论文标题

暗物质概况,用于模拟各种反馈引起的核心大小为$λ$ cdm光环

A dark matter profile to model diverse feedback-induced core sizes of $Λ$CDM haloes

论文作者

Lazar, Alexandres, Bullock, James S., Boylan-Kolchin, Michael, Chan, T. K., Hopkins, Philip F., Graus, Andrew S., Wetzel, Andrew, El-Badry, Kareem, Wheeler, Coral, Straight, Maria C., Kereš, Dušan, Faucher-Giguère, Claude-André, Fitts, Alex, Garrison-Kimmel, Shea

论文摘要

我们分析了使用Fire-2 Galaxy形成物理学模拟的54个星系光环的冷暗物质密度曲线,每个模拟了Halo病毒半径的0.5 \%$。这些晕孔包含带有质量的星系,其范围从超斑点($ m_ \ star \ star \ simeq 10^{4.5} m _ {\ odot} $)到最大的螺旋($ M_ \ star \ star \ simeq 10^{11}} M _ {\ odot} $),并且两者都是浓度和浓度和浓度。我们使用新的分析密度曲线来表征我们的结果,该密度谱扩展标准的Einasto形式,以允许在已解决的最终半径中明显地恒定密度核心。有了一个附加的核心 - 拉迪乌斯参数,$ r_ {c} $,此“ Core-Inasto”配置文件能够表征我们反馈影响的暗物质Halos的形状和标准化。为了启用与观测值的比较,我们为$ r_ {c} $和其他配置文件参数提供了拟合功能,这是$ M_ \ star $和$ m _ {\ star}/m _ {\ rm halo} $的函数。与文献中所做的类似研究一致,我们发现深质物质核心形成在特征性恒星质量与卤素质量比$ m_ \ star/m _ {\ rm halo} \ simeq 5 \ simeq 5 \ simeq 5 \ times 10^{ - 3} $或$ m _ {大约是银河半径半径的大小,$ r_ {c} \ simeq 1-5 $ kpc。此外,我们没有发现在半径上以$ M _ {\ star}/m _ {\ rm halo} <5 \ times 10^{ - 4} $或$ m _ 4} $或$ m_ \ star \ star \ sart \ sart \ sater \ sater \ sater \ sater \ sater \ sater \ sater \ sater \ sater \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ sstar \ 6 6 \,m m _ _ {对于银河系大小的星系,巴里尼克收缩通常会使光晕在恒星半光线半径上明显更加集中和浓密,而仅仅是暗物质。但是,即使在银河系量表上,Fire-2 Galaxy形成仍然会产生$ \ simeq 0.5-2 $ kpc的小型暗物质核心。在银河系的暗物质光环中,$ {\ sim} 2 $ kpc核心的最新证据与这种期望是一致的。

We analyze the cold dark matter density profiles of 54 galaxy halos simulated with FIRE-2 galaxy formation physics, each resolved within $0.5\%$ of the halo virial radius. These halos contain galaxies with masses that range from ultra-faint dwarfs ($M_\star \simeq 10^{4.5} M_{\odot}$) to the largest spirals ($M_\star \simeq 10^{11} M_{\odot}$) and have density profiles that are both cored and cuspy. We characterize our results using a new analytic density profile that extends the standard Einasto form to allow for a pronounced constant-density core in the resolved innermost radius. With one additional core-radius parameter, $r_{c}$, this "core-Einasto" profile is able to characterize the shape and normalization of our feedback-impacted dark matter halos. In order to enable comparisons with observations, we provide fitting functions for $r_{c}$ and other profile parameters as a function of both $M_\star$ and $M_{\star}/M_{\rm halo}$. In agreement with similar studies done in the literature, we find that dark matter core formation is most efficient at the characteristic stellar-mass to halo-mass ratio $M_\star/M_{\rm halo} \simeq 5 \times 10^{-3}$, or $M_{\star} \sim 10^9 \, M_{\odot}$, with cores that are roughly the size of the galaxy half-light radius, $r_{c} \simeq 1-5$ kpc. Furthermore, we find no evidence for core formation at radii $\gtrsim 100\ \rm pc$ in galaxies with $M_{\star}/M_{\rm halo} < 5\times 10^{-4}$ or $M_\star \lesssim 10^6 \, M_{\odot}$. For Milky Way-size galaxies, baryonic contraction often makes halos significantly more concentrated and dense at the stellar half-light radius than dark matter only runs. However, even at the Milky Way scale, FIRE-2 galaxy formation still produces small dark matter cores of $\simeq 0.5-2$ kpc in size. Recent evidence for a ${\sim} 2$ kpc core in the Milky Way's dark matter halo is consistent with this expectation.

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