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arXiv 1604.02458hep-phastro-ph.CO
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冷暗区和不对称再加热

Chilly Dark Sectors and Asymmetric Reheating

Peter Adshead, Yanou Cui, Jessie Shelton

摘要:

在一大类理论中,暗物质的残余丰度是由热化暗扇区内部的相互作用决定的,标准模型(SM)没有直接参与。我们指出,这些理论提出了一个直接的宇宙学问题:暗区最初是如何在早期宇宙中的人口?部分原因是由于难以容纳大量的熵进行暗辐射与宇宙微波背景测量的有效数量的相对论性物种在重组,$N_{\mathrm{eff}}$,我们的目标是建立哪些可接受的宇宙学历史可以填充一个热黑暗的部门,永远不会达到热平衡与SM。这种暗区的最小宇宙学起源是不对称再加热,在早期宇宙中填充SM的相同机制也在较低温度下填充暗区。在这里,我们证明了由此产生的不可避免的暴胀介导的散射之间的黑暗部门和SM可以洗出一个可能的温度不对称性,并建立参数空间的区域,温度不对称性可以产生在最小的再加热方案。因此,获得给定尺寸的温度不对称性要么限制了可能的暴胀子质量和耦合,要么需要一个或两个扇区的非最小宇宙学。作为一个附带的好处,我们开发的技术,用于评估碰撞条款的相对论玻尔兹曼方程时,必须保留玻色-爱因斯坦或费米-狄拉克相空间分布的充分依赖,并提出了几个新的结果相对论热平均在附录中。

英文摘要:

In a broad class of theories, the relic abundance of dark matter is determined by interactions internal to a thermalized dark sector, with no direct involvement of the Standard Model (SM). We point out that these theories raise an immediate cosmological question: how was the dark sector initially populated in the early universe? Motivated in part by the difficulty of accommodating large amounts of entropy carried in dark radiation with cosmic microwave background measurements of the effective number of relativistic species at recombination, $N_{\mathrm{eff}}$, we aim to establish which admissible cosmological histories can populate a thermal dark sector that never reaches thermal equilibrium with the SM. The minimal cosmological origin for such a dark sector is asymmetric reheating, when the same mechanism that populates the SM in the early universe also populates the dark sector at a lower temperature. Here we demonstrate that the resulting inevitable inflaton-mediated scattering between the dark sector and the SM can wash out a would-be temperature asymmetry, and establish the regions of parameter space where temperature asymmetries can be generated in minimal reheating scenarios. Thus obtaining a temperature asymmetry of a given size either restricts possible inflaton masses and couplings or necessitates a non-minimal cosmology for one or both sectors. As a side benefit, we develop techniques for evaluating collision terms in the relativistic Boltzmann equation when the full dependence on Bose-Einstein or Fermi-Dirac phase space distributions must be retained, and present several new results on relativistic thermal averages in an appendix.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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