Abstract

We explore proton decay in a class of realistic supersymmetric flipped SU(5) models supplemented by a U(1)R symmetry which plays an essential role in implementing hybrid inflation. Two distinct neutrino mass models, based on inverse seesaw and type I seesaw, are identified, with the latter arising from the breaking of U(1)R by nonrenormalizable superpotential terms. Depending on the neutrino mass model an appropriate set of intermediate scale color triplets from the Higgs superfields play a key role in proton decay channels that include p → (e+, μ+) π0, p → (e+, μ+) K0, p → overline{v}{pi}^{+} , and p → overline{v}{K}^{+} . We identify regions of the parameter space that yield proton lifetime estimates which are testable at Hyper-Kamiokande and other next generation experiments. We discuss how gauge coupling unification in the presence of intermediate scale particles is realized, and a Z4 symmetry is utilized to show how such intermediate scales can arise in flipped SU(5). Finally, we compare our predictions for proton decay with previous work based on SU(5) and flipped SU(5).

Highlights

  • JHEP02(2021)181 two models of light neutrino masses

  • We explore proton decay in a class of realistic supersymmetric flipped SU(5) models supplemented by a U(1)R symmetry which plays an essential role in implementing hybrid inflation

  • Proton decay with lifetimes accessible at Hyper-K and other future experiments are explored in a flipped SU(5) model of supersymmetric hybrid inflation supplemented by a global U(1)R symmetry

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Summary

Neutrino masses

The dimension four rapid proton decay mediated through the color triplet, Dc ⊂ 101, can appear at nonrenormalizable level via the following operators, S10H 10i10j5k m2P. Later we discuss the proton decay mediation by the color triplets from 10H , 10H by allowing explicit R-symmetry breaking terms with R-charge zero at the nonrenormalizable level. The numerical estimates of partial proton lifetime for charged lepton decay channels are shown in figure 3 as a function of the triplet mass MT = Mλ = Mλ, with tan β values in the range 2 ≤ tan β ≤ 60. GUT models the estimates of branching fractions play a pivotal role For this purpose a variation of various branching fractions with respect to color triplet mass MT = Mλ = Mλ for tan β in the range 2 ≤ tan β ≤ 60 is shown in figure 6. The branching fraction of ν K+ channel plays a key role in making distinctive comparison of the current model with the other models of flipped SU(5) [32, 38] where this channel is highly suppressed

Z4 symmetry and color triplet masses
Gauge coupling unification
Conclusion
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