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arXiv 2201.03885astro-ph.GAastro-ph.IM
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自我调节的星际介质中$X_{\rm CO}$对金属丰度、强度和空间尺度的依赖性

Dependence of $X_{\rm CO}$ on metallicity, intensity, and spatial scale in a self-regulated interstellar medium

Chia-Yu Hu, Andreas Schruba, Amiel Sternberg, Ewine F. van Dishoeck

摘要:

我们在高分辨率(~0.2 pc)流体动力学模拟中研究了CO(1-0)到H的$_2$转换因子($X_{\rm CO}$)和CO(2-1)到CO(1-0)的线比($R_{21}$)在宽范围的金属丰度($0.1 \leq Z/Z_\odot \leq 3$)中的自调节多相星际介质。我们通过辐射转移构建合成CO排放图,并系统地改变“观测”光束的大小来量化尺度依赖性。我们发现,kpc尺度的$X_{\rm CO}$可以高估在低$Z$,如果假设稳态化学或假设恒星形成气体是H $_2$为主。在秒差距尺度上,$X_{\rm CO}$因地而异,主要是由碳原子到CO的转变驱动的。一旦尘埃屏蔽生效,pc尺度的$X_{\rm CO}$就会下降到银河系的值$2\times 10^{20}\ {\rm cm^{-2}~(K~km~s^{-1})^{-1}}$,与$Z$无关。CO谱线在较低的$Z$处变得越来越光学薄,导致较高的$R_{21}$。大部分云区由高$X_{\rm CO}$和低$R_{21}$的扩散气体填充,而大部分CO排放来自低$X_{\rm CO}$和高$R_{21}$的稠密气体。采用一个常数$X_{\rm CO}$强烈过(欠)估计H $_2$在稠密(扩散)气体。线强度与$X_{\rm CO}$($R_{21}$)负(正)相关,因为它是柱密度(体积密度)的代表。在大尺度上,$X_{\rm CO}$和$R_{21}$由束平均决定,并且它们自然偏向于致密气体中的值。我们预测的$X_{\rm CO}$是$Z$、线强度和光束尺寸的多变量函数,其可用于更准确地推断H $_2$质量。

英文摘要:

We study the CO(1-0)-to-H$_2$ conversion factor ($X_{\rm CO}$) and the line ratio of CO(2-1)-to-CO(1-0) ($R_{21}$) across a wide range of metallicity ($0.1 \leq Z/Z_\odot \leq 3$) in high-resolution (~0.2 pc) hydrodynamical simulations of a self-regulated multiphase interstellar medium. We construct synthetic CO emission maps via radiative transfer and systematically vary the "observational" beam size to quantify the scale dependence. We find that the kpc-scale $X_{\rm CO}$ can be over-estimated at low $Z$ if assuming steady-state chemistry or assuming that the star-forming gas is H$_2$-dominated. On parsec scales, $X_{\rm CO}$ varies by orders of magnitude from place to place, primarily driven by the transition from atomic carbon to CO. The pc-scale $X_{\rm CO}$ drops to the Milky Way value of $2\times 10^{20}\ {\rm cm^{-2}~(K~km~s^{-1})^{-1}}$ once dust shielding becomes effective, independent of $Z$. The CO lines become increasingly optically thin at lower $Z$, leading to a higher $R_{21}$. Most cloud area is filled by diffuse gas with high $X_{\rm CO}$ and low $R_{21}$, while most CO emission originates from dense gas with low $X_{\rm CO}$ and high $R_{21}$. Adopting a constant $X_{\rm CO}$ strongly over- (under-)estimates H$_2$ in dense (diffuse) gas. The line intensity negatively (positively) correlates with $X_{\rm CO}$ ($R_{21}$) as it is a proxy of column density (volume density). On large scales, $X_{\rm CO}$ and $R_{21}$ are dictated by beam averaging, and they are naturally biased towards values in dense gas. Our predicted $X_{\rm CO}$ is a multivariate function of $Z$, line intensity, and beam size, which can be used to more accurately infer the H$_2$ mass.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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