利用流体力学模拟测试光环模型的热苏尼耶夫-泽尔多维奇功率谱

Emma Ayçoberry, Pranjal R. S., Karim Benabed, Yohan Dubois, Elisabeth Krause, Tim Eifler
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引用次数: 0

摘要

LSS的统计特性是约束宇宙学特性的有力工具。追踪气体压力,tSZ效应是质量分布的一个有偏差的探测器,可以用来测试反馈物理学或宇宙学模型。因此,为应用于 tSZ 勘测,建立可靠的热气体压力模型至关重要。由于气体坍缩到束缚结构中,预计大部分 tSZ 信号都在宇宙吸积冲击产生的光晕中。因此,可以使用简单的经验光晕模型来预测tSZ功率谱。在这项研究中,我们使用了HMx光环模型来比较tSZ功率谱与几种流体力学模拟的功率谱:Horizon套件和Magneticum模拟。我们研究了不同移位时对tSZ功率谱的各种贡献,包括一晕和二晕项分解、束缚气体量、不同质量的重要性以及电子压力曲线。我们对tSZ功率谱的比较发现,差异随着红移的增加而增大。我们发现在多极范围$ell=10^3-10^4$内,测量的和预测的tSZ角功率谱相差20%到50%。在更高的红移(z~3)下,模拟结果表明,来自virial半径外的功率比来自virial半径内的功率大,这表明光环模型的适用性受到了限制。尽管低红移时的 tSZ 功率谱与光环模型的默认校准结果相当一致,但我们还是观察到了压力谱的差异。总之,我们的研究表明,光环模型的特性需要与真实或模拟数据进行仔细对照,才能被证明对宇宙学有用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Testing the thermal Sunyaev-Zel'dovich power spectrum of a halo model using hydrodynamical simulations
Statistical properties of LSS serve as powerful tools to constrain the cosmological properties of our Universe. Tracing the gas pressure, the tSZ effect is a biased probe of mass distribution and can be used to test the physics of feedback or cosmological models. Therefore, it is crucial to develop robust modeling of hot gas pressure for applications to tSZ surveys. Since gas collapses into bound structures, it is expected that most of the tSZ signal is within halos produced by cosmic accretion shocks. Hence, simple empirical halo models can be used to predict the tSZ power spectra. In this study, we employed the HMx halo model to compare the tSZ power spectra with those of several hydrodynamical simulations: the Horizon suite and the Magneticum simulation. We examined various contributions to the tSZ power spectrum across different redshifts, including the one- and two-halo term decomposition, the amount of bound gas, the importance of different masses and the electron pressure profiles. Our comparison of the tSZ power spectrum reveals discrepancies that increase with redshift. We find a 20% to 50% difference between the measured and predicted tSZ angular power spectrum over the multipole range $\ell=10^3-10^4$. Our analysis reveals that these differences are driven by the excess of power in the predicted two-halo term at low k and in the one-halo term at high k. At higher redshifts (z~3), simulations indicate that more power comes from outside the virial radius than from inside suggesting a limitation in the applicability of the halo model. We observe differences in the pressure profiles, despite the fair level of agreement on the tSZ power spectrum at low redshift with the default calibration of the halo model. In conclusion, our study suggests that the properties of the halo model need to be carefully controlled against real or mock data to be proven useful for cosmological purposes.
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