期刊
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
卷 500, 期 2, 页码 1806-1816出版社
OXFORD UNIV PRESS
DOI: 10.1093/mnras/staa3369
关键词
gravitational lensing: weak; cosmic background radiation; large-scale structure of Universe
资金
- Chinese Academy of Sciences (CAS) Strategic Priority Research Program [XDA15020200]
- NSFC-ISF [11761141012]
- CAS Interdisciplinary Innovation Team
- European Union [797794]
- [NRF-120385]
- [NRF-120378]
- [NSFC-11828301]
- [NSFC-11822305]
- [NSFC-11773031]
- [NSFC-11633004]
- Marie Curie Actions (MSCA) [797794] Funding Source: Marie Curie Actions (MSCA)
The study compared the universal pressure profile (UPP) with measurements of the thermal Sunyaev-Zeldovich (tSZ) effect and weak gravitational lensing, finding consistent UPP parameters under fixed cosmology. The most constrained parameters were the pressure profile concentration c(500) and shape index alpha.
We confront the universal pressure profile (UPP) proposed. with the recent measurement of the cross-correlation function of the thermal Sunyaev-Zeldovich (tSZ) effect from Planck and weak gravitational lensing measurement from the Red Cluster Sequence Lensing Survey. By using the halo model, we calculate the prediction of xi(y-kappa) (lensing convergence and Compton-y parameter) and xi(y-gamma t) (lensing shear and Compton-y parameter) and fit the UPP parameters by using the observational data. We find consistent UPP parameters when fixing the cosmology to either WMAP 9-yr or Planck 2018 best-fitting values. The best constrained parameter is the pressure profile concentration c(500) = r(500)/r(s), for which we find c(500) = 2.68(-0.96)(+1.46) (WMAP-9) and c(500) = 1.91(-0.65)(+1.07) (Planck-2018) for the xi(y-gamma t) estimator. The shape index for the intermediate radius region alpha parameter is constrained to alpha = 1.75(-0.77)(+1.29) and alpha = 1.65(-0.5)(+0.74) for WMAP-9 and Planck-2018 cosmologies, respectively. Propagating the uncertainties of the UPP parameters to pressure profiles results in a factor of 3 uncertainty in the shape and magnitude. Further investigation shows that most of the signal of the cross-correlation comes from the low-redshift, inner halo profile (r <= r(vir)/2) with halo mass in the range of 10(14)-10(15)M(circle dot), suggesting that this is the major regime that constitutes the cross-correlation signal between weak lensing and tSZ.
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