English

Neutrino Mass Spectrum for Co-Bimaximal Mixings from Quantum Gravity

High Energy Physics - Phenomenology 2019-08-23 v1

Abstract

We consider non-renormalizable interaction term as a perturbation of the conventional neutrino mass matrix. Quantum gravitational (Planck scale )effects lead to an effective SU(2)L×U(1)SU(2)_L\times U(1) invariant dimension-5 Lagrangian involving neutrino and Higgs fields,On symmetry breaking, this operator gives rise to correction to the neutrino masses and mixing. The gravitational interaction MX=MplM_X=M_{pl} which gives rise to additional terms in neutrino mass matrix. We also assume that, just above the electroweak breaking scale, neutrino masses are nearly degenerate and their mixing is Co-bimaximal mixing by assuming mixing angle θ130=10o\theta_{13}\neq0 = 10^{o}, θ23=π4\theta_{23}=\frac{\pi}{4}, tanθ122=13sinθ1322=34o\tan\theta_{12}^ 2 = \frac{1-3sin\theta_{13}^2}{2} = 34^{o} and Dirac phase δ=±π2\delta=\pm\frac{\pi}{2}.There additional term can be considered to be perturbation of the GUT scale Co-bimaximal neutrino mass matrix. The relation consider with solar and atmospheric neutrino oscillation data predicted above GUT scale m10.00001eV0.00003eVm_1' \simeq 0.00001eV-0.00003eV, m20.00008eV0.00012m_2' \simeq 0.00008eV-0.00012, and m30.000207eV000320eVm_3' \simeq 0.000207eV-000320eV.

Keywords

Cite

@article{arxiv.1908.08387,
  title  = {Neutrino Mass Spectrum for Co-Bimaximal Mixings from Quantum Gravity},
  author = {Bipin Singh Koranga},
  journal= {arXiv preprint arXiv:1908.08387},
  year   = {2019}
}

Comments

10 pages. arXiv admin note: substantial text overlap with arXiv:1006.5553, arXiv:0810.4394