Abstract
A distorted-wave Born calculation is used to show that the strong initial- and final-state interactions in the nonmesonic hypernuclear decays, Λ+NN+N, are of major importance, greatly suppressing certain transitions, and suggest the dominance of one-pion exchange in the explanation of hypernuclear decay rates. Weak exchange of heavier mesons is also suppressed by the strong interactions both in Λ+NN+N badly breaking any SU(3) symmetry of the reactions—and in the parity-violating N+NN+N. It is shown that the decay rate of heavy hypernuclei provides a measure of the ΛN correlation function at short distances in nuclear matter and should depend significantly on the existence of a hard core in the ΛN strong interaction.

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