论文标题
在宇宙黎明II模拟中,在回报时期期间的银河电离光子预算
Galactic ionising photon budget during the Epoch of Reionisation in the Cosmic Dawn II simulation
论文作者
论文摘要
Cosmic Dawn ("CoDa") II yields the first statistically-meaningful determination of the relative contribution to reionization by galaxies of different halo mass, from a fully-coupled radiation-hydrodynamics simulation of the epoch of reionization large enough ($\sim$ 100 Mpc) to model global reionization while resolving the formation of all galactic halos above $\sim 10^8 M_\odot$.高质量光环内的细胞传输是双模式的 - 电离细胞是透明的,而中性细胞吸收了其恒星产生的光子 - 晕圈逃脱分数$ f_ {ESC} $反映了这些模式之间的恒星形成速率(“ SFR”)的平衡。后者在较高的光环质量下越来越普遍,驱动了$ f_ {esc} $(我们为结果提供了分析拟合),而Halo Essce逃脱光度与$ f_ {Esc} \ times $ sfr成正比,随质量的增加。带有深色物质质量的光环在$ 6.10^{8} m_ \ odot <m_h <3.10^{10} m_ \ odot $ caparity $ \ sim 80 $ \ sim 80 $ \ sim 80 $%在z = 7处逃脱的光子,当宇宙被50%离子化时,使它们成为宇宙抗离数的主要动力。尽管$ f_ {esc} $,但较少的光环虽然虽然较少,但虽然数量却较少,但占光子预算的贡献不到10%。高质量光环太少,太不透明了,尽管SFR较高,但贡献了$ <10美元。在较高(下)红移时,主要的质量范围为较低(较高),因为质量功能和电离一起进展(例如,在z $ = 8.5 $,x $ _ {\ rm hi} = 0.9 $,$ m_h <5.10^9 m_ \ odot $ haloes $ \ sim $ \ sim $ 80%)。带有紫外线大小的星系$ m_ {ab1600} $介于$ -12 $和$ -19 $之间的$ = 6 $和8之间的统治回去。
Cosmic Dawn ("CoDa") II yields the first statistically-meaningful determination of the relative contribution to reionization by galaxies of different halo mass, from a fully-coupled radiation-hydrodynamics simulation of the epoch of reionization large enough ($\sim$ 100 Mpc) to model global reionization while resolving the formation of all galactic halos above $\sim 10^8 M_\odot$. Cell transmission inside high-mass haloes is bi-modal -- ionized cells are transparent, while neutral cells absorb the photons their stars produce - and the halo escape fraction $f_{esc}$ reflects the balance of star formation rate ("SFR") between these modes. The latter is increasingly prevalent at higher halo mass, driving down $f_{esc}$ (we provide analytical fits to our results), whereas halo escape luminosity, proportional to $f_{esc} \times$SFR, increases with mass. Haloes with dark matter masses within $6.10^{8} M_\odot < M_h < 3.10^{10} M_\odot$ produce $\sim 80$% of the escaping photons at z=7, when the Universe is 50% ionized, making them the main drivers of cosmic reionization. Less massive haloes, though more numerous, have low SFRs and contribute less than 10% of the photon budget then, despite their high $f_{esc}$. High mass haloes are too few and too opaque, contributing $<10$% despite their high SFRs. The dominant mass range is lower (higher) at higher (lower) redshift, as mass function and reionization advance together (e.g. at z$=8.5$, x$_{\rm HI}=0.9$, $M_h < 5.10^9 M_\odot$ haloes contributed $\sim$80%). Galaxies with UV magnitudes $M_{AB1600}$ between $-12$ and $-19$ dominated reionization between z$=6$ and 8.