A class of models is devised which, while respecting electron-muon universality in the Lagrangian, results naturally in a small value of mₑm_μ, and which does not involve the introduction of exotic new gauge interactions. [The gauge group is SU(2) ×{} U(1) and the model is a relatively simple extension of the Weinberg-Salam model.] This is achieved by repeated applications of discrete symmetry. The model requires the existence of heavy leptons, and the precise value of mₑm_μ depends upon the masses of these leptons.
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Barr et al. (1977) studied this question.
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