| Issue |
A&A
Volume 526, February 2011
|
|
|---|---|---|
| Article Number | L7 | |
| Number of page(s) | 4 | |
| Section | Letters | |
| DOI | https://doi.org/10.1051/0004-6361/201016140 | |
| Published online | 04 January 2011 | |
Letters to the Editor
The evolution of the cosmic microwave background temperature⋆
Measurements of TCMB at high redshift from carbon monoxide excitation
1
Departamento de AstronomíaUniversidad de Chile,
Casilla 36-D,
Santiago,
Chile
e-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.
; This email address is being protected from spambots. You need JavaScript enabled to view it.
2
Université Paris 6, Institut d’Astrophysique de Paris, CNRS UMR
7095, 98bis bd
Arago, 75014
Paris,
France
e-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.
3
Inter-University Centre for Astronomy and Astrophysics,
Post Bag 4,
Ganeshkhind, 411
007
Pune,
India
e-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.
4
European Southern Observatory, Alonso de Córdova 3107, Vitacura, Casilla 19001,
Santiago 19,
Chile
e-mail: This email address is being protected from spambots. You need JavaScript enabled to view it.
Received:
15
November
2010
Accepted:
13
December
2010
Abstract
A milestone of modern cosmology was the prediction and serendipitous discovery of the cosmic microwave background (CMB), the radiation leftover after decoupling from matter in the early evolutionary stages of the Universe. A prediction of the standard hot Big-Bang model is the linear increase with redshift of the black-body temperature of the CMB (TCMB). This radiation excites the rotational levels of some interstellar molecules, including carbon monoxide (CO), which can serve as cosmic thermometers. Using three new and two previously reported CO absorption-line systems detected in quasar spectra during a systematic survey carried out using VLT/UVES, we constrain the evolution of TCMB to z ~ 3. Combining our precise measurements with previous constraints, we obtain TCMB(z) = (2.725 ± 0.002) × (1 + z)1−β K with β = −0.007 ± 0.027, a more than two-fold improvement in precision. The measurements are consistent with the standard (i.e. adiabatic, β = 0) Big-Bang model and provide a strong constraint on the effective equation of state of decaying dark energy (i.e. weff = −0.996 ± 0.025).
Key words: cosmology: observations / cosmic background radiation / quasars: absorption lines
Based on observations carried out at the European Southern Observatory (ESO) using the Ultraviolet and Visual Echelle Spectrograph (UVES) at the Very Large Telescope (VLT, UT2-Kueyen) under Prgm. IDs 278.A-5062(A), 081.A-0334(B), 082.A-0544(A), and 083.A-0454(A).
© ESO, 2011
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