Emma Ayçoberry, Pranjal R. S., Karim Benabed, Yohan Dubois, Elisabeth Krause, Tim Eifler
{"title":"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","authors":"Emma Ayçoberry, Pranjal R. S., Karim Benabed, Yohan Dubois, Elisabeth Krause, Tim Eifler","doi":"arxiv-2409.11472","DOIUrl":null,"url":null,"abstract":"Statistical properties of LSS serve as powerful tools to constrain the\ncosmological properties of our Universe. Tracing the gas pressure, the tSZ\neffect is a biased probe of mass distribution and can be used to test the\nphysics of feedback or cosmological models. Therefore, it is crucial to develop\nrobust modeling of hot gas pressure for applications to tSZ surveys. Since gas\ncollapses into bound structures, it is expected that most of the tSZ signal is\nwithin halos produced by cosmic accretion shocks. Hence, simple empirical halo\nmodels can be used to predict the tSZ power spectra. In this study, we employed\nthe HMx halo model to compare the tSZ power spectra with those of several\nhydrodynamical simulations: the Horizon suite and the Magneticum simulation. We\nexamined various contributions to the tSZ power spectrum across different\nredshifts, including the one- and two-halo term decomposition, the amount of\nbound gas, the importance of different masses and the electron pressure\nprofiles. Our comparison of the tSZ power spectrum reveals discrepancies that\nincrease with redshift. We find a 20% to 50% difference between the measured\nand predicted tSZ angular power spectrum over the multipole range\n$\\ell=10^3-10^4$. Our analysis reveals that these differences are driven by the\nexcess of power in the predicted two-halo term at low k and in the one-halo\nterm at high k. At higher redshifts (z~3), simulations indicate that more power\ncomes from outside the virial radius than from inside suggesting a limitation\nin the applicability of the halo model. We observe differences in the pressure\nprofiles, despite the fair level of agreement on the tSZ power spectrum at low\nredshift with the default calibration of the halo model. In conclusion, our\nstudy suggests that the properties of the halo model need to be carefully\ncontrolled against real or mock data to be proven useful for cosmological\npurposes.","PeriodicalId":501207,"journal":{"name":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","volume":"214 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Testing the thermal Sunyaev-Zel'dovich power spectrum of a halo model using hydrodynamical simulations\",\"authors\":\"Emma Ayçoberry, Pranjal R. S., Karim Benabed, Yohan Dubois, Elisabeth Krause, Tim Eifler\",\"doi\":\"arxiv-2409.11472\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Statistical properties of LSS serve as powerful tools to constrain the\\ncosmological properties of our Universe. Tracing the gas pressure, the tSZ\\neffect is a biased probe of mass distribution and can be used to test the\\nphysics of feedback or cosmological models. Therefore, it is crucial to develop\\nrobust modeling of hot gas pressure for applications to tSZ surveys. Since gas\\ncollapses into bound structures, it is expected that most of the tSZ signal is\\nwithin halos produced by cosmic accretion shocks. Hence, simple empirical halo\\nmodels can be used to predict the tSZ power spectra. In this study, we employed\\nthe HMx halo model to compare the tSZ power spectra with those of several\\nhydrodynamical simulations: the Horizon suite and the Magneticum simulation. We\\nexamined various contributions to the tSZ power spectrum across different\\nredshifts, including the one- and two-halo term decomposition, the amount of\\nbound gas, the importance of different masses and the electron pressure\\nprofiles. Our comparison of the tSZ power spectrum reveals discrepancies that\\nincrease with redshift. We find a 20% to 50% difference between the measured\\nand predicted tSZ angular power spectrum over the multipole range\\n$\\\\ell=10^3-10^4$. Our analysis reveals that these differences are driven by the\\nexcess of power in the predicted two-halo term at low k and in the one-halo\\nterm at high k. At higher redshifts (z~3), simulations indicate that more power\\ncomes from outside the virial radius than from inside suggesting a limitation\\nin the applicability of the halo model. We observe differences in the pressure\\nprofiles, despite the fair level of agreement on the tSZ power spectrum at low\\nredshift with the default calibration of the halo model. In conclusion, our\\nstudy suggests that the properties of the halo model need to be carefully\\ncontrolled against real or mock data to be proven useful for cosmological\\npurposes.\",\"PeriodicalId\":501207,\"journal\":{\"name\":\"arXiv - PHYS - Cosmology and Nongalactic Astrophysics\",\"volume\":\"214 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Cosmology and Nongalactic Astrophysics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.11472\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11472","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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.