English

Understanding for flavor physics in the lepton sector

High Energy Physics - Phenomenology 2012-12-03 v3

Abstract

In this paper, we give a model for understanding flavor physics in the lepton sector--mass hierarchy among different generations and neutrino mixing pattern. The model is constructed in the framework of supersymmetry, with a family symmetry S4U(1)S4*U(1). There are two right-handed neutrinos introduced for seesaw mechanism, while some standard model(SM) gauge group singlet fields are included which transforms non-trivially under family symmetry. In the model, each order of contributions are suppressed by δ0.1\delta \sim 0.1 compared to the previous one. In order to reproduce the mass hierarchy, mτm_\tau and Δmatm2\sqrt{\Delta m_{atm}^2}, mμm_\mu and Δmsol2\sqrt{\Delta m_{sol}^2} are obtained at leading-order(LO) and next-to-leading-order(NLO) respectively, while electron can only get its mass through next-to-next-to-next-to-leading-order(NNNLO) contributions. For neutrino mixing angels, θ12,θ23,θ13\theta_{12}, \theta_{23}, \theta_{13} are 45,45,045^\circ, 45^\circ, 0 i.e. Bi-maximal mixing pattern as first approximation, while higher order contributions can make them consistent with experimental results. As corrections for θ12\theta_{12} and θ13\theta_{13} originate from the same contribution, there is a relation predicted for them sinθ13=1tanθ121+tanθ12\sin{\theta_{13}}=\displaystyle \frac{1-\tan{\theta_{12}}}{1+\tan{\theta_{12}}}. Besides, deviation from π4\displaystyle \frac{\pi}{4} for θ23\theta_{23} should have been as large as deviation from 0 for θ13\theta_{13} if it were not the former is suppressed by a factor 4 compared to the latter.

Keywords

Cite

@article{arxiv.1207.2545,
  title  = {Understanding for flavor physics in the lepton sector},
  author = {Zhen-hua Zhao},
  journal= {arXiv preprint arXiv:1207.2545},
  year   = {2012}
}

Comments

version to appear in Phys. Rev. D

R2 v1 2026-06-21T21:33:46.014Z