Abstract
Conscrvation of parity in ccrtain of the strong interactions is discussed. The framcwork for thc discussion was the doublet approximation, (DA), a rather high group of symmetrics invoked for two classes of Yukawatypc mcson- baryon interactions, the pion-baryon intcractions, and the K meson-baryon interactions. There appears to bc room, within the limits of thc very scant knowledge of Yukawa type interactions, for possible small cffects of parity nonconservation. (A.C.)
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