The Impact of Non-zero \theta_{13} on Neutrino Mass and Leptogenesis in a SUSY SO(10) Model
The recent measurement of the reactor angle as $\sin^2 2\theta_{13} = 0.092 \pm 0.016(stat) \pm 0.005(syst)$ come from the Daya Bay collaboration. Evidence of nonzero \theta_{13} was also there at T2K, MINOS and Double Chooz experiments. We study the implication of these recent data on neutrino mass...
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Zusammenfassung: | The recent measurement of the reactor angle as $\sin^2 2\theta_{13} = 0.092
\pm 0.016(stat) \pm 0.005(syst)$ come from the Daya Bay collaboration. Evidence
of nonzero \theta_{13} was also there at T2K, MINOS and Double Chooz
experiments. We study the implication of these recent data on neutrino mass
matrix and consequently on leptogenesis in a supersymmetric SO(10) model. To
explain the smallness of neutrino mass, in general, we require a heavy Majorana
neutrino which is a natural candidate in SO(10) model. In minimal SO(10) model,
the symmetry breaking scale or the right-handed neutrino mass scale is close to
the GUT scale. It is not only beyond the reach of any present or future
collider search but the lepton asymmetry generated from its decay is in
conflict with the gravitino constraint as well as unable to fit the neutrino
data. We show that addition of an extra fermion singlet can accommodate the
observed recent neutrino data in a supersymmetric SO(10) model. This model can
generate the desired lepton asymmetry and provide TeV scale doubly-charged
Higgs scalars to be detected at LHC. |
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DOI: | 10.48550/arxiv.1205.4751 |