A measurement of the escaping ionising efficiency of galaxies at redshift 5

Sarah E. I. Bosman, Frederick B. Davies
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Abstract

The escaping ionising efficiency from galaxies, $f_{\rm esc}\xi_{\rm ion}$, is a crucial ingredient for understanding their contribution to hydrogen reionisation, but both of its components, $f_{\rm{esc}}$ and $\xi_{\rm{ion}}$, are extremely difficult to measure. We measure the average escaping ionising efficiency $\langle f_{\rm{esc}} \xi_{\rm{ion}}\rangle$ of galaxies at $z=5$ implied by the mean level of ionisation in the intergalactic medium via the Lyman-$\alpha$ forest. We use the fact that $\dot{N}_{\rm{ion}} = \rho_{\rm{UV}} f_{\rm{esc}} \xi_{\rm{ion}}$, the product of the ionising output and the UV density $\rho_{\rm{UV}}$, can be calculated from the known average strength of the UV background and the mean free path of ionising photons. These quantities, as well as $\rho_{\rm{UV}}$, are robustly measured at $z\leq6$. We calculate the missing factor of $\langle f_{\rm{esc}} \xi_{\rm{ion}}\rangle$ at $z=5$, during a convenient epoch after hydrogen reionisation has completed and the intergalactic medium has reached ionisation equilibrium, but before bright quasars begin to dominate the ionising photon production. Intuitively, our constraint corresponds to the required escaping ionising production from galaxies in order to avoid over- or under-ionising the Lyman-$\alpha$ forest. We obtain a measurement of $\log \langle f_{\rm{esc}} \xi_{\rm{ion}}\rangle /$erg Hz$^{-1}$ $ = 24.28_{-0.20}^{+0.21}$ at $z=5$ when integrating $\rho_\text{UV}$ down to a limiting magnitude $M_\text{lim}=-11$. Our measurement of the escaping ionising efficiency of galaxies is in rough agreement with both observations and most models.
对红移 5 处星系逸出电离效率的测量
星系的逸出电离效率($f_\{rmesc}\xi_\{rm ion}$)是了解星系对氢化贡献的一个关键要素,但它的两个组成部分,即$f_{\rm{esc}}$和$\xi_\{rm{ion}}$,都非常难以测量。我们测量的是平均逸出离子效率 $\langle f_{rm{esc}}$ 和 $\xi_{\rm{ion}}$\我们测量了星系在 $z=5 时的平均逸出离子效率$langle f_{xi_\rm{ion}}/rangle$ ,它是由星系间介质的平均电离水平通过莱曼-$α森林推算出来的。我们使用了 $\dot{N}_{\rm{ion}} =\rho_{\rm{UV}} f_{\rm{esc}} 这一事实。\xi_{\rm{ion}}$,即电离输出与紫外密度 $\rho_{\rm{UV}}$ 的乘积,可以通过已知的紫外背景平均强度和电离光子的平均自由路径计算得出。这些量以及 $\rho_{rm\{UV}}$ 都是在 $z\leq6$ 时测得的。我们计算了 $langle f_{\rm{esc}} 的缺失因子\xi_{\rm{ion}}/rangle$在$z=5$时的缺失因子,这是在氢再电离完成、银河系介质达到电离平衡之后,但在亮类星体开始主导电离光子产生之前的一个合适的时间段。直观地说,我们的约束条件相当于为了避免莱曼-$α森林电离过度或电离不足而需要从星系中逸散出的电离产生量。\xi_{\rm{ion}}\rangle/erg Hz$^{-1}$ $ = 24.28_{-0.20}^{+0.21}$在$z=5$时,将$\rrh_\text{UV}$积分到一个极限量级$M_\text{lim}=-11$。我们对星系逸出电离效率的测量结果与观测结果和大多数模型都大致吻合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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