Six-fermion weak interactions, in addition to the usual four-fermion weak interactions, may exist. Limits on the strength of such interactions deduced from low-energy decay phenomena are not sufficient to exclude observable effects of six-fermion couplings at high energies. In particular, the process ν+p→ν+μ+ē+p may be attributed either to six-fermion couplings, or to the existence of intermediary vector bosons.
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Ericson et al. (1964) studied this question.
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