Abstract
We show that the linear energy weighted M1 sum rule is proportional to the summed E2 strength in the region of vibrational, transitional, and strongly deformed even-even nuclei using the proton-neutron interacting boson model. This general relation is compared with extensive data on M1 and E2 transition strength in rare-earth nuclei truncating the M1 sum rule to states below an excitation energy of 4 MeV. The above observation also implies a quadratic dependence on deformation (\ensuremath{\delta}) for the summed orbital M1 strength.
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.
