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Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model

The gravitino problem gives a severe constraint on the thermal leptogenesis scenario. This problem leads us to consider some alternatives to it if we try to keep the gravitino mass around the weak scale $m_{3/2} \sim 100$ GeV. We consider, in this paper, the non-thermal leptogenesis scenario in the...

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Detalles Bibliográficos
Autores principales: Fukuyama, T, Kikuchi, T, Osaka, T
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1475-7516/2005/06/005
http://cds.cern.ch/record/828539
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author Fukuyama, T
Kikuchi, T
Osaka, T
author_facet Fukuyama, T
Kikuchi, T
Osaka, T
author_sort Fukuyama, T
collection CERN
description The gravitino problem gives a severe constraint on the thermal leptogenesis scenario. This problem leads us to consider some alternatives to it if we try to keep the gravitino mass around the weak scale $m_{3/2} \sim 100$ GeV. We consider, in this paper, the non-thermal leptogenesis scenario in the framework of a minimal supersymmetric SO(10) model. Even if we start with the same minimal SO(10) model, we have different predictions for low-energy phenomenologies dependent on the types of seesaw mechanism. This is the case for leptogenesis: it is shown that the type-I see-saw model gives a consistent scenario for the non-thermal leptogenesis but not for type-II. The predicted inflaton mass needed to produce the observed baryon asymmetry of the universe is found to be $M_I \sim 5 \times 10^{11}$ GeV for the reheating temperature $T_R = 10^6$ GeV.
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spelling cern-8285392019-09-30T06:29:59Zdoi:10.1088/1475-7516/2005/06/005http://cds.cern.ch/record/828539engFukuyama, TKikuchi, TOsaka, TNon-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) ModelParticle Physics - PhenomenologyThe gravitino problem gives a severe constraint on the thermal leptogenesis scenario. This problem leads us to consider some alternatives to it if we try to keep the gravitino mass around the weak scale $m_{3/2} \sim 100$ GeV. We consider, in this paper, the non-thermal leptogenesis scenario in the framework of a minimal supersymmetric SO(10) model. Even if we start with the same minimal SO(10) model, we have different predictions for low-energy phenomenologies dependent on the types of seesaw mechanism. This is the case for leptogenesis: it is shown that the type-I see-saw model gives a consistent scenario for the non-thermal leptogenesis but not for type-II. The predicted inflaton mass needed to produce the observed baryon asymmetry of the universe is found to be $M_I \sim 5 \times 10^{11}$ GeV for the reheating temperature $T_R = 10^6$ GeV.hep-ph/0503201oai:cds.cern.ch:8285392005-03-21
spellingShingle Particle Physics - Phenomenology
Fukuyama, T
Kikuchi, T
Osaka, T
Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title_full Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title_fullStr Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title_full_unstemmed Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title_short Non-thermal Leptogenesis and a Prediction of Inflaton Mass in a Supersymmetric SO(10) Model
title_sort non-thermal leptogenesis and a prediction of inflaton mass in a supersymmetric so(10) model
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/1475-7516/2005/06/005
http://cds.cern.ch/record/828539
work_keys_str_mv AT fukuyamat nonthermalleptogenesisandapredictionofinflatonmassinasupersymmetricso10model
AT kikuchit nonthermalleptogenesisandapredictionofinflatonmassinasupersymmetricso10model
AT osakat nonthermalleptogenesisandapredictionofinflatonmassinasupersymmetricso10model