Abstract
The theory of the parity-nonconserving alpha-decays from levels in O16 is developed. Using the weak nucleon-nucleon interaction of Blin-Stoyle and Herczeg and known O16 wave-functions modified by short-range correlations via Bethe-Goldstone equation, the irregular alpha widths of the states 2−(8.88 MeV) and 3+(11.05 MeV) have been related to known regular widths. The influence by the hard-core of the strong interaction has been studied.
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