Cosmic Microwave Background Temperature at Galaxy Clusters
Author(s) -
E. S. Battistelli,
M. De Petris,
L. Lamagna,
F. Melchiorri,
E. Palladino,
G. Savini,
Asantha Cooray,
A. Melchiorri,
Yoel Rephaeli,
Meir Shimon
Publication year - 2002
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/345589
Subject(s) - cosmic microwave background , physics , astrophysics , redshift , coma cluster , microwave , galaxy , galaxy cluster , scaling , cluster (spacecraft) , spectrometer , optics , quantum mechanics , geometry , mathematics , anisotropy , computer science , programming language
We have deduced the cosmic microwave background (CMB) temperature in the Comacluster (A1656, $z=0.0231$), and in A2163 ($z=0.203$) from spectralmeasurements of the Sunyaev-Zel'dovich (SZ) effect over four passbands at radioand microwave frequencies. The resulting temperatures at these redshifts are$T_{Coma} = 2.789^{+0.080}_{-0.065}$ K and $T_{A2163} =3.377^{+0.101}_{-0.102}$ K, respectively. These values confirm the expectedrelation $T(z)=T_{0}(1+z)$, where $T_{0}= 2.725 \pm 0.002$ K is the valuemeasured by the COBE/FIRAS experiment. Alternative scaling relations that areconjectured in non-standard cosmologies can be constrained by the data; forexample, if $T(z) = T_{0}(1+z)^{1-a}$ or $T(z)=T_{0}[1+(1+d)z]$, then$a=-0.16^{+0.34}_{-0.32}$ and $d = 0.17 \pm 0.36$ (at 95% confidence). Webriefly discuss future prospects for more precise SZ measurements of $T(z)$ athigher redshifts.Comment: 13 pages, 1 figure, ApJL accepted for publicatio
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