2008MNRAS.383..879A


Query : 2008MNRAS.383..879A

2008MNRAS.383..879A - Mon. Not. R. Astron. Soc., 383, 879-896 (2008/January-3)

Improved constraints on dark energy from Chandra X-ray observations of the largest relaxed galaxy clusters.

ALLEN S.W., RAPETTI D.A., SCHMIDT R.W., EBELING H., MORRIS R.G. and FABIAN A.C.

Abstract (from CDS):

We present constraints on the mean matter density, Ωm, dark energy density, ΩDE, and the dark energy equation of state parameter, w, using Chandra measurements of the X-ray gas mass fraction (fgas) in 42 hot (kT > 5keV), X-ray luminous, dynamically relaxed galaxy clusters spanning the redshift range 0.05 < z < 1.1. Using only the fgas data for the six lowest redshift clusters at z < 0.15, for which dark energy has a negligible effect on the measurements, we measure Ωm= 0.28±0.06 (68 per cent confidence limits, using standard priors on the Hubble constant, H0, and mean baryon density, Ωbh2). Analysing the data for all 42 clusters, employing only weak priors on H0 and Ωbh2, we obtain a similar result on Ωm and a detection of the effects of dark energy on the distances to the clusters at ∼99.99 per cent confidence, with ΩDE= 0.86±0.21 for a non-flat ΛCDM model. The detection of dark energy is comparable in significance to recent type Ia supernovae (SNIa) studies and represents strong, independent evidence for cosmic acceleration. Systematic scatter remains undetected in the fgasdata, despite a weighted mean statistical scatter in the distance measurements of only ∼5 per cent. For a flat cosmology with a constant dark energy equation of state, we measure Ωm= 0.28±0.06 and w = -1.14±0.31. Combining the fgas data with independent constraints from cosmic microwave background and SNIa studies removes the need for priors on Ωbh2 and H0 and leads to tighter constraints: Ωm= 0.253±0.021 and w = -0.98±0.07 for the same constant-w model. Our most general analysis allows the equation of state to evolve with redshift. Marginalizing over possible transition redshifts 0.05 < zt< 1, the combined fgas+ CMB + SNIa data set constrains the dark energy equation of state at late and early times to be w0= -1.05±0.29 and wet= -0.83±0.46, respectively, in agreement with the cosmological constant paradigm. Relaxing the assumption of flatness weakens the constraints on the equation of state by only a factor of ∼2. Our analysis includes conservative allowances for systematic uncertainties associated with instrument calibration, cluster physics and data modelling. The measured small systematic scatter, tight constraint on Ωmand powerful constraints on dark energy from the fgas data bode well for future dark energy studies using the next generation of powerful X-ray observatories, such as Constellation-X.

Abstract Copyright: 2007 The Authors. Journal compilation © 2007 RAS

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

CDS comments: RX J1504.1-0248 is RXC J1504.1-0248 in Simbad. In Table 3: RX J0439.0+0521 is a misprint for RX J0439.0+0520 and RX J1347.5-1144 is a misprint for RX J13475-1145.

Simbad objects: 44

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Number of rows : 44
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 ACT-CL J0011.7-1523 ClG 00 11 42.9 -15 23 22           ~ 35 0
2 ACT-CL J0159.8-0849 ClG 01 59 49.4 -08 50 00           ~ 85 0
3 ClG J0242-2132 ClG 02 42 35.9 -21 32 26           ~ 50 0
4 ACO 383 ClG 02 48 03.3915 -03 31 45.228           ~ 359 0
5 ClG J0329-0212 ClG 03 29 41.6 -02 11 47           ~ 142 0
6 ACO 478 ClG 04 13 20.7 +10 28 35           ~ 502 0
7 ClG J0429-0253 ClG 04 29 36.0 -02 53 09           ~ 123 0
8 BAX 069.7593+05.3453 ClG 04 39 02.2 +05 20 43           ~ 78 0
9 3C 186 QSO 07 44 17.4720658920 +37 53 17.250697320   17.5 18.14 17.2   ~ 324 1
10 ClG J0744+3927 ClG 07 44 52.5 +39 27 30           ~ 181 0
11 ClG 0745-19 ClG 07 47 31.3 -19 17 40           ~ 372 0
12 2MASX J07473129-1917403 BiC 07 47 31.3247085936 -19 17 40.013334276   19.60       ~ 409 1
13 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 258 0
14 ClG J0947+7623 ClG 09 46 59.916 +76 23 43.99           ~ 150 0
15 NVSS J094712+762312 Rad 09 47 12.5 +76 23 12           ~ 151 1
16 ACO 963 ClG 10 17 03.4 +39 02 56           ~ 400 0
17 ZwCl 1021+0426 ClG 10 23 39.0 +04 11 14   15.6 17.95     ~ 283 0
18 MCS J1115.8+0129 ClG 11 15 52.1 +01 29 53           ~ 131 0
19 ClG 1137+66 ClG 11 40 23.0 +66 08 16     21.0     ~ 138 0
20 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 430 0
21 ClG J1226+3332 ClG 12 26 57.7 +33 32 50           ~ 215 0
22 ClG J1311-0311 ClG 13 11 01.7 -03 10 38           ~ 109 0
23 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 548 0
24 ACO 1795 ClG 13 48 50.48 +26 35 07.4           ~ 1267 0
25 MCS J1359.2-1929 ClG 13 59 10.3 -19 29 24           ~ 4 0
26 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 689 1
27 3C 295 Sy2 14 11 20.6 +52 12 09   22.34 20.80 18.54   ~ 979 5
28 ClG J1415+3611 ClG 14 15 11.1 +36 12 03           ~ 78 1
29 ClG J1423+2404 ClG 14 23 47.7 +24 04 40           ~ 209 0
30 MCS J1427.3+4408 ClG 14 27 16.2 +44 07 31           ~ 21 0
31 MCS J1427.6-2521 ClG 14 27 39.4 -25 21 02           ~ 25 0
32 ClG J1504-0248 ClG 15 04 07.4 -02 48 15           ~ 175 0
33 ACO 2029 ClG 15 10 56.2 +05 44 42           ~ 943 0
34 ClG J1532+3021 ClG 15 32 53.8 +30 21 00           ~ 113 0
35 ClG J1621+3810 ClG 16 21 25.5 +38 09 43           ~ 79 0
36 ACO 2204 ClG 16 32 45.7 +05 34 43           ~ 436 0
37 ClG J1720+3536 ClG 17 20 16.8 +35 36 27           ~ 141 1
38 ClG J1931-2635 ClG 19 31 49.6 -26 34 33           ~ 161 0
39 MCS J2046.0-3430 ClG 20 46 00.5 -34 30 17           ~ 20 0
40 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 271 0
41 ClG 2137-2353 ClG 21 40 12.8 -23 39 27     18.5     ~ 378 0
42 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 688 2
43 ClG J2229-2756 ClG 22 29 45.36 -27 55 36.5           ~ 46 0
44 ACO 2537 ClG 23 08 22.3 -02 11 29           ~ 137 0

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