论文标题

现代宇宙流体动力模拟中的星系冷气含量

Galaxy Cold Gas Contents in Modern Cosmological Hydrodynamic Simulations

论文作者

Davé, Romeel, Crain, Robert A., Stevens, Adam R. H., Narayanan, Desika, Saintonge, Amelie, Catinella, Barbara, Cortese, Luca

论文摘要

我们介绍了三个最近的宇宙流体动力学模拟(Simba,Eagle和Illustris-tng)中星系原子和分子气体性能的比较,而与$ z \ sim 0-2 $的观测值相比。 These simulations all rely on similar sub-resolution prescriptions to model cold interstellar gas which they cannot represent directly, and qualitatively reproduce the observed $z\approx 0$ HI and H$_2$ mass functions (HIMF, H2MF), CO(1-0) luminosity functions (COLF), and gas scaling relations versus stellar mass, specific star formation rate, and stellar surface density $μ_*$, with some定量差异。为了与COLF相比,我们根据其平均分子表面密度和金属性将h $ _2 $ -to的转换因子应用于模拟星系,从而在$α_ {\ rm co} $中产生实质性变化,并且模型之间的显着差异。使用此情况,预测的$ z = 0 $ colfs与数据比预测的H2MF更好一致。到$ z \ sim 2 $,Eagle's和Simba的Himf和Colf强烈增加,而TNG的HIMF下降,COLF的发展缓慢。 Eagle和Simba在$ z \ sim 1-2 $上以$ z \ sim 1-2 $的形式重现高$ l _ {\ rm co1-0} $ galaxies,部分原因是中间$α_ {\ rm co}(z = 2)\ sim 1 $ vers $ vers $ vers $ vers $α_ {\ rm co}(\ rm co}(z = 0)\ sim \ sim 3 $ 3 $ 3 $。在所有型号中,检查\ hi,h $ _2 $和CO缩放关系,它们具有$ M _*$的趋势是广泛复制的,但是在绿色谷星系中,Eagle在大型星系中的TNG和Simba在绿色谷星系,TNG和SIMBA过度生产冷气,而SIMBA过度生产冷气,SIMBA在小型系统中产生了分子气体。 Using Simba variants that exclude individual AGN feedback modules, we find that Simba's AGN jet feedback is primarily responsible by lowering cold gas contents from $z\sim 1\to0$ by suppressing cold gas in $M_*> 10^{10}{\rm M}_\odot$ galaxies, while X-ray feedback suppresses the formation of high-$μ_*$ systems.

We present a comparison of galaxy atomic and molecular gas properties in three recent cosmological hydrodynamic simulations, Simba, EAGLE, and Illustris-TNG, versus observations from $z\sim 0-2$. These simulations all rely on similar sub-resolution prescriptions to model cold interstellar gas which they cannot represent directly, and qualitatively reproduce the observed $z\approx 0$ HI and H$_2$ mass functions (HIMF, H2MF), CO(1-0) luminosity functions (COLF), and gas scaling relations versus stellar mass, specific star formation rate, and stellar surface density $μ_*$, with some quantitative differences. To compare to the COLF, we apply an H$_2$-to-CO conversion factor to the simulated galaxies based on their average molecular surface density and metallicity, yielding substantial variations in $α_{\rm CO}$ and significant differences between models. Using this, predicted $z=0$ COLFs agree better with data than predicted H2MFs. Out to $z\sim 2$, EAGLE's and Simba's HIMF and COLF strongly increase, while TNG's HIMF declines and COLF evolves slowly. EAGLE and Simba reproduce high $L_{\rm CO1-0}$ galaxies at $z\sim 1-2$ as observed, owing partly to a median $α_{\rm CO}(z=2)\sim 1$ versus $α_{\rm CO}(z=0)\sim 3$. Examining \HI, H$_2$, and CO scaling relations, their trends with $M_*$ are broadly reproduced in all models, but EAGLE yields too little HI in green valley galaxies, TNG and Simba overproduce cold gas in massive galaxies, and Simba overproduces molecular gas in small systems. Using Simba variants that exclude individual AGN feedback modules, we find that Simba's AGN jet feedback is primarily responsible by lowering cold gas contents from $z\sim 1\to0$ by suppressing cold gas in $M_*> 10^{10}{\rm M}_\odot$ galaxies, while X-ray feedback suppresses the formation of high-$μ_*$ systems.

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