Abstract

We discuss the impact of horizontal gauge symmetries on nucleon decay and demonstrate that the ongoing proton-decay experiments may be used to distinguish between different horizontal gauge theories. Under very general assumptions, it is shown that although a minimal $\mathrm{U}{(1)}_{H}$ horizontal symmetry allows dimension-six operators and leads to the decay of the nucleon into leptons of the first generation only, an $\mathrm{SU}{(3)}_{H}$ horizontal symmetry forbids any baryon-nonconserving operator of dimension less than nine.

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