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首页> 外文期刊>The Astrophysical journal >Cosmological H_Ⅱ Bubble Growth During Reionization
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Cosmological H_Ⅱ Bubble Growth During Reionization

机译:电离过程中宇宙H_Ⅱ气泡的生长

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摘要

We present general properties of ionized hydrogen (H_Ⅱ) bubbles and their growth based on a state-of-the-art, large-scale (100 Mpc h~(-1)) cosmological radiative transfer simulation. The simulation resolves all halos with atomic cooling at the relevant redshifts and simultaneously performs radiative transfer and dynamical evolution of structure formation. Our major conclusions include the following: (1) For significant H_Ⅱ bubbles, the number distribution is peaked at a volume of ~0.6 Mpc~3 h~(-3) at all redshifts. But at z ≤ 10, one large, connected network of bubbles dominates the entire H_Ⅱ volume. (2) H_Ⅱ bubbles are highly nonspherical. (3) The H_Ⅱ regions are highly biased with respect to the underlying matter distribution, with the bias decreasing with time. (4) The non-Gaussianity of the H_Ⅱ region is small when the universe becomes 50% ionized. The non-Gaussianity reaches its maximum near the end of the reionization epoch z ~ 6. But at all redshifts of interest there is a significant non-Gaussianity in the H n field. (5) Population III galaxies may play a significant role in the reionization process. Small bubbles are initially largely produced by Population III stars. At z ≥ 10 even the largest H_Ⅱ bubbles have a balanced ionizing photon contribution from Population II and Population III stars, while atz ≤ 8 Population II stars start to dominate the overall ionizing photon production for large bubbles, although Population III stars continue to make a nonnegligible contribution. (6) The relationship between halo number density and bubble size is complicated, but a strong correlation is found between halo number density and bubble size for large bubbles.
机译:基于最新的大规模(100 Mpc h〜(-1))宇宙学辐射转移模拟,我们给出了离子化氢(H_Ⅱ)气泡的一般性质及其增长。该模拟通过在相关红移下的原子冷却来解析所有光晕,并同时执行辐射转移和结构形成的动态演化。我们的主要结论包括以下几个方面:(1)对于明显的H_Ⅱ气泡,在所有红移处,其数量分布均在〜0.6 Mpc〜3 h〜(-3)时达到峰值。但是在z≤10时,一个大的连通气泡网络支配了整个H_Ⅱ体积。 (2)H_Ⅱ气泡高度非球形。 (3)H_Ⅱ区域相对于底层物质的分布高度偏向,偏向随时间减小。 (4)当宇宙离子化率为50%时,H_Ⅱ区的非高斯性很小。非高斯性在电离时代z〜6结束时达到最大值。但是,在所有感兴趣的红移中,H n场中都存在明显的非高斯性。 (5)人口III星系在电离过程中可能起重要作用。小气泡最初主要是由人口III恒星产生的。在z≥10时,即使最大的H_Ⅱ气泡也具有来自种群II和种群III恒星的平衡的电离光子贡献,而atz≤8种群II的恒星开始在大气泡的总体电离光子产生中占主导地位,尽管种群III的恒星继续产生不可忽略的贡献。 (6)晕数密度与气泡大小之间的关系复杂,但是对于大气泡,晕数密度与气泡大小之间存在很强的相关性。

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