Abstract

Realistic neutrino mixing is achieved at one-loop level radiatively using $S3\times Z_2$ symmetry. The model comprises of two right-handed neutrinos, maximally mixed to produce the structure of the left-handed Majorana neutrino mass matrix characterized by $\theta_{13}=0$, $\theta_{23}=\pi/4$ and any value of $\theta_{12}^0$ particular to the Tribimaximal (TBM), Bimaximal (BM) and Golden Ratio (GR) or other mixings. A small deviation from this maximal mixing between the two right-handed neutrinos could generate non-zero $\theta_{13}$, shifts of the atmospheric mixing angle $\theta_{23}$ from $\pi/4$ and also could correct the solar mixing angle $\theta_{12}$ by a small amount altogether in a single step. In this scotogenic mechanism of generating non-zero $\theta_{13}$ by shifting from maximal mixing in the right-handed neutrino sector, two $Z_2$ odd inert scalar $SU(2)_L$ doublets were used, the lightest of which can serve as a dark matter candidate.

Highlights

  • Neutrinos oscillate owing to their massive nature as established by the oscillation experiments

  • Nonzero θ13, though small in comparison to the other mixing angles, was discovered in 2012 by the shortbaseline reactor antineutrino experiments [1]. Before these nonzero θ13 results, models were studied in literature that correspond to the tribimaximal (TBM), bimaximal (BM), and golden ratio (GR) mixings

  • M0 in Eq (21) will represent the form of left-handed neutrino mass matrix needed for θ13 1⁄4 0, θ23 1⁄4 π=4, and θ012 of the popular mixing types as in Eq (4) when we identify a0 ≡ y21v21⁄24r12λ123 þ 2r11λ12Š 1⁄4 y21v21⁄24r12ðλ3 þ λ1 − λ2Þ þ 2r11ðλ1 þ λ2ފ

Read more

Summary

Introduction

Neutrinos oscillate owing to their massive nature as established by the oscillation experiments. Nonzero θ13, though small in comparison to the other mixing angles, was discovered in 2012 by the shortbaseline reactor antineutrino experiments [1] Before these nonzero θ13 results, models were studied in literature that correspond to the tribimaximal (TBM), bimaximal (BM), and golden ratio (GR) mixings (that we onwards collectively refer to as popular lepton mixings). All these mixings have θ13 1⁄4 0, θ23 1⁄4 π=4, and tuning θ012 to the specific values as shown in Table I produced the different mixing patterns viz. TBM, BM, and GR

Objectives
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call