原始黑洞的约束和来自全球21厘米信号的曲率扰动

Yupeng Yang
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引用次数: 10

摘要

最近EDGES对全球21cm信号的观测和LIGO/VIGO对引力波的观测重新唤起了人们对pbh的兴趣。与以往的工作不同,我们研究了pbh对质量范围$6\times 10^{13} {\rm g} \lesssim M_{\rm PBH}\lesssim 3\times 10^{14} \rm g$的IGM演化的影响。由于这些pbh的寿命比宇宙现在的年龄要短,它们在今天已经蒸发了。由于霍金辐射,pbh对IGM的加热效应可以抑制全球21cm信号的吸收幅度。在这项工作中,我们要求全球21cm信号在$10\lesssim z \lesssim 30$(例如$\delta T_{b} \lesssim -100~\rm mK$)红移范围内的亮温差,从而获得了PBHs初始质量分数的上限。我们发现最强上限为$\beta_{\rm PBH} \sim 2\times 10^{-30}$。由于pbh的形成与原始曲率扰动有关,通过对pbh初始质量分数的约束,我们获得了原始曲率扰动在$8.0\times 10^{15}\lesssim k \lesssim 1.8\times 10^{16}~\rm Mpc^{-1}$尺度范围内的功率谱上限,对应于本文考虑的质量范围。我们发现最强上限为$\mathcal P_{\mathcal R}(k) \sim 0.0046$。通过与以往的研究比较,我们发现对于本文研究的质量范围(或尺度范围),全球21cm信号或21cm功率谱应该给出PBHs的初始质量分数和原始曲率摄动的功率谱的最强上限。
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Constraints on primordial black holes and curvature perturbations from the global 21-cm signal
The recent observations of the global 21cm signal by EDGES and gravitational waves by LIGO/VIGO have revived interest in PBHs. Different from previous works, we investigate the influence of PBHs on the evolution of the IGM for the mass range $6\times 10^{13} {\rm g} \lesssim M_{\rm PBH}\lesssim 3\times 10^{14} \rm g$. Since the lifetime of these PBHs is smaller than the present age of the Universe, they have evaporated by the present day. Due to Hawking radiation, the heating effects of PBHs on the IGM can suppress the absorption amplitude of the global 21cm signal. In this work, by requiring that the differential brightness temperature of the global 21cm signals in the redshift range of $10\lesssim z \lesssim 30$, e.g., $\delta T_{b} \lesssim -100~\rm mK$, we obtain upper limits on the initial mass fraction of PBHs. We find that the strongest upper limit is $\beta_{\rm PBH} \sim 2\times 10^{-30}$. Since the formation of PBHs is related to primordial curvature perturbations, by using the constraints on the initial mass fraction of PBHs we obtain the upper limits on the power spectrum of primordial curvature perturbations for the scale range $8.0\times 10^{15}\lesssim k \lesssim 1.8\times 10^{16}~\rm Mpc^{-1}$, corresponding to the mass range considered here. We find that the strongest upper limit is $\mathcal P_{\mathcal R}(k) \sim 0.0046$. By comparing with previous works, we find that for the mass range (or the scale range) investigated in this work the global 21cm signals or the 21cm power spectrum should give the strongest upper limits on the initial mass fraction of PBHs and on the power spectrum of primordial curvature perturbations.
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