2011MNRAS.414.3751R


Query : 2011MNRAS.414.3751R

2011MNRAS.414.3751R - Mon. Not. R. Astron. Soc., 414, 3751-3763 (2011/July-2)

Sunyaev–Zel'dovich observation of the bullet-like cluster Abell 2146 with the arcminute microkelvin imager.

RODRIGUEZ-GONZALVEZ C., OLAMAIE M., DAVIES M.L., FABIAN A.C., FEROZ F., FRANZEN T.M.O., GRAINGE K.J.B., HOBSON M.P., HURLEY-WALKER N., LASENBY A.N., POOLEY G.G., RUSSELL H.R., SANDERS J.S., SAUNDERS R.D.E., SCAIFE A.M.M., SCHAMMEL M.P., SCOTT P.F., SHIMWELL T.W., TITTERINGTON D.J., WALDRAM E.M., ZWART J.T.L. (The AMI Consortium)

Abstract (from CDS):

We present 13.9–18.2 GHz observations of the Sunyaev–Zel'dovich (SZ) effect towards Abell 2146 using the Arcminute Microkelvin Imager (AMI). The cluster is detected with a peak signal-to-noise ratio of 13σ in the radio source subtracted map from 9 h of data. Comparison of the SZ image with the X-ray image from Russell et al. suggests that both have extended regions which lie approximately perpendicular to one another, with their emission peaks significantly displaced. These features indicate non-uniformities in the distributions of the gas temperature and pressure, and suggest complex dynamics indicative of a cluster merger. We use a fast, Bayesian cluster analysis to explore the high-dimensional parameter space of the cluster-plus-sources model to obtain robust cluster parameter estimates in the presence of radio point sources, receiver noise and primordial cosmic microwave background (CMB) anisotropy; despite the substantial radio emission from the direction of Abell 2146, the probability of SZ + CMB primordial structure + radio sources + receiver noise to CMB + radio sources + receiver noise is 3 {x} 106 : 1. We compare the results from three different cluster models. Our preferred model exploits the observation that the gas fractions do not appear to vary greatly between clusters. Given the relative masses of the two merging systems in Abell 2146, the mean gas temperature can be deduced from the virial theorem (assuming all of the kinetic energy is in the form of internal gas energy) without being affected significantly by the merger event, provided the primary cluster was virialized before the merger. In this model we fit a simple spherical isothermal β-model to our data, despite the inadequacy of this model for a merging system like Abell 2146, and assume the cluster follows the mass–temperature relation of a virialized, singular, isothermal sphere. We note that this model avoids inferring large-scale cluster parameters internal to r200 under the widely used assumption of hydrostatic equilibrium. We find that at r200 the average total mass MT= (4.1 ± 0.5) {x} 1014 h–1 M☉ and the mean gas temperature T= 4.5±0.5 keV.

We request that any reference to this paper cites `AMI Consortium: Rodrìguez-Gonzálvez et al. 2011'.


Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): galaxies: clusters: general - galaxies: clusters: individual: Abell 2146 - cosmic background radiation - cosmology observations

Nomenclature: Fig. 3, Table 6: [ROD2011] A (Nos A-O).

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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
2 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 465 0
3 ClG 0657-56 ClG 06 58 26.9 -55 58 21           ~ 1077 1
4 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
5 [ROD2011] G Rad 15 54 03.960 +66 28 41.90           ~ 1 0
6 [ROD2011] B Rad 15 54 30.950 +66 36 39.58           ~ 1 0
7 [ROD2011] K Rad 15 54 47.500 +66 28 37.43           ~ 1 0
8 [ROD2011] L Rad 15 54 49.110 +66 14 21.49           ~ 1 0
9 [ROD2011] I Rad 15 55 10.840 +66 19 45.82           ~ 1 0
10 [ROD2011] H Rad 15 55 25.670 +66 22 03.96           ~ 1 0
11 [ROD2011] E Rad 15 55 57.420 +66 20 03.11           ~ 1 0
12 [ROD2011] A Rad 15 56 04.230 +66 22 12.94           ~ 1 0
13 ACO 2146 ClG 15 56 04.7 +66 20 24           ~ 192 0
14 [ROD2011] C Rad 15 56 14.300 +66 20 53.45           ~ 1 0
15 [ROD2011] M Rad 15 56 15.400 +66 22 44.48           ~ 1 0
16 [ROD2011] N Rad 15 56 27.900 +66 19 43.82           ~ 1 0
17 [ROD2011] D Rad 15 56 36.510 +66 35 21.65           ~ 1 0
18 [ROD2011] J Rad 15 57 09.460 +66 22 37.62           ~ 1 0
19 [ROD2011] O Rad 15 57 56.100 +66 22 49.80           ~ 1 0
20 [ROD2011] F Rad 15 58 10.230 +66 24 35.72           ~ 1 0
21 [VV96] J162304.5+662401 Bla 16 23 04.52169655 +66 24 01.0787041   19.477   17.430   ~ 67 1
22 4C 69.21 Bla 16 42 07.84851261 +68 56 39.7563611   19.723   19.219   ~ 326 1

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