Abstract

A simple extension of Ma's approach in a scotogenic model is studied for the purpose of simultaneously interpreting the neutrino data and the excess of muon anomalous magnetic moment (muon $g-2$). The feasible minimal extension is to add an $Z_2$-odd vector-like lepton doublet to the Ma's model. It is found that in addition to the neutrino data, the strict constraints on the relevant parameters are from the electroweak oblique parameters and the induced lepton-flavor violation processes, such as $\ell_i \to \ell_j \gamma$ and $\ell_i \to \ell^-_j \ell^-_j \ell^+_j$. Performing parameter scan, we numerically demonstrate that when the constraint conditions are satisfied, the muon $g-2$ of $O(10^{-9})$ can be achieved, where it can be expected that with a $5\sigma$ observation, the Muon $g-2$ experiment at Fermilab can observe $a_\mu \approx 13.31 \times 10^{-10}$ when the current experiment and the SM errors are reduced by a factor of 4 and 2, respectively. Moreover, the branching ratio of the $\tau \to \mu \gamma$ decay can match the Belle II sensitivity of $O(10^{-9})$ with an integrated luminosity of 50 ab$^{-1}$.

Highlights

  • In addition to the origin of neutrino mass, a clear hint for new physics is the muon anomalous magnetic moment

  • We will show that the 11 free parameters can be accommodated in the model when all constraints from the electroweak oblique parameters, the lepton flavor violation (LFV) processes, and the neutrino data are satisfied; and the muon g − 2 can still reach the level of 10−9

  • Based on the scotogenic model proposed in [27], we extend the model by including a Z2-odd vectorlike lepton doublet (X) in order to resolve the muon g − 2 excess through the mediation of an inert charged Higgs boson

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Summary

INTRODUCTION

In addition to the origin of neutrino mass, a clear hint for new physics is the muon anomalous magnetic moment (muon g − 2). We will show that the 11 free parameters can be accommodated in the model when all constraints from the electroweak oblique parameters, the LFV processes, and the neutrino data are satisfied; and the muon g − 2 can still reach the level of 10−9. In order to generate the neutrino mass through a one-loop radiative mechanism and provide the dark matter candidate, we add three right-handed neutrinos Nk 1⁄4 ð1; 0Þ (k 1⁄4 1, 2, 3) and one inert Higgs doublet HI 1⁄4 ð2; 1Þ to the SM [27], where both Nk and HI are Z2-odd states, and numbers in brackets denote the SUð2ÞL representation and Uð1ÞY hypercharge, respectively. In addition to Nk, which is free from the mixing with the SM neutrino [27], in principle, the new neutral lepton χ

Yukawa couplings and mass splitting in dark lepton doublet
Scalar potential and gauge couplings to dark sector
Radiative neutrino mass
Lepton anomalous magnetic dipole moment
NUMERICAL ANALYSIS
Allowed parameter spaces from the parameter scan
SUMMARY
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