Cargando…
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...
Autores principales: | , , |
---|---|
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 |
_version_ | 1780905760145801216 |
---|---|
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. |
id | cern-828539 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2005 |
record_format | invenio |
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 |