论文标题

使用FRB探索氢气离子的时代

Exploring the epoch of hydrogen reionization using FRBs

论文作者

Beniamini, Paz, Kumar, Pawan, Ma, Xiangcheng, Quataert, Eliot

论文摘要

我们描述了使用快速无线电爆发(FRB)探索氢气离子时期的三种不同方法,并为在高红移(Z)上存在FRB的存在提供了参数。从观察上讲,最简单的方法是确定FRB的最大分散度度量(DM $ _ {\ rm max} $)的合奏,其中包括在电源过程中进行爆发。 dm $ _ {\ rm max} $提供了有关振荡的信息,就像cmb的光学深度到汤姆森散射一样,如果可以将dm $ _ {\ rm max} $比500 $ \ mbox $ \ mbox $ \ mbobs $ \ mbox c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c c的,它具有比Planck的约束更准确的可能性。另一种方法是用$ \ sim10 \%$精度测量6-10 Z之间的红移,以获得4个不同的Z bin的平均电子密度,具有$ \ sim4 \%$ $精度。这两种方法不需要了解FRB光度函数及其可能的红移演变。最后,我们表明,鉴于对包括在电离时期内发生的爆发的FRB的调查限制了每单位DM的FRB数量,电源历史反映了。我们使用消防模拟表明,在Reionization时代,FRB主机Galaxy $ \&$ CGM对DM的贡献是观察到的DM的一小部分。第三种方法不需要红移信息,但确实需要了解FRB光度功能。

We describe three different methods for exploring the hydrogen reionization epoch using fast radio bursts (FRBs) and provide arguments for the existence of FRBs at high redshift (z). The simplest way, observationally, is to determine the maximum dispersion measure (DM$_{\rm max}$) of FRBs for an ensemble that includes bursts during the reionization. The DM$_{\rm max}$ provides information regarding reionization much like the optical depth of the CMB to Thomson scattering does, and it has the potential to be more accurate than constraints from Planck, if DM$_{\rm max}$ can be measured to a precision better than 500 $\mbox{pc cm}^{-3}$. Another method is to measure redshifts of about 40 FRBs between z of 6-10 with$\sim10\%$ accuracy to obtain the average electron density in 4 different z-bins with $\sim4\%$ accuracy. These two methods don't require knowledge of the FRB luminosity function and its possible redshift evolution. Finally, we show that the reionization history is reflected in the number of FRBs per unit DM, given a fluence limited survey of FRBs that includes bursts during the reionization epoch; we show using FIRE simulations that the contributions to DM from the FRB host galaxy $\&$ CGM during the reionization era is a small fraction of the observed DM. This third method requires no redshift information but does require knowledge of the FRB luminosity function.

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