Abstract
The nonleptonic interaction and its consequences in a particular renormalizable theory of weak interactions mediated by spin-zero bosons are discussed. It is pointed out that the $\ensuremath{\Delta}S=0$ weak nuclear processes and the deviations from octet dominance in the $\ensuremath{\Delta}S=1$ nonleptonic decays $B\ensuremath{\rightarrow}{B}^{\ensuremath{'}}+\ensuremath{\pi}$ can serve to distinguish it from the usual $V\ensuremath{-}A$ theory.
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