Abstract

We explore the possible values of the mu rightarrow e gamma branching ratio, text {BR}(mu rightarrow egamma ), and the electron dipole moment (eEDM), d_e, in no-scale SU(5) super-GUT models with the boundary conditions that soft supersymmetry-breaking matter scalar masses vanish at some high input scale, M_mathrm{in}, above the GUT scale, M_{mathrm{GUT}}. We take into account the constraints from the cosmological cold dark matter density, Omega _{CDM} h^2, the Higgs mass, M_h, and the experimental lower limit on the lifetime for p rightarrow K^+ bar{nu }, the dominant proton decay mode in these super-GUT models. Reconciling this limit with Omega _{CDM} h^2 and M_h requires the Higgs field responsible for the charge-2/3 quark masses to be twisted, and possibly also that responsible for the charge-1/3 and charged-lepton masses, with model-dependent soft supersymmetry-breaking masses. We consider six possible models for the super-GUT initial conditions, and two possible choices for quark flavor mixing, contrasting their predictions for proton decay with versions of the models in which mixing effects are neglected. We find that tau left( prightarrow K^+ bar{nu }right) may be accessible to the upcoming Hyper-Kamiokande experiment, whereas all the models predict text {BR}(mu rightarrow egamma ) and d_e below the current and prospective future experimental sensitivities or both flavor choices, when the dark matter density, Higgs mass and current proton decay constraints are taken into account. However, there are limited regions with one of the flavor choices in two of the models where mu rightarrow e conversion on a heavy nucleus may be observable in the future. Our results indicate that there is no supersymmetric flavor problem in the class of no-scale models we consider.

Highlights

  • Supersymmetry remains an attractive prospective extension of the Standard Model (SM), despite its non-appearance during Runs 1 and 2 of the LHC [1,2,3,4,5,6]

  • We explore the possible values of the μ → eγ branching ratio, BR(μ → eγ ), and the electron dipole moment, de, in no-scale SU(5) super-GUT models with the boundary conditions that soft supersymmetrybreaking matter scalar masses vanish at some high input scale, Min, above the GUT scale, MGUT

  • The continuing absence of supersymmetry at the LHC [1,2,3,6] reinforces the need to seek complementary indications of supersymmetry outside colliders. It is in this context that we address the questions of proton decay, contributions to the electron dipole moment and μ flavor violation observables in the SU(5) models based on no-scale supergravity that were introduced in [29]

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Summary

Introduction

Supersymmetry remains an attractive prospective extension of the Standard Model (SM), despite its non-appearance during Runs 1 and 2 of the LHC [1,2,3,4,5,6]. An issue discussed in [29], namely how to obtain the correct mass of the observed Higgs boson and the cold dark matter density in no-scale supergravity models, while avoiding proton decay in violation of the current limits. 2 we introduce the class of no-scale SU(5) super-GUT models we study, including the specification of different choices for the embedding of MSSM fields in GUT multiplets and the corresponding Ansätze for matter Yukawa coupling matrices, the noscale boundary conditions on soft supersymmetry breaking at Min, and our treatment of the renormalization-group running down to the electroweak scale.

Model framework
Soft supersymmetry breaking
Renormalization-group running of parameters
Hd m2H
Proton decay
Flavor violation
Models
Both Higgs fields in twisted sectors
Models in which only His twisted
Findings
Overview and conclusions
Full Text
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