R-symmetric flipped SU(5)

A bstract We construct a supersymmetric flipped SU(5) grand unified model that possesses an R symmetry. This R symmetry forbids dangerous non-renormalizable operators suppressed by a cut-off scale up to sufficiently large mass dimensions so that the SU(5)-breaking Higgs field develops a vacuum expec...

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Veröffentlicht in:The journal of high energy physics 2020-11, Vol.2020 (11), Article 140
Hauptverfasser: Hamaguchi, Koichi, Hor, Shihwen, Nagata, Natsumi
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Sprache:eng
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Zusammenfassung:A bstract We construct a supersymmetric flipped SU(5) grand unified model that possesses an R symmetry. This R symmetry forbids dangerous non-renormalizable operators suppressed by a cut-off scale up to sufficiently large mass dimensions so that the SU(5)-breaking Higgs field develops a vacuum expectation value of the order of the unification scale along the F - and D -flat directions, with the help of the supersymmetry-breaking effect. The mass terms of the Higgs fields are also forbidden by the R symmetry, with which the doublet-triplet splitting problem is solved with the missing partner mechanism. The masses of right-handed neutrinos are generated by non-renormalizable operators, which then yield a light neutrino mass spectrum and mixing through the seesaw mechanism that are consistent with neutrino oscillation data. This model predicts one of the color-triplet Higgs multiplets to lie at an intermediate scale, and its mass is found to be constrained by proton decay experiments to be ≳ 5 × 10 11 GeV. If it is ≲ 10 12 GeV, future proton decay experiments at Hyper-Kamiokande can test our model in the p → π 0 μ + and p → K 0 μ + decay modes, in contrast to ordinary grand unified models where p → π 0 e + or p → K + ν ¯ is the dominant decay mode. This characteristic prediction for the proton decay branches enables us to distinguish our model from other scenarios.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP11(2020)140