Abstract

We show that, in the simplest model where strong interaction effects are included in the baryon vertices and propagators only, the peratization of the nuclear vector $\ensuremath{\beta}$-decay coupling strength is no longer equal to the corresponding peratization of the $\ensuremath{\mu}$-decay coupling strength. This might suggest a vastly different role of strong interactions in the weak interaction (peratization) theory of Feinberg and Pais, in order to conform with the observed equality of nuclear vector $\ensuremath{\beta}$-decay and $\ensuremath{\mu}$-decay strengths.

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