Issue |
A&A
Volume 561, January 2014
|
|
---|---|---|
Article Number | A143 | |
Number of page(s) | 12 | |
Section | Cosmology (including clusters of galaxies) | |
DOI | https://doi.org/10.1051/0004-6361/201322632 | |
Published online | 27 January 2014 |
Measurement of the TCMB evolution from the Sunyaev-Zel’dovich effect
1
Institut d’Astrophysique Spatiale, CNRS (UMR8617) Université Paris-Sud
11, Bâtiment 121,
91405
Orsay Cedex,
France
e-mail:
ghurier@ias.u-psud.fr
2
CNRS, IRAP, 9
Av. colonel Roche, BP
44346, 31028
Toulouse Cedex 4,
France
3
Université de Toulouse, UPS-OMP, IRAP,
31400
Toulouse,
France
Received:
9
September
2013
Accepted:
27
November
2013
In the standard hot cosmological model, the black-body temperature of the cosmic microwave background (CMB), TCMB, increases linearly with redshift. Across the line of sight CMB photons interact with the hot (~ 107−8 K ) and diffuse gas of electrons from galaxy clusters. This interaction leads to the well-known thermal Sunyaev-Zel’dovich effect (tSZ), which produces a distortion of the black-body emission law, depending on TCMB. Using tSZ data from the Planck satellite, it is possible to constrain TCMB below z = 1. Focusing on the redshift dependance of TCMB, we obtain TCMB(z) = (2.726 ± 0.001) × (1 + z)1−β K with β = 0.009 ± 0.017, which improves on previous constraints. Combined with measurements of molecular species absorptions, we derive β = 0.006 ± 0.013. These constraints are consistent with the standard (i.e. adiabatic, β = 0) Big-Bang model.
Key words: cosmology: observations / cosmic background radiation / galaxies: clusters: general
© ESO, 2014
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