2000MNRAS.316..299W


Query : 2000MNRAS.316..299W

2000MNRAS.316..299W - Mon. Not. R. Astron. Soc., 316, 299-306 (2000/August-1)

A combined analysis of cluster mass estimates from strong lensing, X-ray measurement and the universal density profile.

WU X.-P.

Abstract (from CDS):

We present a combined analysis of mass estimates in the central cores of galaxy clusters from the strong lensing, the X-ray measurements and the universal density profile (NFW). Special attention is paid to the questions (1) whether the previously claimed mass discrepancy between the strong lensing and X-ray measurements is associated with the presence of cooling/non-cooling flows, (2) whether the cusped NFW density model can provide a consistent cluster mass with the strong lensing result and (3) whether a non-zero cosmological constant can be of any help to reducing the strong lensing-X-ray mass ratios. We analyse a sample of 26 arc-like images among 21 clusters, the X-ray data of which are available in archive. The X-ray and NFW cluster masses are obtained by assuming that the intracluster gas is isothermal and in hydrostatic equilibrium with the underlying gravitational potential of the clusters.

A statistical comparison of these three mass estimates reveals that the mass discrepancies for all the events are well within a factor of 2, if X-ray measurement uncertainties are included. In particular, we confirm the result of Allen that the larger mass discrepancy is only detected in the intermediate cooling, especially non-cooling flow clusters, thus attributing the mass discrepancy to the local dynamical activities in the central regions. We show that the NFW profile yields a consistent cluster mass with the conventional X-ray measurement, which is interpreted as the consequence of the common working hypothesis behind the two methods. Any difference between these two models must occur at even smaller radii (e.g. within the arc-like images) or at large radii. It appears that the introduction of the cusped density profile as the dark matter distribution of clusters cannot raise the cluster masses enclosed within arc-like images. Finally, a non-zero cosmological constant is able to moderately reduce the mass ratios of mlens to mxray. These results, together with the excellent agreement between the X-ray, optical and weak lensing determined cluster masses on scales greater than the X-ray core sizes found in the early work, indicate that the mass discrepancy between strong lensing and other methods in the intermediate cooling and non-cooling flow clusters is likely to have arisen from both the oversimplification of the lensing model and the inappropriate application of isothermality and equilibrium hypothesis in the central regions of clusters where the local dynamical activities make a non-negligible contribution to both mass estimates.


Abstract Copyright: 2000, Royal Astronomical Society

Journal keyword(s): galaxies: clusters: general - dark matter - gravitational lensing - X-rays: galaxies

Simbad objects: 22

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Number of rows : 22
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 ZwCl 0024+1652 ClG 00 26 35.6 +17 09 32     18.35     ~ 648 1
2 ACO 370 ClG 02 39 50.5 -01 35 08           ~ 825 0
3 ClG 0303+1658 ClG 03 05 31.6 +17 10 02     20.13     ~ 92 0
4 ClG 0440+02 ClG 04 43 09.7 +02 10 19     17.03     ~ 129 0
5 ClG 0451-03 ClG 04 54 10.9 -03 01 07     20.0     ~ 368 0
6 ACO S 506 ClG 05 01 04.4 -24 24 41           ~ 60 0
7 PKS 0745-19 rG 07 47 31.3247085936 -19 17 40.013334276   19.60       ~ 422 1
8 ClG 0745-1910 ClG 07 47 32.4 -19 18 23           ~ 378 0
9 ClG 1008-12 ClG 10 10 34.1 -12 39 48     18.0     ~ 155 0
10 ACO 963 ClG 10 17 03.4 +39 02 56           ~ 414 0
11 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1178 0
12 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 577 0
13 ZwCl 1358+6245 ClG 13 59 54.3 +62 30 36     18.5     ~ 370 0
14 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
15 ZwCl 1455+2232 ClG 14 57 15.2 +22 20 30     18.62 20.04   ~ 309 0
16 ACO 2163 ClG 16 15 46.1 -06 08 50           ~ 586 0
17 ACO 2218 ClG 16 35 54.0 +66 13 00           ~ 827 1
18 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 381 0
19 ClG 2137-2353 ClG 21 40 12.8 -23 39 27     18.5     ~ 390 0
20 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 732 2
21 ClG 2236-04 ClG 22 39 35.6 -04 28 47           ~ 28 0
22 ClG 2244.6-0222 ClG 22 47 12.2 -02 05 37           ~ 128 0

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