Cygni profile observed in long-period Cepheids also seems to be caused by the main shock wave. Although to date He?II has only been detected in some Blazhko stars, a comprehensive survey of RR Lyrae stars is necessary to confirm this trend, so we can say that the most intense shocks will only be observed in Blazhko stars. Conclusions. The development of a model of atmospheric pulsation that takes the effects of 2D and 3D convection into account, seems to be a necessary step to fully quantify the effects of shock waves on the atmospheric dynamics of radially pulsating stars.
机译:上下文。人们认为,在径向脉动星中观察到的发射线是原子被激波激发后去激励而产生的,激波进入并压缩,加热并加速了大气中的气体。目的借助最近的观察,我们检查了在脉动周期中出现的所有不同类型的氢和氦发射线的起源。方法。为了分析发射线的物理起源,我们使用了迄今已计算的RR天琴星大气动力学的不同模型。结果。与最近的解释相反,我们认为Hα的红移发射分量发生在脉动相位0.3附近,是由主冲击产生的。在这种情况下,排放是膨胀空气大范围扩展的自然结果。因此,仅在RR天琴座的恒星中会观察到这种(微弱)发射,因为这些恒星的主激波将传播到距光球足够远的地方。它显示为P-Cygni类型配置文件。我们估计了在大气中的冲击传播过程中的冲击前速度,并表明当Hα发射激波从光球层到达高层大气时,它降低了40%。在长周期造父变星中观察到的HαP-Cygni轮廓似乎也是由主冲击波引起的。尽管迄今为止仅在布拉科科的一些恒星中发现了HeII,但是有必要对RR天琴星进行全面的调查以确认这种趋势,因此可以说,只有布拉科科的恒星会受到最强烈的冲击。结论。考虑到2D和3D对流的影响,建立大气脉动模型似乎是充分量化冲击波对径向脉动星的大气动力学影响的必要步骤。

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