论文标题

Simba中环乳介质吸收器的物理性质

The Physical Nature of Circumgalactic Medium Absorbers in Simba

论文作者

Appleby, Sarah, Davé, Romeel, Sorini, Daniele, Cui, Weiguang, Christiansen, Jacob

论文摘要

我们研究了SIMBA宇宙学模拟中低红速CGM的性质,这些图是由紫外线吸收线所追踪的,在星体块($ m_ \ star> 10^{10} {10} m_ \ odot $)的星形,Green Valley,Green Valley和Quenched Galaxies at Impact Pameters $ r_ per_ pep pep \ pep pep pleq eq 1.25.25.25.25.25.我们为HI,MGII,CII,SIIII,CIV和OVI生成合成光谱,适合VOIGT曲线以获得线路性能,并估算吸收气体的密度,温度和金属性。我们发现,CGM吸收剂周围最丰富,售价为$ M_ \ star <10^{11} M_ \ ODOT $,而绿色谷的丰富度则表现出与淬火星系的行为相似,表明在恒星形成之前,CGM“ QGM”停止。 HI吸收气体存在于广泛的宇宙相(凝结气体,弥漫性气体,热光晕气和热热层间培养基)中,而基本上所有低离世金属吸收都来自冷凝的气体。 OVI吸收器在热光晕气和异想天开之间分配。碰撞电离的CGM吸收器的比例为$ \ sim 25-55 \%$,OVI的$ \ sim 80-95 \%$,具体取决于出色的质量和影响参数。通常,每个离子的最高柱密度吸收特征来自致密气体。卫星气体定义为$ 10R_ {1/2,\ star},$贡献$ \ sim 3 \%$的整体HI吸收,但$ \ sim 30 \%的MGII吸收,卫星的分数随着电离激发的增加而减少。

We study the nature of the low-redshift CGM in the Simba cosmological simulations as traced by ultraviolet absorption lines around galaxies in bins of stellar mass ($M_\star>10^{10}M_\odot$) for star-forming, green valley and quenched galaxies at impact parameters $r_\perp\leq 1.25r_{200}$. We generate synthetic spectra for HI, MgII, CII, SiIII, CIV, and OVI, fit Voigt profiles to obtain line properties, and estimate the density, temperature, and metallicity of the absorbing gas. We find that CGM absorbers are most abundant around star forming galaxies with $M_\star < 10^{11}M_\odot$, while the abundance of green valley galaxies show similar behaviour to those of quenched galaxies, suggesting that the CGM "quenches" before star formation ceases. HI absorbing gas exists across a broad range of cosmic phases (condensed gas, diffuse gas, hot halo gas and Warm-Hot Intergalactic Medium), while essentially all low-ionisation metal absorption arises from condensed gas. OVI absorbers are split between hot halo gas and the WHIM. The fraction of collisionally ionised CGM absorbers is $\sim 25-55\%$ for CIV and $\sim 80-95\%$ for OVI, depending on stellar mass and impact parameter. In general, the highest column density absorption features for each ion arise from dense gas. Satellite gas, defined as that within $10r_{1/2,\star},$ contributes $\sim 3\%$ of overall HI absorption but $\sim 30\%$ of MgII absorption, with the fraction from satellites decreasing with increasing ion excitation energy.

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