论文标题

调查[C $ \,{\ rm \ scriptsize ii} $] - to-h $ \,{\ rm \ scriptsize i} $转换因子和H $ \,{\ rm \ rm \ rm \ scriptsize i} $ a s $ z \ y y 6 $ s $ z \ y hydrodynalnic simulations的气体预算

Investigating the [C$\,{\rm \scriptsize II}$]-to-H$\,{\rm \scriptsize I}$ conversion factor and the H$\,{\rm \scriptsize I}$ gas budget of galaxies at $z\approx 6$ with hydrodynamical simulations

论文作者

Vizgan, David, Heintz, Kasper E., Greve, Thomas R., Narayanan, Desika, Davé, Romeel, Olsen, Karen P., Popping, Gergö, Watson, Darach

论文摘要

星系中最基本的最基本的重型物质成分之一是中性原子氢(h $ \,{\ rm \ scriptsize i} $)。在低红移时,可以直接通过21厘米的过渡来追溯此组件,但是为了推断h $ \,{\ rm \ scriptsize i} $最遥远星系的气体含量,需要一个可行的示踪剂。我们在这里调查了($ ^2p_ {3/2} - ^2p_ {1/3} $)单人离子化的碳[C $ \,{\ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ rm \ scriptssize ii} $]的良好结构过渡的保险。在Heintz等人的工作之后,星系为$ z \ 6 $。 (2021)。我们从SIMBA模拟中选择了11,125个恒星形成的星系,并在Sigame框架内进行了后处理和建模的远红外线排放。我们在[C $ \,{\ rm \ scriptsize ii} $]和h $ \,{\ rm \ scriptsize i} $之间找到了一个牢固的联系,以及此[c $ \,{\ rm \ rm \ rm \ rm \ rm \ rm \ rm \ scriptsize ii} $] - [C \,{\ rm \ ScriptSize ii}]} $)与模拟星系的气相金属性抗相关。我们进一步使用这些仿真来预测星系的总重质物质含量约为$ z \ 6 $,尤其是HI气体质量分数。我们发现$ m _ {\ rm hi}/m _ \ star = 1.4 $的平均值和$ m _ {\ rm hi}/m _ {\ rm bar,tot} = 0.45 $。这些结果为H $ \,{\ rm \ Scriptsize i} $提供了有力的证据,是星系中质量为$ z \ 6 $的主要的Baryonic物质组成部分。

One of the most fundamental baryonic matter components of galaxies is the neutral atomic hydrogen (H$\,{\rm \scriptsize I}$). At low redshifts, this component can be traced directly through the 21-cm transition, but to infer H$\,{\rm \scriptsize I}$ gas content of the most distant galaxies, a viable tracer is needed. We here investigate the fidelity of the fine structure transition of the ($^2P_{3/2} - ^2P_{1/3}$) transition of singly-ionized carbon [C$\,{\rm \scriptsize II}$] at $158\,μ$m as a proxy for H$\,{\rm \scriptsize I}$ in a set simulated galaxies at $z\approx 6$, following the work by Heintz et al. (2021). We select 11,125 star-forming galaxies from the SIMBA simulations, with far-infrared line emissions post-processed and modeled within the SIGAME framework. We find a strong connection between [C$\,{\rm \scriptsize II}$] and H$\,{\rm \scriptsize I}$, with the relation between this [C$\,{\rm \scriptsize II}$]-to-H$\,{\rm \scriptsize I}$ relation ($β_{\rm [C\,{\rm \scriptsize II}]}$) being anti-correlated with the gas-phase metallicity of the simulated galaxies. We further use these simulations to make predictions for the total baryonic matter content of galaxies at $z\approx 6$, and specifically the HI gas mass fraction. We find mean values of $M_{\rm HI}/M_\star = 1.4$, and $M_{\rm HI}/M_{\rm bar,tot} = 0.45$. These results provide strong evidence for H$\,{\rm \scriptsize I}$ being the dominant baryonic matter component by mass in galaxies at $z\approx 6$.

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