2019
DOI: 10.1007/jhep09(2019)065
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Leptogenesis after superconformal subcritical hybrid inflation

Abstract: We consider an extended version of superconformal subcritical hybrid inflation model by introducing three right-handed neutrinos that have Majorana mass terms. In the model one of the right-handed sneutrinos plays a role of the inflaton field, and it decays to reheat the universe after inflation. Vacuum expectation value for the waterfall field gives an unconventional pattern of the light neutrino mass matrix, and the neutrino Yukawa couplings that determine the reheating temperature are not constrained by the… Show more

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Cited by 6 publications
(10 citation statements)
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References 76 publications
(115 reference statements)
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“…From the superpotential, the light neutrinos acquire masses in the seesaw mechanism [107][108][109][110][111][112]. In our model, however, S + obtains a vacuum expectation value (VEV), denoted as S + , at the global minimum, which leads to an unconventional mass matrix for the light neutrinos [105]. In addition, the components of the mass matrices are given in a limited number of parameters due to A 4 symmetry, which results in the characteristic pattern of the neutrino mixing and CP phases in the lepton sector.…”
Section: Neutrino Masses and Mixing Patternmentioning
confidence: 89%
See 3 more Smart Citations
“…From the superpotential, the light neutrinos acquire masses in the seesaw mechanism [107][108][109][110][111][112]. In our model, however, S + obtains a vacuum expectation value (VEV), denoted as S + , at the global minimum, which leads to an unconventional mass matrix for the light neutrinos [105]. In addition, the components of the mass matrices are given in a limited number of parameters due to A 4 symmetry, which results in the characteristic pattern of the neutrino mixing and CP phases in the lepton sector.…”
Section: Neutrino Masses and Mixing Patternmentioning
confidence: 89%
“…We notice that the lightest neutrino mass becomes zero since rank of M ν is two [105]. Therefore, by imposing the condition in which the neutrino mass squared differences are within 3σ range of the observed values, the cosmological upper bound on the sum of light neutrino masses [113,114] i…”
Section: ŷmentioning
confidence: 91%
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“…3 The opposite scenario, κ ≪ g, has been considered in [62,63] (see also [64][65][66][67]), which results in a super-Planckian critical field value, s crit > M Pl . In this case, inflation occurs during the waterfall transition and leads to an O (0.1) tensor-to-scalar ratio.…”
Section: Introductionmentioning
confidence: 99%