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首页> 外文期刊>Astronomy and astrophysics >Variable X-ray emission from the accretion shock in the classical T Tauri star V2129?Ophiuchi
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Variable X-ray emission from the accretion shock in the classical T Tauri star V2129?Ophiuchi

机译:经典T Tauri星V2129?Ophiuchi吸积激荡产生的可变X射线发射

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Context. The soft X-ray emission from high density plasma observed in several CTTS is usually associated with the accretion process. However, it?is still unclear whether this high density “cool” plasma is heated in the accretion shock, or?if it is coronal plasma fed or modified by the accretion process. Aims. We conducted a coordinated quasi-simultaneous optical and X-ray observing campaign of the CTTS V2129?Oph. In this paper, we analyze Chandra grating spectrometer data and attempt to correlate the observed X-ray emitting plasma components with the characteristics of the accretion process and the stellar magnetic field constrained by simultaneous optical observations. Methods. We analyze a 200?ks Chandra/HETGS observation, subdivided into two 100?ks segments, of the CTTS V2129?Oph. For the two observing segments corresponding to two different phases within one stellar rotation, we measure the density of the cool plasma component and the emission measure distribution. Results. The X-ray emitting plasma covers a wide range of temperatures: from?2 up to 34?MK. The cool plasma component of V2129?Oph (T?≈?3?4?MK) varies between the two segments of the Chandra observation: during the first observing segment high density plasma () with high?EM at ~3?4?MK is present, whereas, during the second segment, this plasma component has lower?EM and lower density (log?Ne?3 R?). Conclusions. Our observation provides additional confirmation that the dense cool plasma at a?few?MK in CTTS is material heated in the accretion shock. The variability of this cool plasma component on V2129?Oph may be explained in terms of X-rays emitted in the accretion shock and seen with different viewing angles at the two rotational phases probed by our observation. In particular, during the first time interval a direct view of the shock region is possible, while, during the second, the accretion funnel itself intersects the line of sight to the shock region, preventing us from observing the accretion-driven X-rays.
机译:上下文。在几个CTTS中观察到的来自高密度等离子体的软X射线发射通常与吸积过程有关。然而,仍然不清楚这种高密度“冷”等离子体是在积聚激波中被加热,还是被冠状血浆喂入或通过积聚过程进行了改性。目的我们对CTTS V2129?Oph进行了协调的准同时光学和X射线观测活动。在本文中,我们分析了钱德拉光栅光谱仪的数据,并试图将观察到的X射线发射等离子体成分与吸积过程的特性以及同时进行光学观测所限制的恒星磁场相关联。方法。我们分析了CTTS V2129?Oph的200?ks Chandra / HETGS观测结果,细分为两个100?ks段。对于在一次恒星旋转中对应于两个不同相位的两个观测段,我们测量了冷等离子体成分的密度和发射测量分布。结果。发射X射线的等离子体覆盖的温度范围很广:从2到最高34 MK。 V2129?Oph的冷血浆成分(T?≈?3?4?MK)在钱德拉观测的两个部分之间变化:在第一个观察段期间,高密度电磁(〜3?4?MK)处于较高密度存在第二部分,而在第二段中,该血浆组分具有较低的ΔEM和较低的密度(log 2 Ne 3 R 3)。结论。我们的观察结果进一步证实了CTTS中少量MK处的致密冷等离子体是吸积激波中加热的物质。 V2129ΔOph上这种冷等离子体成分的变化可以用增生激波发出的X射线来解释,并且在我们观察到的两个旋转相位以不同的视角看到。特别是,在第一个时间间隔内可以直接看到冲击区域,而在第二个时间间隔内,吸积漏斗本身会与通往冲击区域的视线相交,从而使我们无法观察到由吸积驱动的X射线。

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