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arXiv 0908.0245astro-ph.GAastro-ph.CO
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Subaru/Suprime-Cam巡天仙女座恒星晕的结构和星族

Structure and Population of the Andromeda Stellar Halo from a Subaru/Suprime-Cam Survey

M. Tanaka, M. Chiba, Y. Komiyama, P. Guhathakurta, J. S. Kalirai, M. Iye

摘要:

我们提出了一个光度调查的恒星晕的仙女座星系,使用Suprime-Cam的斯巴鲁望远镜。详细分析VI色星等图的解决恒星星族被用来测量的属性,如视距,表面亮度,金属丰度,和年龄,这些被用来隔离和表征不同的组成部分的M31晕:(1)几个子结构,(2)光滑的晕。首先,我们研究了M31的晕子结构沿西北/东南短轴到R ~ 100 kpc和西南长轴区域在R ~ 60 kpc。我们证实了Ibata等人(2007)报道的东南晕中的两个亚结构,并在西北晕中发现了两个过密的亚结构。我们研究了这四个子结构以及包括西大陆架在内的其他结构的性质,发现这些系统之间的恒星星族存在差异,从而表明每个系统都有不同的起源。我们的统计分析表明,M31晕作为一个整体可能包含至少16个子结构,每一个都有不同的起源。其次,我们研究了R > 100 kpc的基础,光滑和扩展的晕分量的性质。我们发现这个光滑晕的表面密度可以用尺度半径为17 kpc的Hernquist模型或R^{-2.17 +/-0.15}的幂律分布拟合。与相对平滑的晕密度分布相反,它的金属丰度分布似乎是空间上不均匀的,随着半径的非单调变化,这表明晕人口没有足够的时间来动态均匀的吸积人口。对M31晕形成的进一步影响进行了讨论。

英文摘要:

We present a photometric survey of the stellar halo of the Andromeda galaxy, using Suprime-Cam on the Subaru Telescope. A detailed analysis of VI color-magnitude diagrams of the resolved stellar population is used to measure properties such as line-of-sight distance, surface brightness, metallicity, and age, and these are used to isolate and characterize different components of the M31 halo: (1) several substructures, and (2) the smooth halo. First, we study M31's halo substructure along the north-west/south-east minor axis out to R ~ 100 kpc and the south-west major axis region at R ~ 60 kpc. We confirm two substructures in the south-east halo reported by Ibata et al. (2007) and discover two overdense substructures in the north-west halo. We investigate the properties of these four substructures as well as other structures including the western shelf and find that differences in stellar populations among these systems, thereby suggesting each has a different origin. Our statistical analysis implies that the M31 halo as a whole may contain at least 16 substructures, each with a different origin. Second, we investigate the properties of an underlying, smooth and extended halo component out to R > 100 kpc. We find that the surface density of this smooth halo can be fitted to a Hernquist model of scale radius ~ 17 kpc or a power-law profile with ~ R^{-2.17 +/- 0.15}. In contrast to the relative smoothness of the halo density profile, its metallicity distribution appears to be spatially non-uniform with non-monotonic variations with radius, suggesting that the halo population has not had sufficient time to dynamically homogenize the accreted populations. Further implications for the formation of the M31 halo are discussed.

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