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首页> 外文期刊>The Astrophysical journal >First Structure Formation under the Influence of Gas–Dark Matter Streaming Velocity and Density: Impact of the “Baryons Trace Dark Matter” Approximation
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First Structure Formation under the Influence of Gas–Dark Matter Streaming Velocity and Density: Impact of the “Baryons Trace Dark Matter” Approximation

机译:气体暗物质流速度和密度影响下的第一结构形成:“重子痕迹暗物质”的影响近似

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The impact of streaming between baryons and dark matter on the first structures has been actively explored by recent studies. We investigate how the key results are affected by two popular approximations. One is to implement the streaming by accounting for only the relative motion while assuming "baryons trace dark matter" spatially at the initialization of simulation. This neglects the smoothing on the gas density taking place before the initialization. In our simulation initialized at z _(i )?=?200, it overestimates the gas density power spectrum by up to 40% at k ?≈?10~(2) h Mpc~(?1) at z ?=?20. Halo mass (M _(h )) and baryonic fraction in halos ( ) are also overestimated, but the relation between the two remains unchanged. The other approximation tested is to artificially amplify the density/velocity fluctuations in the cosmic mean density to simulate the first minihalos that form in overdense regions. This gives a head start to the halo growth while the subsequent growth is similar to that in the mean density. The growth in a true overdense region, on the other hand, is accelerated gradually in time. For example, raising σ _(8) by 50% effectively transforms in the halo mass growth history while, at 2σ overdensity, the growth is accelerated by a constant in redshift: . As a result, halos have grown more massive in the former than in the latter before z ?≈?27 and vice versa after. The –M _(h ) relation is unchanged in those cases as well, suggesting that the Population III formation rate for a given M _(h ) is insensitive to the tested approximations.
机译:最近的研究已经积极探索了在第一结构上的重区和暗物质之间的流动的影响。我们调查关键结果如何受到两个流行近似的影响。一个是通过仅在空间上在初始化初始化时占用相对运动来实现流媒体。这忽略了在初始化之前发生的气体密度的平滑。在我们的模拟中初始化在 z _( i)中?=Δ200,在 k k = k = k = k = x 10〜(2) h MPC〜(?1)在 z?=?20。卤素质量( m _( h))和卤素()中的缩放部分也被高估,但两个保持关系保持不变。测试的其他近似是人工放大宇宙平均密度中的密度/速度波动,以模拟形成在过阵地区的第一个minihalos。这使得头部开始于光晕增长,而随后的增长与平均密度相似。另一方面,真正的过阵地区的增长在时间逐渐加速。例如,在卤素质量生长历史中升高50%的升高50%,同时,在2 σ过度密度下,通过红移中的常数加速生长:。结果,晕圈在前者中比在 z之前在前者中产生了更大的巨大巨大,反之亦然。 - M _( h)关系在这些情况下不变,表明给定的 m _( h)的群体III形成速率对测试的近似不敏感。

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