Hannah C. Turner, M. Lovell, J. Zavala, M. Vogelsberger
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引用次数: 22
摘要
有人提出暗物质自相互作用引起的引力热坍缩(即自相互作用暗物质,SIDM)可以解释观测到的银河系(MW)卫星中心动力质量的多样性。我们利用速度依赖自相互作用暗物质(vdSIDM)的mw模拟晕的$N$ -体模拟来研究这一假设背后的过程,其中低速自散射截面$\sigma_\rmn{T}/m_\rmn{x}$达到100 $~$ cm $^{2}$ g $^{-1}$;我们称这个模型为vd100模型。我们将此模拟结果与使用不同暗模型(包括冷暗物质(CDM)和其他不太极端的SIDM模型)的相同晕的模拟结果进行了比较。vd100光晕的质量与CDM光晕非常相似,但其最大圆周速度$V_\rmn{max}$的值要高得多。我们确定这些高$V_\rmn{max}$亚晕是质量范围在[$5\times10^{6}$, $1\times10^{8}$] $~$$\msun$ at $z=1$的物体,它们经历了地心引力的核心坍缩。这些坍缩晕的密度分布由单次幂定律描述,直到模拟的分辨率极限,该密度分布的内斜率约为$-3$。解决不断减少的坍塌区域是具有挑战性的,需要量身定制的模拟,以在$<1$$~$ kpc尺度上精确地模拟失控的不稳定性。
The onset of gravothermal core collapse in velocity-dependent self-interacting dark matter subhaloes
It has been proposed that gravothermal collapse due to dark matter self-interactions (i.e. self-interacting dark matter, SIDM) can explain the observed diversity of the Milky Way (MW) satellites' central dynamical masses. We investigate the process behind this hypothesis using an $N$-body simulation of a MW-analogue halo with velocity dependent self-interacting dark matter (vdSIDM) in which the low velocity self-scattering cross-section, $\sigma_\rmn{T}/m_\rmn{x}$, reaches 100$~$cm$^{2}$g$^{-1}$; we dub this model the vd100 model. We compare the results of this simulation to simulations of the same halo that employ different dark models, including cold dark matter (CDM) and other, less extreme SIDM models. The masses of the vd100 haloes are very similar to their CDM counterparts, but the values of their maximum circular velocities, $V_\rmn{max}$, are significantly higher. We determine that these high $V_\rmn{max}$ subhaloes were objects in the mass range [$5\times10^{6}$, $1\times10^{8}$]$~$$\msun$ at $z=1$ that undergo gravothermal core collapse. These collapsed haloes have density profiles that are described by single power laws down to the resolution limit of the simulation, and the inner slope of this density profile is approximately $-3$. Resolving the ever decreasing collapsed region is challenging, and tailored simulations will be required to model the runaway instability accurately at scales $<1$$~$kpc.