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arXiv 2301.01151astro-ph.GA
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限制支持CCSN遗迹中水形成的最小晕质量

Constraining the Minimum Halo Mass that Supports Water Formation in a CCSN Remnant

Christopher T. D. Jessop

摘要:

我们提出了一个模拟探测水的形成在宇宙学minihalo的低质量第三族超新星的残余物,并提供了一个暂定的主机minihaloes,可以在足够短的时间尺度上,并有效地混合金属在高密度的质量下限。我们从宇宙学的初始条件开始,当中心密度发生灾难性的坍缩时结束模拟,从而报告了水的丰度。在第三星族恒星的一生中,微晕(M $ = 5 \times 10^5$ M $_{\odot}$)被吹灭,因此微弱的超新星爆炸(E $_{\mathrm{SN}} = 5\times 10^{50}$ ergs)完全不局限于微晕的维里半径。在模拟结束时,整个遗迹的任何地方都没有明显的水形成,并且中心的第一个金属消失区域在将第一个金属融入自身时效率低下,保持在低金属含量。大多数金属通过双极流出从核心喷射到空隙中,并在非常低的密度下达到$\mathrm{Z} \sim 10^{-6}\ \mathrm{Z}_{\odot}$的金属丰度峰值。微晕的质量足够低,以至于在时间尺度上,这种结构是早期宇宙中水形成的主要途径是不合理的。我们还提供了与常规CCSN(E $_{\mathrm{SN}} = 10^{51}$ ergs)的比较,发现了相同的效果,但放大了。因此,我们可以认为,一个封闭的爆炸所需的最小微晕质量,因此水的形成的可能性至少是$10^{6}$ M $_{\odot}$和超新星遗迹的化学热演化是更敏感的主机微晕的质量比居住在它的第三族恒星的质量。

英文摘要:

We present a simulation probing the formation of water in the remnant of low-mass Population III supernovae in a cosmological minihalo, and provide a tentative lower mass limit on host minihaloes that can recollapse on a short enough timescale and efficiently mix metals at high densities. We start from cosmological initial conditions and end the simulation when the central density undergoes catastrophic recollapse, whereby the water abundance is reported. During the Population III stars lifetime, the minihalo (M$ = 5 \times 10^5$ M$_{\odot}$) becomes blown out, and consequently the faint supernova explosion (E$_{\mathrm{SN}} = 5\times 10^{50}$ ergs) is completely unconfined to the virial radius of the minihalo. At the end of the simulation there is no significant water formation anywhere throughout the remnant, and the central recollapsing region is inefficient at incorporating the first metals into itself, remaining at low metallicity. The majority of metals are ejected from the core via bipolar outflow into the void and reach a peak metallicity of $\mathrm{Z} \sim 10^{-6}\ \mathrm{Z}_{\odot}$ at very low densities. The mass of the minihalo is low enough such that the recollapse timescale is unreasonable for this configuration to be the primary avenue of water formation in the early universe. We also provide a comparison with a regular CCSN (E$_{\mathrm{SN}} = 10^{51}$ ergs) and find the same effect, but amplified. As such, we can suggest that the minimum minihalo mass required for a confined explosion, and therefore the possibility of water formation is at least $10^{6}$ M$_{\odot}$ and the chemo-thermal evolution of a supernova remnant is more sensitive to the mass of the host minihalo than the mass of the Population III star residing within it.

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