From weak-scale observables to leptogenesis
Author(s) -
Sacha Davidson
Publication year - 2003
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2003/03/037
Subject(s) - leptogenesis , physics , particle physics , baryon asymmetry , yukawa potential , gravitino , observable , seesaw molecular geometry , neutrino , asymmetry , supersymmetry , nuclear physics , lepton , quantum mechanics , supergravity , electron
Thermal leptogenesis is an attractive mechanism for generating the baryonasymmetry of the Universe. However, in supersymmetric models, the parameterspace is severely restricted by the gravitino bound on the reheat temperature$T_{RH}$. For hierarchical light neutrino masses, it is shown that thermalleptogenesis {\it can} work when $T_{RH} \sim 10^{9} $ GeV. The low-energyobservable consequences of this scenario are $ BR(\tau \to \ell \gamma) \sim10^{-8} - 10^{-9} $. For higher $T_{RH}$, thermal leptogenesis works in alarger area of parameter space, whose observable consequences are moreambiguous. A parametrisation of the seesaw in terms of weak-scale inputs isused, so the results are independent of the texture chosen for the GUT-scaleYukawa matrices.Comment: a few references adde
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