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arXiv 2403.09476astro-ph.GA
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来自$L^*$星系的Sunyaev-Zeldovich信号:观测、解析与模拟

Sunyaev-Zeldovich Signals from $L^*$ Galaxies: Observations, Analytics, and Simulations

Yossi Oren, Amiel Sternberg, Christopher F. McKee, Yakov Faerman, Shy Genel

AI总结:

本研究通过多套CGM模型、新幂律模型及TNG100模拟分析$L^*$星系热SZ效应观测数据,约束了CGM物理参数,验证观测一致性并指出模拟的反馈与气体损失设定偏高。

摘要:

我们分析了Bregman等人2022年与Das等人2023年报道的、产生于$L^*$星系周介质(CGM)的热Sunyaev-Zeldovich(tSZ)效应的测量结果。分析中我们使用了Faerman等人2017年和2020年的CGM模型、一种新的幂律模型(PLM)以及TNG100模拟。对于给定的$M_{\rm vir}$(位力质量),我们的PLM包含四个参数:热CGM气体中的晕重子质量占比$f_{\rm hCGM}$、位力半径处实际气体温度与位力温度的比值$\phi_T$,以及热电子压强和氢核子密度的幂律指数$a_{P,{\rm th}}$与$a_n$。\n\nB+22的康普顿-$y$剖面意味着陡峭的电子压强斜率($a_{P,{\rm th}}\simeq 2$)。在等温条件下,温度至少为$1.1\times 10^6$ K,对于位力质量为$2.75\times 10^{12}$ M$_\odot$的系统,热CGM气体质量最高可达$3.5\times 10^{11}$ M$_\odot$。然而,若气体呈等温状态,则必然正在向外膨胀离开晕。研究更支持等熵物态方程,该方程下流体静力学平衡是可行的。\n\nB+22与D+23的结果彼此一致,也与Zhang等人2024年对银河系质量系统开展的近期(0.5-2 keV)CGM X射线观测结果相符。对于$M_{\rm vir}\simeq 3\times 10^{12}$ M$_\odot$的系统,三组观测得到的标度康普顿压强积分$E(z)^{-2/3}Y_{500}/M_{\rm vir,12}^{5/3}$均处于$2.5\times 10^{-4}$至$5.0\times 10^{-4}$ kpc$^2$的窄范围内。TNG100模拟对$L^*$星系的tSZ参数预测值偏低约0.5 dex,表明在该质量尺度下,模拟晕中的反馈强度和CGM气体损失被高估了。

英文摘要:

We analyze measurements of the thermal Sunyaev-Zeldovich (tSZ) effect arising in the circumgalactic medium (CGM) of $L^*$ galaxies, reported by Bregman et al. 2022 and Das et al. 2023. In our analysis we use the Faerman et al. 2017 and Faerman et al. 2020 CGM models, a new power-law model (PLM), and the TNG100 simulation. For a given $M_{\rm vir}$, our PLM has four parameters; the fraction, $f_{\rm hCGM}$, of the halo baryon mass in hot CGM gas, the ratio, $ϕ_T$, of the actual gas temperature at the virial radius to the virial temperature, and the power-law indicies, $a_{P,{\rm th}}$ and $a_n$ for the thermal electron pressure and the hydrogen nucleon density. The B+22 Compton-$y$ profile implies steep electron pressure slopes ($a_{P,{\rm th}}\simeq 2$). For isothermal conditions the temperature is at least $1.1\times 10^6$ K, with a hot CGM gas mass of up to $3.5\times 10^{11}$ M$_\odot$ for a virial mass of $2.75\times 10^{12}$ M$_\odot$. However, if isothermal the gas must be expanding out of the halos. An isentropic equation of state is favored for which hydrostatic equilibrium is possible. The B+22 and D+23 results are consistent with each other and with recent (0.5-2 keV) CGM X-ray observations by Zhang et al. 2024 of Milky Way mass systems. For $M_{\rm vir}\simeq 3\times 10^{12}$ M$_\odot$, the scaled Compton pressure integrals, $E(z)^{-2/3}Y_{500}/M_{\rm vir,12}^{5/3}$, lie in the narrow range, $2.5\times 10^{-4}$ to $5.0\times 10^{-4}$ kpc$^2$, for all three sets of observations. TNG100 underpredicts the tSZ parameters by factors $\sim 0.5$ dex for the $L^*$ galaxies, suggesting that the feedback strengths and CGM gas losses are overestimated in the simulated halos at these mass scales.

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