Abstract

An explicit numerical estimate of the many-body contributions (specifically, three-body and four-body contributions) to the effective Hamiltonian, introduced by the truncation of the shell-modell valence space, is presented. On the average, they are found to be rather small. In particular, in the case of four nucleons, it turns out that three-body and four-body contributions have generally opposite signs and therefore cancel each other. Only rarely they add and become significant. This holds for realistic and phenomenological interactions and also for empirical set of interaction matrix elements, and therefore lends support to the conventional practice of using effective two-body interactions in nuclear shell-model calculations. This is confirmed, in the case of six and eight nucleons, by the results obtained in the one-broken-pair approximation.

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 call

Disclaimer: 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.