2006ApJ...639...64O


Query : 2006ApJ...639...64O

2006ApJ...639...64O - Astrophys. J., 639, 64-80 (2006/March-1)

Effects of mergers and core structure on the bulk properties of nearby galaxy clusters.

O'HARA T.B., MOHR J.J., BIALEK J.J. and EVRARD A.E.

Abstract (from CDS):

We use X-ray morphological measurements and the scatter of clusters about observed and simulated scaling relations to examine the impact of merging and core-related phenomena on the structure of galaxy clusters. We use a range of X-ray and near-infrared (near-IR) scaling relations; all observed scaling relations constructed from emission-weighted mean temperature and intracluster medium mass, X-ray luminosity, isophotal size, and near-IR luminosity show a separation between clusters identified as cool core (CC) and those identified as non-cool core (NCC). We attribute this partially to a simple temperature bias in CC clusters and partially to other cool core-related structural changes. Scaling relations constructed from observables that are largely independent of core structure show smaller separation between CC and NCC populations. We attempt to minimize CC-related separation in scaling relations via two methods: by applying a uniform scale factor to CC cluster temperatures and determining the scale factor for each relation that minimizes the separation between CC and NCC populations, and by introducing cluster central surface brightness as a third parameter in observable-temperature scaling relations. We find an average temperature bias factor of 1.07±0.02 between the CC and NCC populations; the three-parameter approach reduces scatter in scaling relations more than a simple CC temperature scaling. We examine the scatter about the best-fit observable-temperature-brightness scaling relations and compare the intrinsic scatter within subsamples split by CC/NCC and four different morphological merger indicators. CC clusters and clusters with less substructure generally exhibit higher scatter about scaling relations. The larger structural variations in CC clusters are present well outside the core, suggesting that a process more global than core radiative instability is at work. Simulations without cooling mechanisms also show no correlation between substructure and larger scatter about scaling relations, indicating that any merger-related scatter increases are subtle. Taken together, the observational and simulation results indicate that cool core-related phenomena–not merging processes–are the primary contributor to scatter in scaling relations. Our analysis does not appear to support the scenario in which clusters evolve cool cores over time unless they experience major mergers.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Clusters: General - Galaxies: Intergalactic Medium - X-Rays: Galaxies: Clusters

Simbad objects: 45

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Number of rows : 45
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 85 ClG 00 41 36.21 -09 19 30.4           ~ 974 0
2 ACO 119 ClG 00 56 08.57 -01 12 00.8           ~ 577 2
3 ACO 262 ClG 01 52 50.4 +36 08 46           ~ 727 1
4 2A 0251+413 ClG 02 54 26.6 +41 33 25           ~ 328 1
5 ACO 401 ClG 02 58 50.3 +13 34 07           ~ 592 0
6 ACO 3112 ClG 03 17 52.9 -44 15 06           ~ 329 1
7 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
8 ACO 3158 ClG 03 43 07.5 -53 38 09           ~ 327 0
9 ACO 478 ClG 04 13 24.8 +10 27 52           ~ 522 0
10 ACO 3266 ClG 04 31 26.4 -61 25 17           ~ 447 0
11 ACO 496 ClG 04 33 40.8 -13 14 34           ~ 728 2
12 ACO 3391 ClG 06 26 15.4 -53 40 52           ~ 222 1
13 PKS 0745-19 rG 07 47 31.3247085936 -19 17 40.013334276   19.60       ~ 422 1
14 ClG 0745-1910 ClG 07 47 32.4 -19 18 23           ~ 378 0
15 ACO 644 ClG 08 17 26.1 -07 31 13           ~ 241 0
16 ACO 754 ClG 09 09 14.8 -09 40 35           ~ 695 1
17 ACO 780 ClG 09 18 30 -12 15.7           ~ 469 0
18 NAME Hydra I Cluster ClG 10 36 36.0 -27 31 04           ~ 905 1
19 ACO 1367 ClG 11 44 44.6 +19 41 59           ~ 1127 1
20 ACO 3526 ClG 12 48 49.2 -41 18 17           ~ 1154 2
21 ACO 3532 ClG 12 57 19.2 -30 22 13           ~ 185 2
22 ACO 1651 ClG 12 59 27.3 -04 10 49           ~ 307 0
23 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
24 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1178 0
25 ACO 3558 ClG 13 28 03.2 -31 31 35           ~ 476 2
26 ACO 3562 ClG 13 33 31.8 -31 40 23           ~ 337 1
27 ACO 3571 ClG 13 47 32.4 -32 50 12           ~ 308 2
28 ACO 1795 ClG 13 48 47.4 +26 34 55           ~ 1330 0
29 ACO 2029 ClG 15 10 54.2 +05 44 23           ~ 1020 0
30 ACO 2052 ClG 15 16 41.64 +07 01 45.5           ~ 756 1
31 ACT-CL J1521.8+0742 ClG 15 21 48.8 +07 43 41     15.13     ~ 326 0
32 ACO 2063 ClG 15 23 01.8 +08 38 22           ~ 414 2
33 ACO 2142 ClG 15 58 26.5 +27 13 52           ~ 825 0
34 ACO 2199 ClG 16 28 34.5 +39 32 26           ~ 1206 1
35 ACO 2204 ClG 16 32 47.7 +05 34 18           ~ 457 0
36 BAX 249.5848-64.5165 ClG 16 38 13.2 -64 21 21           ~ 123 0
37 ACO 2244 ClG 17 02 40.33 +34 02 58.7           ~ 301 0
38 ACO 2256 ClG 17 03 37.5 +78 37 23           ~ 928 1
39 BAX 258.1082-23.3759 ClG 17 12 26.3 -23 21 38           ~ 303 0
40 ACO 2255 ClG 17 12 56.0 +64 04 06           ~ 605 0
41 ACO 2319 ClG 19 21 14.0 +43 56 57           ~ 495 1
42 ACO 3667 ClG 20 12 33.68 -56 50 26.3           ~ 676 1
43 ACO 2597 ClG 23 25 19.70 -12 07 27.7           ~ 572 0
44 ACO 4038 ClG 23 47 31.1 -28 12 10           ~ 349 3
45 ACO 4059 ClG 23 57 02.2 -34 45 58           ~ 400 1

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