The halo mass dependence of physical and observable properties in the circumgalactic medium

Andrew W. S. Cook, Freeke van de Voort, Rüdiger Pakmor, Robert J. J. Grand
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Abstract

We study the dependence of the physical and observable properties of the CGM on its halo mass. We analyse 22 simulations from the Auriga suite of high resolution cosmological `zoom-in' simulations at $z=0$ with halo masses $10^{10}~\text{M}_{\odot}\leq\text{M}_{\mathrm{200c}}\leq10^{12}~\text{M}_{\odot}$. We find a larger scatter in temperature and smaller scatter in metallicity in more massive haloes. The scatter of temperature and metallicity as a function of radius increases out to larger radii. The median and scatter of the volume-weighted density and mass-weighted radial velocity show no significant dependence on halo mass. Our results highlight that the CGM is more multiphase in haloes of higher mass. We additionally investigate column densities for HI and the metal ions CIV, OVI, MgII and SiII as a function of stellar mass and radius. We find the HI and metal ion column densities increase with stellar mass at sufficiently large radii ($R\gtrsim{0.2}$R$_{\mathrm{200c}}$). We find good agreement between our HI column densities and observations outside $20$% of the virial radius and overpredict within $20$%. MgII and SiII are similarly overpredicted within $20$% of the virial radius, but drop off steeply at larger radii. Our OVI column densities underpredict observations for stellar masses between $10^{9.7}~\text{M}_{\odot}\leq\text{M}_{\star}<10^{10.8}~\text{M}_{\odot}$ with reasonable agreement at $10^{10.8}~\text{M}_{\odot}$. CIV column densities agree with observational detections above a halo mass of $10^{9.7}~\text{M}_{\odot}$. We find that OVI (MgII) traces the highest (lowest) temperatures, and lowest (highest) density and metallicity. OVI and CIV are photo-ionized (collisionally ionized) at low (high) halo masses with a transition to higher temperatures at $10^{11}~\text{M}_{\odot}$. However, there is no clear trend for the radial velocity of the ions.
环银河介质中物理和可观测特性的晕质量依赖性
我们研究了 CGMon 的物理和可观测特性与光环质量的关系。我们分析了Auriga高分辨率宇宙学 "放大 "模拟套件中的22个模拟,模拟的光环质量为$10^{10}~\text{M}_\{odot}\leq\text{M}_\{mathrm{200c}}\leq10^{12}~\text{M}_{\odot}$。温度和金属性的散度与半径的函数关系在半径越大时越大。体积加权密度和质量加权径向速度的中值和散度与光环质量没有明显的关系。我们的结果表明,在质量较大的光环中,CGM的多相性更强。我们还研究了HI和金属离子CIV、OVI、MgII和SiII的柱密度与恒星质量和半径的函数关系。我们发现在足够大的半径($R/gtrsim{0.2}$R$_{\mathrm{200c}}$)下,HI 和金属离子柱密度随着恒星质量的增加而增加。我们发现,在新星半径的 20% 以外,我们的 HI 柱密度与观测结果非常吻合,而在 20% 以内,则预测过高。MgII和SiII在半径的20%范围内也同样被高估了,但在较大的半径范围内则急剧下降。对于质量在10^{9.7}~text/{M}_{\odot}\leq/text{M}_{star}<10^{10.8}~text/{M}_{\odot}$之间的恒星,我们的OVI柱密度低于观测值,而在10^{10.8}~text/{M}_{\odot}$时,我们的OVI柱密度与观测值保持合理一致。CIV柱密度与高于10^{9.7}~text/{M}_{/odot}$光环质量的观测探测结果一致。我们发现,OVI(MgII)的温度最高(最低),密度和金属性最低(最高)。OVI和CIV在低(高)光晕质量时被光电离(碰撞电离),在10^{11}~text{M}_{\odot}$时过渡到较高温度。然而,离子的径向速度并没有明显的变化趋势。
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