2015
DOI: 10.1103/physrevd.92.084006
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Cosmological evolution of thermal relic particles inf(R)gravity

Abstract: By considering f (R) gravity models, the cosmic evolution is modified with respect to the standard ΛCDM scenario. In particular, the thermal history of particles results modified. In this paper, we derive the evolution of relics particles (WIMPs) assuming a reliable f (R) cosmological solution and taking into account observational constraints. The connection to the PAMELA experiment is also discussed. Results are consistent with constraints coming from BICEP2 and PLANCK experiments.

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Cited by 17 publications
(11 citation statements)
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“…It is well known that the physics of the universe at early times constitutes a great laboratory to explore physics beyond the standard cosmological model. For instance, torsion in f (T ) theories of gravity can be constrained by big bang nucleosynthesis [68], modifications on the evolution of the thermal relic particles (particles like WIMPs (weakly interactive massive particles)) within f (R) gravity context are also taken into account in [69]. Thus, it is worth noting that the nonzero ratio of baryon-to-entropy of the universe could be a potential quantity to constrain extended theories of gravity too.…”
Section: Discussionmentioning
confidence: 99%
“…It is well known that the physics of the universe at early times constitutes a great laboratory to explore physics beyond the standard cosmological model. For instance, torsion in f (T ) theories of gravity can be constrained by big bang nucleosynthesis [68], modifications on the evolution of the thermal relic particles (particles like WIMPs (weakly interactive massive particles)) within f (R) gravity context are also taken into account in [69]. Thus, it is worth noting that the nonzero ratio of baryon-to-entropy of the universe could be a potential quantity to constrain extended theories of gravity too.…”
Section: Discussionmentioning
confidence: 99%
“…Different values for the parameter ν appear in various modified cosmological scenarios [16,[115][116][117][118][119]: ν = 2 in Randall-Sundrum type II brane cosmology [120], ν = 1 in kination models [121][122][123], ν = 0 in cosmologies with an overall boost of the Hubble expansion rate like in the case of a large number of additional relativistic degrees of freedom in the thermal plasma [16], ν = 2/n − 2 in f (x) cosmology with f (x) = x + α x n , where x = R, T ; R and T being the scalar curvature and the scalar torsion, respectively [124][125][126][127]. 2 If the evolution of the Universe is adiabatic, and therefore the SM entropy is conserved, the temperature and the scale factor are related via…”
Section: Parametrizationmentioning
confidence: 99%
“…2 Investigations along these lines have been performed in different cosmological scenarios [63][64][65][66][67][68][69][70][71][72], where The parameter ν labels cosmological models: ν = 2 in Randall-Sundrum type II brane cosmology [73], ν = 1 in kination models [74][75][76][77], ν = 0 in cosmologies with an overall boost of the Hubble expansion rate [63], ν = − 0.8 in scalar-tensor cosmology [63,78], ν = 2/n − 2 in f (R) cosmology, with f (R) = R + α R n [79,80]. In terms of the modified expansion rate (3.2), it then follows that the inverse decay processes (2.6) takes the form…”
Section: Pev Neutrinos In Modified Cosmologiesmentioning
confidence: 99%