Abstract

The lifetimes of particles and their antiparticles are discussed under different assumptions. It is shown that if P · C is conserved these lifetimes are rigorously equal, but in practice their equality is no evidence for P · C conservation even when strong final state interactions do exist. The P · C conservation is best tested by the K 0 modes of decay. A description of Kμν interaction by means of a direct coupling only (Yukawa type) is shown to be impossible.

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