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  • A blind detection of a larg...
    Shimwell, T. W; Barker, R. W; Biddulph, P; Bly, D; Boysen, R. C; Brown, A. R; Brown, M. L; Clementson, C; Crofts, M; Culverhouse, T. L; Czeres, J; Dace, R. J; Davies, M. L; D'Alessandro, R; Doherty, P; Duggan, K; Ely, J. A; Felvus, M; Feroz, F; Flynn, W; Franzen, T. M. O; Geisbüsch, J; Génova-Santos, R; Grainge, K. J. B; Grainger, W. F; Hammett, D; Hobson, M. P; Holler, C. M; Hurley-Walker, N; Jilley, R; Kaneko, T; Kneissl, R; Lancaster, K; Lasenby, A. N; Marshall, P. J; Newton, F; Norris, O; Northrop, I; Odell, D. M; Olamaie, M; Perrott, Y. C; Pober, J. C; Pooley, G. G; Pospieszalski, M. W; Quy, V; Rodríguez-Gonzálvez, C; Saunders, R. D. E; Scaife, A. M. M; Schammel, M. P; Schofield, J; Scott, P. F; Shaw, C; Smith, H; Titterington, D. J; Velić, M; Waldram, E. M; West, S; Wood, B. A; Yassin, G; Zwart, J. T. L

    Monthly notices of the Royal Astronomical Society, June 2012, Letnik: 423, Številka: 2
    Journal Article

    We present an interesting Sunyaev-Zel'dovich (SZ) detection in the first of the Arcminute Microkelvin Imager (AMI) 'blind', degree-square fields to have been observed down to our target sensitivity of . In follow-up deep pointed observations the SZ effect is detected with a maximum peak decrement greater than eight times the thermal noise. No corresponding emission is visible in the ROSAT all-sky X-ray survey and no cluster is evident in the Palomar all-sky optical survey. Compared with existing SZ images of distant clusters, the extent is large (≈10 arcmin) and complex; our analysis favours a model containing two clusters rather than a single cluster. Our Bayesian analysis is currently limited to modelling each cluster with an ellipsoidal or spherical β model, which does not do justice to this decrement. Fitting an ellipsoid to the deeper candidate we find the following. (a) Assuming that the Evrard et al. approximation to Press & Schechter correctly gives the number density of clusters as a function of mass and redshift, then, in the search area, the formal Bayesian probability ratio of the AMI detection of this cluster is 7.9 × 104:1; alternatively assuming Jenkins et al. as the true prior, the formal Bayesian probability ratio of detection is 2.1 × 105:1. (b) The cluster mass is . (c) Abandoning a physical model with number density prior and instead simply modelling the SZ decrement using a phenomenological β model of temperature decrement as a function of angular distance, we find a central SZ temperature decrement of K - this allows for cosmic microwave background primary anisotropies, receiver noise and radio sources. We are unsure if the cluster system we observe is a merging system or two separate clusters.