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Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages

Absent any indirect tests on the thermal history of the Universe prior to the formation of light nuclear elements, it is legitimate to investigate situations where, before nucleosyntheis, the sound speed of the plasma was larger than $c/\sqrt{3}$, at most equalling the speed of light $c$. In this pl...

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Autor principal: Giovannini, Massimo
Lenguaje:eng
Publicado: 2008
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2008.07.107
http://cds.cern.ch/record/1115023
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author Giovannini, Massimo
author_facet Giovannini, Massimo
author_sort Giovannini, Massimo
collection CERN
description Absent any indirect tests on the thermal history of the Universe prior to the formation of light nuclear elements, it is legitimate to investigate situations where, before nucleosyntheis, the sound speed of the plasma was larger than $c/\sqrt{3}$, at most equalling the speed of light $c$. In this plausible extension of the current cosmological paradigm, hereby dubbed Tensor-$\Lambda$CDM (i.e. T$\Lambda$CDM) scenario, high-frequency gravitons are copiously produced. Without conflicting with the bounds on the tensor to scalar ratio stemming from the combined analysis of the three standard cosmological data sets (i.e. cosmic microwave background anisotropies, large-scale structure and supenovae), the spectral energy density of the relic gravitons in the T$\Lambda$CDM scenario can be potentially observable by wide-band interferometers (in their advanced version) operating in a frequency window which ranges between few Hz and few kHz.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-11150232023-03-15T19:11:21Zdoi:10.1016/j.physletb.2008.07.107http://cds.cern.ch/record/1115023engGiovannini, MassimoStochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff agesAstrophysics and AstronomyAbsent any indirect tests on the thermal history of the Universe prior to the formation of light nuclear elements, it is legitimate to investigate situations where, before nucleosyntheis, the sound speed of the plasma was larger than $c/\sqrt{3}$, at most equalling the speed of light $c$. In this plausible extension of the current cosmological paradigm, hereby dubbed Tensor-$\Lambda$CDM (i.e. T$\Lambda$CDM) scenario, high-frequency gravitons are copiously produced. Without conflicting with the bounds on the tensor to scalar ratio stemming from the combined analysis of the three standard cosmological data sets (i.e. cosmic microwave background anisotropies, large-scale structure and supenovae), the spectral energy density of the relic gravitons in the T$\Lambda$CDM scenario can be potentially observable by wide-band interferometers (in their advanced version) operating in a frequency window which ranges between few Hz and few kHz.Absent any indirect tests on the thermal history of the Universe prior to the formation of light nuclear elements, it is legitimate to investigate situations where, before nucleosynthesis, the sound speed of the plasma was larger than c/3 , at most equalling the speed of light c . In this plausible extension of the current cosmological paradigm, hereby dubbed Tensor-ΛCDM (i.e. TΛCDM) scenario, high-frequency gravitons are copiously produced. Without conflicting with the bounds on the tensor to scalar ratio stemming from the combined analysis of the three standard cosmological data sets (i.e. cosmic microwave background anisotropies, large-scale structure and supenovae), the spectral energy density of the relic gravitons in the TΛCDM scenario can be potentially observable by wide-band interferometers (in their advanced version) operating in a frequency window which ranges between few Hz and few kHz.Absent any indirect tests on the thermal history of the Universe prior to the formation of light nuclear elements, it is legitimate to investigate situations where, before nucleosyntheis, the sound speed of the plasma was larger than $c/\sqrt{3}$, at most equalling the speed of light $c$. In this plausible extension of the current cosmological paradigm, hereby dubbed Tensor-$\Lambda$CDM (i.e. T$\Lambda$CDM) scenario, high-frequency gravitons are copiously produced. Without conflicting with the bounds on the tensor to scalar ratio stemming from the combined analysis of the three standard cosmological data sets (i.e. cosmic microwave background anisotropies, large-scale structure and supenovae), the spectral energy density of the relic gravitons in the T$\Lambda$CDM scenario can be potentially observable by wide-band interferometers (in their advanced version) operating in a frequency window which ranges between few Hz and few kHz.arXiv:0807.1914CERN-PH-TH-2008-151CERN-PH-TH-2008-151oai:cds.cern.ch:11150232008-07-14
spellingShingle Astrophysics and Astronomy
Giovannini, Massimo
Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title_full Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title_fullStr Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title_full_unstemmed Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title_short Stochastic backgrounds of relic gravitons, T$\Lambda$CDM paradigm and the stiff ages
title_sort stochastic backgrounds of relic gravitons, t$\lambda$cdm paradigm and the stiff ages
topic Astrophysics and Astronomy
url https://dx.doi.org/10.1016/j.physletb.2008.07.107
http://cds.cern.ch/record/1115023
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