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 |
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Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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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. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP11(2020)140 |