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arXiv 1105.2580astro-ph.COastro-ph.HE
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动态S0 Galerkin II:扩散热气体的作用

Dynamic S0 Galaxies II: the Role of Diffuse Hot Gas

Jiang-Tao Li, Q. Daniel Wang, Zhiyuan Li, Yang Chen

摘要:

气体损失被认为是重要的SF淬火和形态转变的S 0星系的演化过程中。在高密度环境中,气体损失可以通过许多外部机制实现。然而,在相对孤立的环境中,这些外部机制不能有效,气体损失必须由一些内部过程主导。我们进行钱德拉分析的热气体在附近的五个孤立的S 0星系,定量减去各种恒星的贡献的基础上。我们发现,在本工作中研究的所有星系的X射线微弱,与热气体光度LX<5%的预期Ia SN的能量注入率。我们进一步比较我们的结果与最近的相关论文,以调查的能量收支,冷热气体的关系,和气体从孤立的环境中的S 0星系的去除。我们发现椭圆星系和S 0星系在低质量端的LX没有显著差异(通常LK<1 e11 Lsun)。然而,在高质量的一端,S 0星系往往有显着较低的LX比相同的恒星质量的椭圆星系。我们进一步讨论了S 0和椭圆星系中弥散X射线辐射与冷气含量的潜在关系。我们发现,当M(H2 +HI)<1 e8 Msun时,贫气体星系的LX/LK ^2与冷气总质量M(H2 + HI)呈正相关,而当富气体星系的LX/LK ^2与冷气总质量M(H2 +HI)反相关。这种冷热气体的关系可以用星系演化的场景来解释,来自前体恒星形成星系的剩余冷气体主要被持久的Ia SN反馈所消除。富气星系和贫气星系的这两种不同的变化趋势可能分别是由于星系初始的SN速率快速下降和后来的质量负荷快速下降的结果。

英文摘要:

Gas loss is thought to be important in SF quenching and morphological transition during the evolution of S0 galaxies. In high density environments, gas loss can be achieved via many external mechanisms. However, in relatively isolated environments, where these external mechanisms cannot be efficient, gas loss must be dominated by some internal processes. We perform Chandra analysis of hot gas in five nearby isolated S0 galaxies, based on quantitative subtraction of various stellar contributions. We find that all the galaxies studied in the present work are X-ray faint, with the hot gas luminosity LX<5% of the expected Ia SN energy injection rate. We further compare our results with those from relevant recent papers, in order to investigate the energy budget, cold-hot gas relation, and gas removal from S0 galaxies in isolated environments. We find that elliptical and S0 galaxies are not significantly different in LX at the low mass end (typically with LK<1e11Lsun). However, at the high mass end, S0 galaxies tend to have significantly lower LX than elliptical galaxies of the same stellar masses. We further discuss the potential relation of the diffuse X-ray emission with the cold gas content in S0 and elliptical galaxies. We find that LX/LK^2 tends to correlate positively with the total cold gas mass M(H2+HI) for gas-poor galaxies with M(H2+HI)<1e8Msun, while they anti-correlate with each other for gas-rich ones. This cold-hot gas relation can be explained in a scenario of galaxy evolution, with the leftover cold gas from the precursor star forming galaxy mainly removed by the long-lasting Ia SN feedback. The two different trends for gas-rich and -poor galaxies may be the results of the initial fast decreasing SN rate and the later fast decreasing mass-loading to hot gas, respectively.

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