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

Lewis, Joseph S. W., Ocvirk, Pierre, Aubert, Dominique, Sorce, Jenny G., Shapiro, Paul R., Deparis, Nicolas, Dawoodbhoy, Taha, Teyssier, Romain, Yepes, Gustavo, Gottlöber, Stefan, Ahn, Kyungjin, Iliev, Ilian T., Chardin, Jonathan

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.

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