2024A&A...691A.340R


Query : 2024A&A...691A.340R

2024A&A...691A.340R - Astronomy and Astrophysics, volume 691A340 (2024/11-1)

CHEX-MATE: The intracluster medium entropy distribution in the gravity-dominated regime.

RIVA G., PRATT G.W., ROSSETTI M., BARTALUCCI I., KAY S.T., RASIA E., GAVAZZI R., UMETSU K., ARNAUD M., BALBONI M., BONAFEDE A., BOURDIN H., DE GRANDI S., DE LUCA F., ECKERT D., ETTORI S., GASPARI M., GASTALDELLO F., GHIRARDINI V., GHIZZARDI S., GITTI M., LOVISARI L., MAUGHAN B.J., MAZZOTTA P., MOLENDI S., POINTECOUTEAU E., SAYERS J., SERENO M. and TOWLER I.

Abstract (from CDS):

We characterise the intracluster gas entropy profiles of 32 very high-mass (M500 > 7.75 × 1014 M⊙) Planck SZ-detected galaxy clusters (HIGHMz), selected from the CHEX-MATE sample, allowing us to study the intracluster medium (ICM) entropy distribution in a regime where non-gravitational effects are expected to be minimised. Using XMM-Newton measurements, we determined the entropy profiles up to ∼R500 for all objects. We assessed the relative role of gas density and temperature measurements on the uncertainty in entropy reconstruction, showing that in the outer regions the largest contribution comes from the temperature. The scaled profiles exhibit a large dispersion in the central regions, but converge rapidly to the value expected from simple gravitational collapse beyond the core regions. We quantified the correlation between the ICM morphological parameters and scaled entropy as a function of radius, showing that centrally peaked objects have low central entropy, while morphologically disturbed objects have high central entropy. We compared the scaled HIGHMz entropy profiles to results from other observational samples, finding differences in normalisation, which appear linked to the average mass of the samples in question. Combining HIGHMz with other samples, we found that a weaker mass dependence than self-similar in the scaling (Am ∼ -0.25) allows us to minimise the dispersion in the radial range [0.3 - 0.8] R500 for clusters spanning over a decade in mass. The deviation from self-similar predictions is radially dependent and is more pronounced at small and intermediate radii than at R500. We also investigated the distribution of central entropy K0, finding no evidence for bimodality in the data and outer slope α, which peaks at α ∼ 1.1 with tails at both low and high α that correlate with dynamical state. Using weak-lensing masses for half of the sample, we found an indication for a small suppression of the scatter (∼30%) beyond the core when using masses derived from YX in the rescaling. Finally, we compared our results to recent cosmological numerical simulations from THE THREE HUNDRED and MACSIS, finding good agreement with the observational data in this mass regime. These results provide a robust observational benchmark in the gravity-dominated regime, and will serve as a future reference for samples at lower masses, higher redshifts, and for ongoing work using cosmological numerical simulations.

Abstract Copyright: © The Authors 2024

Journal keyword(s): galaxies: clusters: general - galaxies: clusters: intracluster medium

Simbad objects: 35

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Number of rows : 35
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 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
2 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 517 0
3 ACO 209 ClG 01 31 52.9 -13 36 53           ~ 326 0
4 ACT-CL J0137.4-0827 ClG 01 37 24.9 -08 27 22           ~ 50 0
5 ACT-CL J0159.0-3413 ClG 01 59 00.3 -34 13 00           ~ 33 0
6 ACT-CL J0254.3-5857 ClG 02 54 17.7 -58 57 11           ~ 57 0
7 ACT-CL J0417.5-1154 ClG 04 17 34.6 -11 54 32           ~ 116 0
8 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 465 0
9 ClG 0451-03 ClG 04 54 10.9 -03 01 07     20.0     ~ 368 0
10 ACO S 520 ClG 05 16 37.40 -54 30 01.5           ~ 114 0
11 ACT-CL J0553.4-3342 ClG 05 53 27.200 -33 42 53.02           ~ 74 0
12 MCS J0600.1-2008 ClG 06 00 17.0 -20 06 16           ~ 47 0
13 ClG 0657-56 ClG 06 58 26.9 -55 58 21           ~ 1077 1
14 PLCKESZ G210.6+17.1 ClG 07 48 46.60 +09 40 10.6           ~ 14 0
15 ACO 697 ClG 08 42 57.6 +36 21 45           ~ 277 0
16 ZwCl 0947+1723 ClG 09 49 51.8 +17 07 05           ~ 92 0
17 ACO 1300 ClG 11 32 00.7 -19 53 34           ~ 168 0
18 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 546 0
19 PLCKESZ G287.0+32.9 ClG 11 50 49.20 -28 04 36.5           ~ 100 0
20 MCS J1206.2-0847 ClG 12 06 12.2 -08 48 02           ~ 286 0
21 MCXC J1332.7+5032 ClG 13 32 44.8 +50 32 24           ~ 134 0
22 ACO 1763 ClG 13 35 20.1 +41 00 04           ~ 335 0
23 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 577 0
24 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
25 ACO S 780 ClG 14 59 29.1 -18 10 45           ~ 93 0
26 2MASX J15150305-1521537 ClG 15 14.9 -15 23           ~ 57 0
27 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 381 0
28 MCS J1731.6+2252 ClG 17 31 39.2 +22 51 50           ~ 48 0
29 PLCKESZ G004.5-19.5 ClG 19 16 54 -33 30.5           ~ 31 0
30 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 732 2
31 ACT-CL J2211.7-0349 ClG 22 11 44.8 -03 49 33           ~ 96 0
32 ACT-CL J2214.9-1359 ClG 22 14 57.3 -14 00 12           ~ 100 0
33 ClG J2243-0935 ClG 22 43 21.1 -09 35 43           ~ 96 0
34 ACO S 1063 ClG 22 48 45.4 -44 31 42           ~ 395 0
35 ACT-CL J2344.7-4243 ClG 23 44 43.9 -42 43 11           ~ 229 0

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