2014MNRAS.440.2077M


Query : 2014MNRAS.440.2077M

2014MNRAS.440.2077M - Mon. Not. R. Astron. Soc., 440, 2077-2098 (2014/May-3)

Cosmology and astrophysics from relaxed galaxy clusters - II. Cosmological constraints.

MANTZ A.B., ALLEN S.W., MORRIS R.G., RAPETTI D.A., APPLEGATE D.E., KELLY P.L., VON DER LINDEN A. and SCHMIDT R.W.

Abstract (from CDS):

This is the second in a series of papers studying the astrophysics and cosmology of massive, dynamically relaxed galaxy clusters. The data set employed here consists of Chandra observations of 40 such clusters, identified in a comprehensive search of the Chandra archive for hot (kT ≳ 5keV), massive, morphologically relaxed systems, as well as high-quality weak gravitational lensing data for a subset of these clusters. Here we present cosmological constraints from measurements of the gas mass fraction, fgas, for this cluster sample. By incorporating a robust gravitational lensing calibration of the X-ray mass estimates, and restricting our measurements to the most self-similar and accurately measured regions of clusters, we significantly reduce systematic uncertainties compared to previous work. Our data for the first time constrain the intrinsic scatter in fgas, 7.4±2.3 percent in a spherical shell at radii 0.8-1.2 r2500 ( ∼ 1/4 of the virial radius), consistent with the expected level of variation in gas depletion and non-thermal pressure for relaxed clusters. From the lowest redshift data in our sample, five clusters at z < 0.16, we obtain a constraint on a combination of the Hubble parameter and cosmic baryon fraction, h3/2Ωb/Ωm = 0.089±0.012, that is insensitive to the nature of dark energy. Combining this with standard priors on h and Ωbh2 provides a tight constraint on the cosmic matter density, Ωm = 0.27±0.04, which is similarly insensitive to dark energy. Using the entire cluster sample, extending to z > 1, we obtain consistent results for Ωm and interesting constraints on dark energy: Ω_Λ=0.65^+0.17_-0.22 for non-flat ΛCDM (cosmological constant) models, and w = -0.98±0.26 for flat models with a constant dark energy equation of state. Our results are both competitive and consistent with those from recent cosmic microwave background, Type Ia supernova and baryon acoustic oscillation data. We present constraints on more complex models of evolving dark energy from the combination of fgas data with these external data sets, and comment on the possibilities for improved fgas constraints using current and next-generation X-ray observatories and lensing data.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): galaxies: clusters: general - cosmological parameters - cosmology: observations - dark matter - distance scale - X-rays: galaxies: clusters

Simbad objects: 48

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Number of rows : 48
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 J0000.9-5748 ClG 00 01 00 -57 48.5           ~ 57 0
2 ACT-CL J0011.7-1523 ClG 00 11 42.9 -15 23 22           ~ 39 0
3 ACT-CL J0150.3-1005 ClG 01 50 21.24 -10 05 29.6           ~ 27 0
4 ACT-CL J0159.8-0849 ClG 01 59 49.4 -08 50 00           ~ 98 0
5 ClG J0242-2132 ClG 02 42 35.9 -21 32 26           ~ 55 0
6 ACO 383 ClG 02 48 03.3915 -03 31 45.228           ~ 389 0
7 MCS J0326.8-0043 ClG 03 26 49.0 -00 43 41           ~ 10 0
8 ACO 478 ClG 04 13 24.8 +10 27 52           ~ 522 0
9 ClG J0429-0253 ClG 04 29 36.0 -02 53 09           ~ 131 0
10 BAX 069.7593+05.3453 ClG 04 39 02.2 +05 20 43           ~ 82 0
11 3C 186 QSO 07 44 17.4720658920 +37 53 17.250697320   17.5 18.14 17.2   ~ 339 1
12 ClG J0744+3927 ClG 07 44 52.5 +39 27 30           ~ 189 0
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 ZwCl 0857+2107 ClG 09 00 36.90 +20 53 40.3           ~ 103 0
16 RXC J0913.7+4056 ClG 09 13 46.0 +40 56 20           ~ 71 0
17 ClG J0947+7623 ClG 09 46 59.916 +76 23 43.99           ~ 165 0
18 NVSS J094712+762312 Rad 09 47 12.37 +76 23 09.3           ~ 151 1
19 ZwCl 0949+5207 ClG 09 52 49.1 +51 53 05           ~ 141 0
20 ACO 3444 ClG 10 23 53.1540 -27 15 07.840           ~ 97 0
21 MCS J1115.8+0129 ClG 11 15 52.1 +01 29 53           ~ 142 0
22 ClG 1137+66 ClG 11 40 23.0 +66 08 16     21.0     ~ 141 0
23 ClG J1226+3332 ClG 12 26 57.7 +33 32 50           ~ 228 0
24 ClG J1311-0311 ClG 13 11 01.7 -03 10 38           ~ 120 0
25 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 577 0
26 MCS J1359.1-1929 ClG 13 59 09.0 -19 29 07           ~ 13 0
27 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
28 3C 295 Sy1 14 11 20.6 +52 12 09   22.34 20.80 18.54   ~ 1021 4
29 ClG J1415+3611 ClG 14 15 11.1 +36 12 03           ~ 85 1
30 ClG J1423+2404 ClG 14 23 47.7 +24 04 40           ~ 231 0
31 MCS J1427.3+4408 ClG 14 27 16.2 +44 07 31           ~ 34 0
32 MCS J1427.6-2521 ClG 14 27 39.4 -25 21 02           ~ 27 0
33 ACO S 780 ClG 14 59 29.1 -18 10 45           ~ 93 0
34 ClG J1504-0248 ClG 15 04 07.4 -02 48 15           ~ 186 0
35 ACO 2029 ClG 15 10 54.2 +05 44 23           ~ 1020 0
36 MCXC J1524.2-3154 ClG 15 24 12.9 -31 54 25           ~ 34 0
37 ClG J1532+3021 ClG 15 32 53.8 +30 21 00           ~ 122 0
38 ClG J1621+3810 ClG 16 21 25.5 +38 09 43           ~ 83 0
39 ACO 2204 ClG 16 32 47.7 +05 34 18           ~ 457 0
40 ClG J1720+3536 ClG 17 20 16.8 +35 36 27           ~ 150 1
41 ClG J1931-2635 ClG 19 31 49.6 -26 34 33           ~ 181 0
42 ACT-CL J2043.2-5035 ClG 20 43 16.7205 -50 35 30.861           ~ 47 0
43 ACT-CL J2046.0-3430 ClG 20 46 00.1 -34 30 12           ~ 24 0
44 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 308 0
45 ClG 2137-2353 ClG 21 40 12.8 -23 39 27     18.5     ~ 390 0
46 ClG J2229-2756 ClG 22 29 45.36 -27 55 36.5           ~ 50 0
47 PSZSPT J2331-5052 ClG 23 31 51 -50 51.9           ~ 53 0
48 ACT-CL J2344.7-4243 ClG 23 44 43.9 -42 43 11           ~ 229 0

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