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From weak-scale observables to leptogenesis

Thermal leptogenesis is an attractive mechanism for generating the baryon asymmetry of the Universe. However, in supersymmetric models, the parameter space is severely restricted by the gravitino bound on the reheat temperature $T_{RH}$. For hierarchical light neutrino masses, it is shown that therm...

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Autor principal: Davidson, Sacha
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2003/03/037
http://cds.cern.ch/record/604969
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author Davidson, Sacha
author_facet Davidson, Sacha
author_sort Davidson, Sacha
collection CERN
description Thermal leptogenesis is an attractive mechanism for generating the baryon asymmetry of the Universe. However, in supersymmetric models, the parameter space is severely restricted by the gravitino bound on the reheat temperature $T_{RH}$. For hierarchical light neutrino masses, it is shown that thermal leptogenesis {\it can} work when $T_{RH} \sim 10^{9} $ GeV. The low-energy observable consequences of this scenario are $ BR(\tau \to \ell \gamma) \sim 10^{-8} - 10^{-9} $. For higher $T_{RH}$, thermal leptogenesis works in a larger area of parameter space, whose observable consequences are more ambiguous. A parametrisation of the seesaw in terms of weak-scale inputs is used, so the results are independent of the texture chosen for the GUT-scale Yukawa matrices.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
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spelling cern-6049692019-09-30T06:29:59Zdoi:10.1088/1126-6708/2003/03/037http://cds.cern.ch/record/604969engDavidson, SachaFrom weak-scale observables to leptogenesisParticle Physics - PhenomenologyThermal leptogenesis is an attractive mechanism for generating the baryon asymmetry of the Universe. However, in supersymmetric models, the parameter space is severely restricted by the gravitino bound on the reheat temperature $T_{RH}$. For hierarchical light neutrino masses, it is shown that thermal leptogenesis {\it can} work when $T_{RH} \sim 10^{9} $ GeV. The low-energy observable consequences of this scenario are $ BR(\tau \to \ell \gamma) \sim 10^{-8} - 10^{-9} $. For higher $T_{RH}$, thermal leptogenesis works in a larger area of parameter space, whose observable consequences are more ambiguous. A parametrisation of the seesaw in terms of weak-scale inputs is used, so the results are independent of the texture chosen for the GUT-scale Yukawa matrices.hep-ph/0302075IPPP-02-83DCPT-02-166CERN-TH-2003-006oai:cds.cern.ch:6049692003-02-11
spellingShingle Particle Physics - Phenomenology
Davidson, Sacha
From weak-scale observables to leptogenesis
title From weak-scale observables to leptogenesis
title_full From weak-scale observables to leptogenesis
title_fullStr From weak-scale observables to leptogenesis
title_full_unstemmed From weak-scale observables to leptogenesis
title_short From weak-scale observables to leptogenesis
title_sort from weak-scale observables to leptogenesis
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/1126-6708/2003/03/037
http://cds.cern.ch/record/604969
work_keys_str_mv AT davidsonsacha fromweakscaleobservablestoleptogenesis