Abstract
The theory of the parity-nonconserving alpha decays from the ${2}^{\ensuremath{-}}$ (8.88 MeV), ${0}^{\ensuremath{-}}$ (10.937 MeV), and ${3}^{+}$ (11.05 MeV) ${\mathrm{O}}^{16}$ levels is developed. Using the weak nucleon-nucleon interaction of Blin-Stoyle and Herczeg and known ${\mathrm{O}}^{16}$ wave functions modified by short-range correlations via the Bethe-Goldstone equation, the irregular alpha widths have been related to known regular widths. The influence by the hard core of the strong interaction has been studied.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
