Bibcode
Scóccola, C. G.; Sánchez, Ariel G.; Rubiño-Martín, J. A.; Génova-Santos, R.; Rebolo, R.; Ross, A. J.; Percival, W. J.; Manera, M.; Bizyaev, D.; Brownstein, J. R.; Ebelke, G.; Malanushenko, E.; Malanushenko, V.; Oravetz, D.; Pan, K.; Schneider, D. P.; Simmons, A.
Bibliographical reference
Monthly Notices of the Royal Astronomical Society, Volume 434, Issue 2, p.1792-1807
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9
2013
Citations
12
Refereed citations
10
Description
We obtain constraints on the variation of the fundamental constants from
the full shape of the redshift-space correlation function of a sample of
luminous galaxies drawn from the Data Release 9 of the Baryonic
Oscillations Spectroscopic Survey. We combine this information with
additional data from recent cosmic microwave background, baryon acoustic
oscillations and H0 measurements. We focus on possible
variations of the fine structure constant α and the electron mass
me in the early Universe, and study the degeneracies between
these constants and other cosmological parameters, such as the dark
energy equation of state parameter wDE, the massive neutrinos
fraction fν, the effective number of relativistic species
Neff and the primordial helium abundance YHe. In
the case when only one of the fundamental constants is varied, our final
bounds are α / α _0 = 0.9957_{-0.0042}^{+0.0041} and m_e
/(m_e)_0 = 1.006_{-0.013}^{+0.014}. For the joint variation of both
fundamental constants, our results are α / α _0 =
0.9901_{-0.0054}^{+0.0055} and me/(me)0
= 1.028 ± 0.019. The variations of α and me from
their present values affect the bounds on other cosmological parameters.
Although when me is allowed to vary our constraints on
wDE are consistent with a cosmological constant, when α
is treated as a free parameter we find wDE = -1.20 ±
0.13; more than 1σ away from its standard value. When
fν and α are allowed to vary simultaneously, we find
fν < 0.043 (95 per cent confidence level, CL), implying
a limit of ∑mν < 0.46 eV (95 per cent CL), while
for me variation, we obtain fν < 0.086 (95
per cent CL), which implies ∑mν < 1.1 eV (95 per
cent CL). When Neff or YHe are considered as free
parameters, their simultaneous variation with α provides
constraints close to their standard values (when the H0 prior
is not included in the analysis), while when me is allowed to
vary, their preferred values are significantly higher. In all cases, our
results are consistent with no variations of α or me at
the 1σ or 2σ level.
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