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arXiv 1612.00535astro-ph.HEastro-ph.GA
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钱德拉对NGC 1404的深度观测:坠落的早期星系揭示的星系团等离子体物理

Deep Chandra observations of NGC 1404: cluster plasma physics revealed by an infalling early-type galaxy

Yuanyuan Su, Ralph P. Kraft, Elke Roediger, Paul E. J. Nulsen, William R. Forman, Eugene Churazov, Scott W. Randall, Christine Jones, Marie E. Machacek

摘要:

团内介质(ICM)作为一种磁化和高度电离的流体,为研究地球上尚无法实现的极端条件下的等离子体物理提供了理想的实验室。NGC 1404是一个明亮的椭圆星系,当它穿过天炉座星系团的ICM时,正在被气体剥离。我们利用NGC 1404的{ \sl Chandra} X射线新观测资料研究ICM微物理。NGC 1404的星际介质(ISM)的特征是有一个尖锐的前缘,距离星系中心8 kpc,和一个短的下游气体尾部。由于NGC 1404的邻近性、{ \sl Chandra}的极好的空间分辨率和非常深(670 ksec)的曝光的组合,接触不连续性在前所未有的空间尺度($0\farcs5=45$ \,pc)上被解决。在前缘,我们观察到了由Kelvin-Helmholtz不稳定性产生的亚kpc尺度的涡旋,并对热团簇等离子体的各向同性粘滞系数提出了5%的Spitzer上限.我们还观察到在下游剥离的尾巴,这提供了一个低粘度等离子体的进一步证据,热的星系团气体和较冷的星系气体之间的混合。假设ICM中的有序磁场应小于5\,$μ$ G,以允许KHI的发展。刚好在接触边缘外部缺乏明显的磁性覆盖层与这样的上限一致。

英文摘要:

The intracluster medium (ICM), as a magnetized and highly ionized fluid, provides an ideal laboratory to study plasma physics under extreme conditions that cannot yet be achieved on Earth. NGC 1404 is a bright elliptical galaxy that is being gas stripped as it falls through the ICM of the Fornax Cluster. We use the new {\sl Chandra} X-ray observations of NGC 1404 to study ICM microphysics. The interstellar medium (ISM) of NGC 1404 is characterized by a sharp leading edge, 8 kpc from the galaxy center, and a short downstream gaseous tail. Contact discontinuities are resolved on unprecedented spatial scales ($0\farcs5=45$\,pc) due to the combination of the proximity of NGC 1404, the superb spatial resolution of {\sl Chandra}, and the very deep (670 ksec) exposure. At the leading edge, we observe sub-kpc scale eddies generated by Kelvin-Helmholtz instability and put an upper limit of 5\% Spitzer on the isotropic viscosity of the hot cluster plasma. We also observe mixing between the hot cluster gas and the cooler galaxy gas in the downstream stripped tail, which provides further evidence of a low viscosity plasma. The assumed ordered magnetic fields in the ICM ought to be smaller than 5\,$μ$G to allow KHI to develop. The lack of evident magnetic draping layer just outside the contact edge is consistent with such an upper limit.

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