Abstract

We study the possibility that the lepton-flavor changing process can induce the suitable magnitude of the muon anomalous magnetic moment (g_\mu -2) in the decoupling solution to the flavor problem in the minimal supersymmetric standard model. Our analyses introduce the flavor mixings of left- and right-handed stau and smuon phenomenologically. It is found that if both the left- and right-handed sleptons have sizable flavor mixings, the correction to g_\mu -2 from the lighter slepton can reach to 10^{-9} while the correction to the branching ratio of \tau \to \mu \gamma satisfies the current experimental bound. On the other hand, when only the left-handed or right-handed sleptons have the large flavor mixing, the suitable magnitude of the correction to g_\mu-2 is not realized owing to the experimental bound of \tau \to \mu \gamma.

Highlights

  • We study the possibility that the lepton-flavor changing process can induce the suitable magnitude of the muon anomalous magnetic moment in the decoupling solution to the flavor problem in the minimal supersymmetric standard model

  • If the energy scale of the SUSY-breaking mediation to the minimal supersymmetric (SUSY) standard model (MSSM) is higher than the mass scale of the right-handed neutrino, this spectrum should be realized so that the tau-neutrino Yukawa coupling does not destabilize the naturalness of the Higgs boson mass

  • We examine the possibility that the lepton-flavor changing process can induce the suitable magnitude of the muon anomalous magnetic moment in the decoupling solution to the flavor problem

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Summary

Introduction

We study the possibility that the lepton-flavor changing process can induce the suitable magnitude of the muon anomalous magnetic moment (gμ − 2) in the decoupling solution to the flavor problem in the minimal supersymmetric standard model. When only the left-handed sleptons have a large mixing between the second and third generations, the supersymmetric contribution to gμ −2 is constrained to be smaller than 10−10 from the experimental bound of τ → μγ.

Results
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