English

Generalized Friedberg-Lee model for CP violation in neutrino physics

High Energy Physics - Phenomenology 2012-11-20 v1

Abstract

We propose a phenomenological model of Dirac neutrino mass operator based on the Fridberg-Lee (FL) neutrino mass model to include CP violation. By considering the most general set of complex coefficients, and imposing the condition that the mass eigenvalues are real, we find a neutrino mass matrix which is non-hermitian, symmetric and magic. In particular, we find that the requirement of obtaining real mass eigenvalues by transferring the residual phases to the mass eigenstates self-consistently, dictates the following relationship between the imaginary part of the mass matrix elements BB and the parameters of the FL model: B=±3/4(abr)2sin22θ13cos2θ12B=\pm\sqrt{3/4(a-b_{r})^{2}\sin^{2}2\theta_{13}\cos^{2}\theta_{12}}. We obtain inverted neutrino mass hierarchy, m3=0m_{3}=0. Making a correspondence between our model and the experimental data produces stringent conditions on the parameters as follows: 35.06θ1236.2735.06^{\circ}\lesssim\theta_{12}\lesssim36.27^{\circ}, θ23=45\theta_{23}= 45^{\circ}, 7.27θ1311.097.27^{\circ}\lesssim\theta_{13}\lesssim11.09^{\circ}, and 82.03δ85.3782.03^{\circ}\lesssim\delta\lesssim85.37^{\circ}. We get mildly broken μτ\mu-\tau symmetry, which reduces the resultant neutrino mixing pattern from tribimaximal (TBM) to trimaximal (TM). The CP violation as measured by the Jarlskog parameter is restricted by 0.027J0.0440.027\lesssim J\lesssim0.044.

Keywords

Cite

@article{arxiv.1211.4389,
  title  = {Generalized Friedberg-Lee model for CP violation in neutrino physics},
  author = {N. Razzaghi and S. S. Gousheh},
  journal= {arXiv preprint arXiv:1211.4389},
  year   = {2012}
}

Comments

8 pages, 3 figures, published in Phys. Rev. D