2022A&A...665A.124L


Query : 2022A&A...665A.124L

2022A&A...665A.124L - Astronomy and Astrophysics, volume 665A124-124 (2022/9-1)

Chandra follow-up of the Hectospec Cluster Survey: Comparison of caustic and hydrostatic masses and constraints on the hydrostatic bias.

LOGAN C.H.A., MAUGHAN B.J., DIAFERIO A., DUFFY R.T., GELLER M.J., RINES K. and SOHN J.

Abstract (from CDS):


Context. Clusters of galaxies are powerful probes with which to study cosmology and astrophysics. However, for many applications, an accurate measurement of a cluster's mass is essential. A systematic underestimate of hydrostatic masses from X-ray observations (the so-called hydrostatic bias) may be responsible for tension between the results of different cosmological measurements.
Aims. We compare X-ray hydrostatic masses with masses estimated using the caustic method (based on galaxy velocities) in order to explore the systematic uncertainties of both methods and place new constraints on the level of hydrostatic bias.
Methods. Hydrostatic and caustic mass profiles were determined independently for a sample of 44 clusters based on Chandra observations of clusters from the Hectospec Cluster Survey. This is the largest systematic comparison of its kind. Masses were compared at a standardised radius (R500) using a model that includes possible bias and scatter in both mass estimates. The systematics affecting both mass determination methods were explored in detail.
Results. The hydrostatic masses were found to be systematically higher than caustic masses on average, and we found evidence that the caustic method increasingly underestimates the mass when fewer galaxies are used to measure the caustics. We limit our analysis to the 14 clusters with the best-sampled caustics where this bias is minimised (≥210 galaxies), and find that the average ratio of hydrostatic-to-caustic mass at R500 is M500,X/M500,C = 1.12–0.10+0.11.
Conclusions. We interpret this result as a constraint on the level of hydrostatic bias, favouring small or zero levels of hydrostatic bias (less than 20% at the 3σ level). However, we find that systematic uncertainties associated with both mass estimation methods remain at the 10 - 15% level, which would permit significantly larger levels of hydrostatic bias.

Abstract Copyright: © C. H. A. Logan et al. 2022

Journal keyword(s): galaxies: clusters: general - galaxies: kinematics and dynamics - cosmology: observations - X-rays: galaxies: clusters

Simbad objects: 62

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Number of rows : 62
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 267 ClG 01 52 43.016 +00 59 58.90           ~ 241 0
2 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
3 ZwCl 0755+5408 ClG 07 59 54.4 +54 01 01           ~ 26 0
4 ACO 646 ClG 08 22 10.0 +47 05 58           ~ 102 1
5 ACO 655 ClG 08 25 16.12 +47 09 34.2           ~ 118 0
6 ACO 667 ClG 08 28 05.8 +44 46 00           ~ 45 0
7 ACO 689 ClG 08 37 29 +14 59.5           ~ 53 0
8 ACO 697 ClG 08 42 57.6 +36 21 45           ~ 277 0
9 ClG 0906.4+1114 ClG 09 08 52.1 +11 01 36           ~ 21 0
10 ClG 0906.5+1110 ClG 09 09 12.7 +10 58 32           ~ 108 0
11 ACO 773 ClG 09 17 51.3 +51 43 20           ~ 308 0
12 ACO 795 ClG 09 24 11.26 +14 09 03.5           ~ 120 0
13 ZwCl 0949+5207 ClG 09 52 49.1 +51 53 05           ~ 141 0
14 ACO 963 ClG 10 17 03.4 +39 02 56           ~ 414 0
15 ACO 980 ClG 10 22 30.6 +50 06 06           ~ 70 0
16 ZwCl 1021+0426 ClG 10 23 39.0 +04 11 14   15.6 17.95     ~ 297 0
17 ACO 990 ClG 10 23 39.46 +49 08 19.6           ~ 88 0
18 ZwCl 1023+1257 ClG 10 25 55.9 +12 41 07           ~ 54 0
19 ACO 1033 ClG 10 31 39.78 +35 05 34.4           ~ 97 0
20 ACO 1068 ClG 10 40 47.1 +39 57 19           ~ 232 0
21 ACO 1132 ClG 10 58 32.05 +56 47 14.2           ~ 145 1
22 ACO 1201 ClG 11 12 54.4 +13 26 08           ~ 131 1
23 ACO 1204 ClG 11 13 32.2 +17 35 40           ~ 101 0
24 ACO 1235 ClG 11 23 26.10 +19 34 59.9           ~ 59 0
25 ACO 1246 ClG 11 23 57.4 +21 29 14           ~ 118 0
26 ACO 1302 ClG 11 33 12.02 +66 22 26.9           ~ 81 0
27 ACO 1361 ClG 11 43 45.85 +46 20 51.8           ~ 96 0
28 ACO 1366 ClG 11 44 44.72 +67 24 51.9           ~ 56 0
29 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 456 0
30 ACO 1423 ClG 11 57 17.3206 +33 36 39.364           ~ 181 0
31 ACO 1437 ClG 12 00 24.5 +03 19 52           ~ 93 0
32 ACO 1553 ClG 12 30 48.000 +10 33 21.60           ~ 95 0
33 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
34 ACO 1682 ClG 13 06 49.7 +46 32 59           ~ 149 1
35 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1178 0
36 ACO 1758 ClG 13 32 32.1 +50 30 37           ~ 266 2
37 ACO 1763 ClG 13 35 20.1 +41 00 04           ~ 335 0
38 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
39 ACO 1902 ClG 14 21 39.7 +37 17 43           ~ 67 0
40 ACO 1918 ClG 14 25 22.7 +63 11 14           ~ 71 0
41 ACO 1914 ClG 14 25 57.4 +37 49 54           ~ 338 0
42 ACO 1930 ClG 14 32 42.6 +31 34 07           ~ 63 0
43 ACO 1978 ClG 14 51 09.4 +14 36 43           ~ 30 0
44 ACO 2009 ClG 15 00 15.2 +21 22 09           ~ 113 0
45 ClG J1504-0248 ClG 15 04 07.4 -02 48 15           ~ 186 0
46 ACO 2034 ClG 15 10 03.9 +33 30 57           ~ 248 1
47 ACO 2050 ClG 15 16 18.7 +00 05 31           ~ 122 0
48 ACO 2055 ClG 15 18 46.29 +06 13 42.9           ~ 113 0
49 ACO 2069 ClG 15 24 02.92 +29 53 20.3           ~ 165 0
50 ACO 2111 ClG 15 39 40.9 +34 25 04           ~ 188 0
51 ACO 2142 ClG 15 58 26.5 +27 13 52           ~ 825 0
52 ACO 2187 ClG 16 24 13.9 +41 14 37           ~ 47 0
53 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 381 0
54 ZwCl 1717+5636 ClG 17 18 09.272 +56 40 00.02           ~ 53 1
55 ACO 2259 ClG 17 20 09.2 +27 40 09           ~ 131 0
56 ClG J1720+2638 ClG 17 20 09.6 +26 37 35           ~ 284 0
57 [RGD2013] J172213.019+320651.768 BiC 17 22 13.047 +32 06 51.79           ~ 5 0
58 ACO 2261 ClG 17 22 26.9 +32 07 58           ~ 370 0
59 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 308 0
60 ACO 2396 ClG 21 55 40.6527 +12 30 54.132           ~ 44 0
61 ACO 2631 ClG 23 37 40.7 +00 16 35           ~ 183 0
62 ACO 2645 ClG 23 41 17.0 -09 01 11           ~ 98 0

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