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arXiv 0805.2841astro-ph
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嵌入喷流的IR诊断:HH34和HH1喷流的速度分辨观察

IR diagnostics of embedded jets: velocity resolved observations of the HH34 and HH1 jets

R. Garcia Lopez, B. Nisini, T. Giannini, J. Eisloeffel, F. Bacciotti, L. Podio

摘要:

我们介绍了HH 34和HH 1喷流的VLT-ISAAC中等分辨率光谱。我们的目的是推导出运动学和物理参数,并研究它们如何随射流速度而变化。我们使用了几条重要的诊断线,如[Fe Ⅱ] 1.644 μ m,1.600 μ m和H2 2.122 μ m。在HH 34的内喷流区,我们发现原子和分子气体都呈现出高速和低速两种成分。HH 34中的[FeII] LVC在距离源很远的地方(>1000 AU)被检测到,与TTauri喷流不同。在H2 2.122um中,LVC和HVC在空间上分离。我们第一次探测到了中心源的较暗的红移对应物。在HH 1中,我们追踪射流到VLA 1驱动源的~1”处:该内部区域的运动学再次以两个速度分量的存在为特征,一个相对于源LSR速度蓝移,一个相对于源LSR速度红移。在HH 34射流内部区域,ne随速度的减小而增大。在距离驱动源约10”处,沿着整个HH 1射流观察到相反的行为,ne随速度增加。在这两种射流中,质量通量主要由高速气体携带。对HH 34的位置速度图和导出的电子密度与MHD喷气发射机制模型进行了比较。虽然在喷流底部的线发射的运动学特性可以,至少在定性上,再现的X风和盘风模型,这些模型都不能解释的程度LVC和电子密度与速度的依赖关系,我们观察到。可能的是,HH 34中的LVC表示不直接喷射在射流中的气体,而是由高速准直射流夹带的更密集的环境气体。

英文摘要:

We present VLT-ISAAC medium resolution spectroscopy of the HH34 and HH1 jets. Our aim is to derive the kinematics and the physical parameters and to study how they vary with jet velocity. We use several important diagnostic lines such as [FeII] 1.644um, 1.600um and H2 2.122um. In the inner jet region of HH34 we find that both the atomic and molecular gas present two components at high and low velocity. The [FeII] LVC in HH34 is detected up to large distances from the source (>1000 AU), at variance with TTauri jets. In H2 2.122um, the LVC and HVC are spatially separated. We detect, for the first time, the fainter red-shifted counterpart down to the central source. In HH1, we trace the jet down to ~1" from the VLA1 driving source: the kinematics of this inner region is again characterised by the presence of two velocity components, one blue-shifted and one red-shifted with respect to the source LSR velocity. In the inner HH34 jet region, ne increases with decreasing velocity. Up to ~10" from the driving source, and along the whole HH1 jet an opposite behaviour is observed instead, with ne increasing with velocity. In both jets the mass flux is carried mainly by the high-velocity gas. A comparison between the position velocity diagrams and derived electron densities with models for MHD jet launching mechanisms has been performed for HH34. While the kinematical characteristics of the line emission at the jet base can be, at least qualitatively, reproduced by both X-winds and disc-wind models, none of these models can explain the extent of the LVC and the dependence of electron density with velocity that we observe. It is possible that the LVC in HH34 represents gas not directly ejected in the jet but instead denser ambient gas entrained by the high velocity collimated jet.

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