星系中恒星形成速率密度的演化

J. Wirsich
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摘要

本文提出了一种基于约束冷暗物质晕质量函数的全球恒星形成密度(SFD)的半解析计算。光晕质量MH(z)和恒星质量M*(z)都是从Lyα发射星系(LAEs)和/或Lyman破星系(LBGs)的观测中得到的。它们中的大多数,经过光谱选择,以高恒星形成率为特征。星系形成的观点主要基于结构形成的分层(“自下而上”)冷暗物质模型。我们使用了晕质量和星系中晕质量MH在红移z的恒星形成率之间的联系。我们的模型的优点是我们能够通过一个封闭方程计算全球恒星形成率ρ*(z)(在M * y-1Mpc-3中)。所有参数(MH;M*和n)具有明确定义的物理意义。从CDM谱来看,光晕质量函数的幂律指数得到了很好的约束。我们的结果编译在表1和图1中。在这里,我们的结果与观测和流体动力学模拟进行了比较。讨论了共动宇宙恒星密度随三个时期红移的演化的物理意义。在红移z = 0 - 7的范围内,我们发现从观测推断的SFD与我们的模型之间有很好的一致性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Evolution of Star Formation Rate Density of Galaxies
We present a semi-analytical calculation of the global star formation density (SFD) by using the well constrained cold dark matter (CDM) halo mass function. Both, halo masses MH(z) and stellar masses M*(z) are taken from observations of Lyα emitter (LAEs) and/or Lyman break galaxies (LBGs). Most of them, spectroscopically selected, are characterized by high star formation rates. The view of galaxy formation is mainly based on the hierarchical (“botton-up”) cold dark matter model for structure formation. We have used the connection between the halo mass and the star formation rate in galaxies of the halo mass MH at redshift z. Our model has the advantage that we are able to calculate the global star formation rate ρ*(z) (in Mʘy-1Mpc-3) by a closed equation. All parameters (MH; M* and n) have a well-defined physical meaning. From the CDM spectrum, the power law index of the halo mass function is well constrained. Our results are compiled in Table 1 and Figure 1. Here our results are compared with observations and hydrodynamical simulations. The physical meaning of the evolution of comoving cosmic star density as a function of redshift with three epochs is discussed. We find a good agreement between the SFD inferred from observations and our model in the range of redshifts z = 0 - 7.
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