vix.ing · top · new · best · stats · spec

Baryon Asymmetry in Neutrino Mass Models with and without θ13

2014/01/31 by Ng. K. Francis, Francis, Ng. K.
Physics and Astronomy · #Astrophysics and Cosmic Phenomena #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #Neutrino Physics Research #Particle physics theoretical and experimental studies #hep-ph

paper · pdf · doi:10.48550/arxiv.1401.8186

18 pages, 3 Tables, no figure

openalex publication_date 2014/01/31 · arxiv created 2014/03/26 · arxiv updated 2014/03/27 · openalex created_date 2024/04/10 · openalex updated_date 2026/07/28

Abstract

We investigate the comparative studies of cosmological baryon asymmetry in different neutrino mass models with and without θ13 by considering the three diagonal form of Dirac neutrino mass matrices, down-quark (4,2), up-quark (8,4) and charged lepton (6,2). The predictions of any models with θ13 are consistent in all the three stages of leptogenesis calculations and the results are better than the predictions of any models without θ13 which are consistent in a piecemeal manner with the observational data. For the best model, the normal hierarchy Type-IA for charged lepton (6,2) without θ13, the predicted inflaton mass required to produce the observed baryon asymmetry is found to be 3.6x10 to the power 10 GeV corresponding to reheating temperature TR 4.5x10 to the power 6 GeV, while for the same model with θ13, the inflaton mass is 2.24x10 to the power 11 GeV, TR 4.865x10 to the power 6 GeV and weak scale gravitino mass m(2 divided by 3) 100 GeV without causing the gravitino problem. These values apply to the recent discovery of Higgs boson of mass 125 GeV. The relic abundance of gravitino is proportional to the reheating temperature of the thermal bath. One can have the right order of relic dark matter abundance only if the reheating temperature is bounded to below 10 to the power 7 GeV.

Related