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On Higgs and sphaleron effects during the leptogenesis era
Author(s) -
Enrico Nardi,
Yosef Nir,
J. Racker,
Esteban Roulet
Publication year - 2006
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 - 10.1088/1126-6708/2006/01/068
Subject(s) - leptogenesis , baryon asymmetry , particle physics , physics , sphaleron , asymmetry , baryogenesis , electroweak interaction , lepton , higgs boson , nuclear physics , electron
We discuss the effects of various processes that can be active during theleptogenesis era, and present the Boltzmann equations that take them intoaccount appropriately. A non-vanishing Higgs number asymmetry is alwayspresent, enhancing the washout of the lepton asymmetry. This is the main neweffect when leptogenesis takes place at $T>10^{12}$ GeV, reducing the finalbaryon asymmetry and tightening the leptogenesis bound on the neutrino masses.If leptogenesis occurs at lower temperatures, electroweak sphalerons partiallytransfer the lepton asymmetry to a baryonic one, while Yukawa interactions andQCD sphalerons partially transfer the asymmetries of the left-handed fields tothe right-handed ones, suppressing the washout processes. Depending on thespecific temperature range in which leptogenesis occurs, the final baryonasymmetry can be enhanced or suppressed by factors of order 20%--40% withrespect to the case when these effects are altogether ignored.Comment: one reference adde

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