A unified view of the first-excited and states of Cd, Sn and Te isotopes
arXiv:2007.04105 · doi:10.1140/epjst/e2020-000097-3
Abstract
Symmetries are known to play an important role in the low lying level structure of Sn isotopes, mostly in terms of the seniority and generalized seniority schemes. In this paper, we revisit the multi-j generalized seniority approach for the first excited and states in the Cd (), Sn () and Te () isotopes, where the Cd and Te isotopes represent two-proton hole and two-proton particle nuclei, thus involving both kind of particles (protons and neutrons) in contrast to Sn isotopes. Interestingly, the approach based on neutron valence space alone is able to explain the B(E2) and B(E3) trends respectively for the and states in all the three Cd, Sn and Te isotopes. The new results on the inverted parabolic behavior of B(E3) values in Cd and Te isotopes are understood in a manner identical to that of Sn isotopes by using the generalized seniority scheme. No shell quenching is supported by these calculations; hence, the neutron magic numbers, and , remain robust in these isotopic chains. It is quite surprising that the generalized seniority continues to be reasonably successful away from the semi-magic region, thus providing a unifying view of the and states.
arXiv commentAccepted in European Physical Journal Special Topics on role of symmetries in nuclear physics. arXiv admin note: substantial text overlap with arXiv:1908.05028
References in corpus (7)
- Tables of E2 Transition Probabilities from the first States in Even-Even Nuclei
- Odd tensor electric transitions in high-spin Sn-isomers and generalized seniority
- Asymmetric behavior of the B values in Sn and Generalized Seniority
- Evolution of nuclear structure in and around Z=50 closed shell: Generalized Seniority in Cd, Sn and Te isotopes
- Generalized Seniority Schmidt Model and the g-factors in Semi-magic Nuclei
- seniority changing transitions in yrast states and B(E3) systematics of Sn isotopes
- Multiple multi-orbit pairing algebras in shell model and interacting boson models