2024A&A...692A.253L


Query : 2024A&A...692A.253L

2024A&A...692A.253L - Astronomy and Astrophysics, volume 692A253 (2024/12-1)

Gas thermodynamics meets galaxy kinematics: Joint mass measurements for eROSITA galaxy clusters.

LI P., LIU A., KLUGE M., COMPARAT J., TIAN Y., JULIO M.P., PAWLOWSKI M.S., SANDERS J., BULBUL E., SCHWOPE A., GHIRARDINI V., ZHANG X., BAHAR Y.E., RAMOS-CEJA M.E., BALZER F. and GARREL C.

Abstract (from CDS):

The mass of galaxy clusters is a critical quantity for probing cluster cosmology and testing theories of gravity, but its measurement could be biased, given that assumptions are inevitable in order to make use of any approach. In this paper, we employ and compare two mass proxies for galaxy clusters: thermodynamics of the intracluster medium and kinematics of member galaxies. We selected 22 galaxy clusters from the cluster catalog in the first SRG/eROSITA All-Sky Survey (eRASS1) that have sufficient optical and near-infrared observations. We generated multiband images in the energy range of (0.3, 7) keV for each cluster, and derived their temperature profiles, gas mass profiles, and hydrostatic mass profiles using a parametric approach that does not assume dark matter halo models. With spectroscopically confirmed member galaxies collected from multiple surveys, we numerically solved the spherical Jeans equation for their dynamical mass profiles. Our results quantify the correlation between dynamical mass and the line-of-sight velocity dispersion, log Mdyn = (1.296 ± 0.001)log(σlos2rproj/G)-(3.87 ± 0.23), with a root mean square (rms) scatter of 0.14 dex. We find that the two mass proxies lead to roughly the same total mass, with no observed systematic bias. As such, the σ8 tension is not specific to hydrostatic mass or weak lensing shears, but also appears with galaxy kinematics. Interestingly, the hydrostatic-to-dynamical mass ratios decrease slightly toward large radii, which could possibly be evidence for accreting galaxies in the outskirts. We also compared our hydrostatic masses with the latest weak lensing masses inferred with scaling relations. The comparison shows that the weak lensing mass is significantly higher than our hydrostatic mass by ∼110%. This might explain the significantly larger value of σ8 from the latest measurement using eRASS1 clusters than almost all previous estimates in the literature. Finally, we tested the radial acceleration relation established in disk galaxies. We confirm the missing baryon problem in the inner region of galaxy clusters using three independent mass proxies for the first time. As ongoing and planned surveys are providing deeper X-ray observations and more galaxy spectra for cluster members, we expect to extend the study to cluster outskirts in the near future.

Abstract Copyright: © The Authors 2024

Journal keyword(s): galaxies: clusters: general - galaxies: clusters: intracluster medium - cosmology: observations - dark matter - X-rays: galaxies: clusters

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ACT-CL J0040.8-4407 ClG 00 40 49.9 -44 07 50           ~ 43 0
2 ACO 2811 ClG 00 42 08.82 -28 32 08.8           ~ 78 0
3 ACT-CL J0243.5-4833 ClG 02 43 38.873 -48 33 38.94           ~ 26 0
4 ACT-CL J0346.9-5438 ClG 03 46 55.50 -54 38 54.8           ~ 33 0
5 ACT-CL J0438.2-5419 ClG 04 38 17.70 -54 19 20.7           ~ 78 0
6 ACT-CL J0528-5259 ClG 05 28 05.30 -52 59 52.8           ~ 52 0
7 ACT-CL J0559.7-5249 ClG 05 59 43.20 -52 49 27.1           ~ 63 0
8 ACO 586 ClG 07 32 20.3 +31 37 58           ~ 196 0
9 ACO 590 ClG 07 37 29 +35 16.2           ~ 6 0
10 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 275 0
11 ACO 657 ClG 08 23 37.04 +15 57 09.1           ~ 17 0
12 ACO 697 ClG 08 42 57.6 +36 21 45           ~ 277 0
13 eFEDS J090131.1+030056 ClG 09 01 31.2 +03 00 57           ~ 6 0
14 ACT-CL J0901.5+0301 ClG 09 01 32.4334 +03 01 09.609           ~ 4 0
15 ACO 963 ClG 10 17 03.4 +39 02 56           ~ 414 0
16 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 456 0
17 ZwCl 1215+0400 ClG 12 17 43.62 +03 38 51.5           ~ 169 0
18 ACO 1651 ClG 12 59 27.3 -04 10 49           ~ 307 0
19 ACO 1663 ClG 13 02 52.55 -02 31 04.0           ~ 112 0
20 MARD J213049.6-645946 ClG 21 30 56.209 -64 58 40.32           ~ 16 0
21 ACT-CL J2135.6-5726 ClG 21 35 39.8 -57 26 29           ~ 30 0
22 1eRASS J213800.9-600758 ClG 21 38 00.059 -60 07 54.34           ~ 25 0
23 ACT-CL J2351.6-5452 ClG 23 51 36.4073 -54 52 51.379           ~ 20 0

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