Abstract

Abstract The ratio of the partial widths of some dimension-5 proton decay modes can be predicted without detailed knowledge of supersymmetric (SUSY) particle masses, and this allows us to experimentally test various SUSY grand unified theory (GUT) models without discovering SUSY particles. In this paper, we study the ratio of the partial widths of the $p\to K^0\mu^+$ and $p\to K^+\bar{\nu}_\mu$ decays in the minimal renormalizable SUSY $SO(10)$ GUT, under only a plausible assumption that the 1st- and 2nd-generation left-handed squarks are mass-degenerate. In the model, we expect that the Wilson coefficients of dimension-5 operators responsible for these modes are on the same order and that the ratio of $p\to K^0\mu^+$ and $p\to K^+\bar{\nu}_\mu$ partial widths is $O(0.1)$. Hence, we may be able to detect both $p\to K^0\mu^+$ and $p\to K^+\bar{\nu}_\mu$ decays at Hyper-Kamiokande, thereby gaining a hint for the minimal renormalizable SUSY $SO(10)$ GUT. Moreover, since this partial width ratio is quite suppressed in the minimal $SU(5)$ GUT, it allows us to distinguish the minimal renormalizable SUSY $SO(10)$ GUT from the minimal $SU(5)$ GUT. In the main body of the paper, we perform a fitting of the quark and lepton masses and flavor mixings with the Yukawa couplings of the minimal renormalizable $SO(10)$ GUT, and derive a concrete prediction for the partial width ratio based on the fitting results. We find that the partial width ratio generally varies in the range $0.05$–$0.6$, confirming the above expectation.

Highlights

  • The SO(10) grand unified theory (GUT) [1, 2] is a well-motivated scenario beyond the Standard Model (SM), since it unifies the SM gauge groups into an anomaly-free group, it unifies the SM matter fields and right-handed neutrino of each generation into one 16 representation, and it includes the seesaw mechanism [3, 4, 5, 6] for the tiny neutrino mass

  • We find that p → K0μ+ partial width is quite suppressed compared to p → K+νμ partial width because of the factor 0.002 coming from the ratio of yu and λ2yc, namely, the large hierarchy between the up and charm quark Yukawa couplings suppresses the partial width ratio

  • The ratio of the partial widths of some dimension-5 proton decay modes can be predicted without knowledge of SUSY particle masses, and serves as a probe for various SUSY GUT models even when SUSY particles are not discovered

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Summary

Introduction

The SO(10) grand unified theory (GUT) [1, 2] is a well-motivated scenario beyond the Standard Model (SM), since it unifies the SM gauge groups into an anomaly-free group, it unifies the SM matter fields and right-handed neutrino of each generation into one 16 representation, and it includes the seesaw mechanism [3, 4, 5, 6] for the tiny neutrino mass. SUSY particles have not been discovered at the LHC and no concrete prediction is available for the partial widths of dimension-5 proton decays, since they are inversely proportional to the soft SUSY breaking scale squared. In this situation, the ratio of the partial widths of different decay modes, which is independent of the soft SUSY breaking scale 2, allows us to test various SUSY GUT models including the minimal renormalizable SUSY SO(10) GUT

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