Abstract

In the framework of the seesaw mechanism with three heavy right-handed Majorana neutrinos and no Higgs triplets we carry out a systematic study of the structure of the right-handed neutrino sector. Using the current low-energy neutrino data as an input and assuming hierarchical Dirac-type neutrino masses mDim_{Di}, we calculate the masses MiM_i and the mixing of the heavy neutrinos. We confront the inferred properties of these neutrinos with the constraints coming from the requirement of a successful baryogenesis via leptogenesis. In the generic case the masses of the right-handed neutrinos are highly hierarchical: MimDi2M_i \propto m_{Di}^2; the lightest mass is M1103106M_1 \approx 10^3 - 10^6 GeV and the generated baryon-to-photon ratio ηB1014\eta_B\lesssim 10^{-14} is much smaller than the observed value. We find the special cases which correspond to the level crossing points, with maximal mixing between two quasi-degenerate right-handed neutrinos. Two level crossing conditions are obtained: mee0{m}_{ee}\approx 0 (1-2 crossing) and d120d_{12}\approx 0 (2-3 crossing), where mee{m}_{ee} and d12d_{12} are respectively the 11-entry and the 12-subdeterminant of the light neutrino mass matrix in the basis where the neutrino Yukawa couplings are diagonal. We show that sufficient lepton asymmetry can be produced only in the 1-2 crossing where M1M2108M_1 \approx M_2 \approx 10^{8} GeV, M31014M_3 \approx 10^{14} GeV and (M2M1)/M2105(M_2 - M_1)/ M_2 \lesssim 10^{-5}.Comment: 30 pages, 2 eps figures, JHEP3.cls, typos corrected, note (and references) added on non-thermal leptogenesi

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    Last time updated on 01/04/2019