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arXiv 0807.2102astro-ph
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小麦哲伦云的总质量和暗晕性质

The total mass and dark halo properties of the Small Magellanic Cloud

Kenji Bekki, Snezana Stanimirovic

摘要:

基于小麦哲伦云(SMC)高分辨率中性氢(HI)观测,讨论了在合理的$V$波段星质光比($M_{\rm s}/L_{\rm V}$)下SMC的总质量和暗晕性质.我们采用Burkert和NFW配置文件的暗物质晕的SMC,以模拟所观察到的旋转曲线的径向轮廓。我们表明,质量($M_{\rm dm}$)和平均密度($ρ_{\rm dm}$)的光学半径($\sim 3$ kpc)的SMC内的暗物质晕可以显着低的$M_{\rm s}/L_{\rm V}=2-4$合理的星系占主导地位的老恒星种群。例如,对于$M_{\rm s}/L_{\rm V} = 3.8$,估计的$M_{\rm dm}$和$ρ_{\rm dm}$分别是$7.5 \times 10^7 {\rm M}_{\odot}$和$6.7 \times 10^{-4} {\rm M}_{\odot}$ pc $^{-3}$。具有较低$M_{\rm s}/L_{\rm V}$($<1.0$)的模型可以显示较高的$M_{\rm dm}$和$ρ_{\rm dm}$,但难以再现Burkert和NFW轮廓的内旋转曲线轮廓。对于合理的$M_{\rm s}/L_{\rm V} \sim2$,具有较大核心半径($>1$ kpc)(因此密度较低)和较大质量(${\rm M}_{\rm dm} > 3 \times 10^9 {\rm M}_{\odot}$)的Burkert剖面比NFW剖面更能拟合观测到的缓慢上升的旋转曲线。这意味着大部分暗晕质量最初可能位于SMC的光学半径之外,因此由于与银河系以及可能与大麦哲伦云(LMC)的强烈潮汐相互作用,暗晕已经失去了其原始质量的重要部分。

英文摘要:

We discuss the total mass and dark halo properties of the Small Magellanic Cloud (SMC) for reasonable $V$-band stellar-to-mass-to-light ratios ($M_{\rm s}/L_{\rm V}$) based on the high-resolution neutral hydrogen (HI) observations of the SMC. We adopt both the Burkert and the NFW profiles for the dark matter halo of the SMC in order to model the radial profile of the observed rotation curve. We show that the mass ($M_{\rm dm}$) and the mean density ($ρ_{\rm dm}$) of the dark matter halo within the optical radius ($\sim 3$ kpc) of the SMC can be significantly low for $M_{\rm s}/L_{\rm V}=2-4$ reasonable for a galaxy dominated by older stellar populations. For example, the estimated $M_{\rm dm}$ and $ρ_{\rm dm}$ are $7.5 \times 10^7 {\rm M}_{\odot}$ and $6.7 \times 10^{-4} {\rm M}_{\odot}$ pc$^{-3}$, respectively, for $M_{\rm s}/L_{\rm V} = 3.8$. The models with lower $M_{\rm s}/L_{\rm V}$ ($<1.0$) can show higher $M_{\rm dm}$ and $ρ_{\rm dm}$ yet have difficulties in reproducing the inner rotation curve profile both for the Burkert and the NFW profiles. The Burkert profile with a larger core radius ($>1$ kpc) (thus a low density) and a large mass (${\rm M}_{\rm dm} > 3 \times 10^9 {\rm M}_{\odot}$) can be better fit to the observed slowly rising rotation curve than the NFW one for a reasonable $M_{\rm s}/L_{\rm V} \sim2$. This means that most of the dark halo mass can be initially located outside the optical radius in the SMC and thus that the dark halo would have already lost a significant fraction of its original mass due to the strong tidal interactions with the Galaxy and possibly with the Large Magellanic Cloud (LMC).

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