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Halo Mass-concentration Relation at the High-mass End

Authors :
Eric Jullo
Ginevra Favole
Jean-Paul Kneib
Ran Li
Huanyuan Shan
Weiwei Xu
Chunxiang Wang
Linhua Jiang
Chaoli Zhang
Laboratoire d'Astrophysique de Marseille (LAM)
Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Aix Marseille Université (AMU)-Centre National d'Études Spatiales [Toulouse] (CNES)
Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)
Source :
Astrophys.J., Astrophys.J., 2021, 922 (2), pp.162. ⟨10.3847/1538-4357/ac1b9e⟩
Publication Year :
2021
Publisher :
HAL CCSD, 2021.

Abstract

The concentration-mass (c-M) relation encodes the key information of the assembly history of the dark matter halos, however its behavior at the high mass end has not been measured precisely in observations yet. In this paper, we report the measurement of halo c-M relation with galaxy-galaxy lensing method, using shear catalog of the Dark Energy Camera Legacy Survey (DECaLS) Data Release 8, which covers a sky area of 9500 deg^2. The foreground lenses are selected from redMaPPer, LOWZ, and CMASS catalogs, with halo mass range from 10^{13} to 10^{15} M_sun and redshift range from z=0.08 to z=0.65. We find that the concentration decreases with the halo mass from 10^{13} to 10^{14} M_sun, but shows a trend of upturn after the pivot point of ~10^{14} M_sun. We fit the measured c-M relation with the concentration model c(M)=C_0 (M/(10^{12} M_sun/h)^{-��} [1+(M/M_0)^{0.4}], and get the values (C_0, ��, log(M_0) = (5.119_{-0.185}^{0.183}, 0.205_{-0.010}^{0.010}, 14.083_{-0.133}^{0.130}), and (4.875_{-0.208}^{0.209}, 0.221_{-0.010}^{0.010}, 13.750_{-0.141}^{0.142}) for halos with 0.08<br />12 pages, 5 figures, accepted by ApJ

Details

Language :
English
Database :
OpenAIRE
Journal :
Astrophys.J., Astrophys.J., 2021, 922 (2), pp.162. ⟨10.3847/1538-4357/ac1b9e⟩
Accession number :
edsair.doi.dedup.....9c9b8e51eadc03efba1078a5b483f801
Full Text :
https://doi.org/10.3847/1538-4357/ac1b9e⟩