论文标题

用星系和活性银河核电归因于

Reionization with galaxies and active galactic nuclei

论文作者

Dayal, Pratika, Volonteri, Marta, Choudhury, Tirthankar Roy, Schneider, Raffaella, Trebitsch, Maxime, Gnedin, Nickolay Y., Atek, Hakim, Hirschmann, Michaela, Reines, Amy

论文摘要

在这项工作中,我们调查了高红移宇宙中恢复了层间介质(IGM)的来源的特性。使用旨在在宇宙的第一个1.5 GYR中重现星系和黑洞的半分析模型,我们重新审视了可以逃脱到IgM中的电离光子中恒星形成和黑洞积聚的相对作用。恒星形成和黑洞的积聚都受超新星反馈的调节,导致黑洞积聚在低质量晕圈中。我们探索了从两个星形形成($ \ langle f _ {\ rm eSc}^{\ rm sf}^{\ rm sf} \ rm sf} \ rangle $)和agn($ f _ {$ rm rm rm rm rm rm rm}^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^i,电离预算由低恒星质量($ m _* <10^9 {\ rm m_ \ odot} $)的星系归为主导m_ \ odot} $星系)在较低的红移; (ii)对于与观察到的电源约束的模型相匹配的累积电离发射率的AGN仅为$ z = 4 $贡献$ 10-25 \%$; (iii)如果$ \ langle f _ {\ rm Esc}^{\ rm sf} \ rangle $的恒星质量依赖性比$ f _ {\ rm eSc}^{\ rm eSc}^{\ rm bh} $较浅(iv)过渡恒星质量随着红移的减少而减小。当Agn以$ z \ sim 6.8 $为单位的逃脱的发射率在恒星质量功能的膝盖上方,但它们在恒星群众中占据了膝盖质量的十分之一,$ z = 4 $。

In this work we investigate the properties of the sources that reionized the intergalactic medium (IGM) in the high-redshift Universe. Using a semi-analytical model aimed at reproducing galaxies and black holes in the first 1.5 Gyr of the Universe, we revisit the relative role of star formation and black hole accretion in producing ionizing photons that can escape into the IGM. Both star formation and black hole accretion are regulated by supernova feedback, resulting in black hole accretion being stunted in low-mass halos. We explore a wide range of combinations for the escape fraction of ionizing photons (redshift-dependent, constant and scaling with stellar mass) from both star formation ($\langle f_{\rm esc}^{\rm sf} \rangle$) and AGN ($f_{\rm esc}^{\rm bh}$) to find: (i) the ionizing budget is dominated by stellar radiation from low stellar mass ($M_*<10^9 {\rm M_\odot}$ ) galaxies at $z>6$ with the AGN contribution (driven by $M_{bh}>10^6 {\rm M_\odot}$ black holes in $M_* > 10^9 {\rm M_\odot}$ galaxies) dominating at lower redshifts; (ii) AGN only contribute $10-25\%$ to the cumulative ionizing emissivity by $z=4$ for the models that match the observed reionization constraints; (iii) if the stellar mass dependence of $\langle f_{\rm esc}^{\rm sf} \rangle$ is shallower than $f_{\rm esc}^{\rm bh}$, at $z<7$ a transition stellar mass exists above which AGN dominate the escaping ionizing photon production rate; (iv) the transition stellar mass decreases with decreasing redshift. While AGN dominate the escaping emissivity above the knee of the stellar mass function at $z \sim 6.8$, they take-over at stellar masses that are a tenth of the knee mass by $z=4$.

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