Shell model based deformation analysis of light Cadmium isotopes
arXiv:1706.02544 · doi:10.1103/PhysRevC.96.014302
Abstract
Large-scale shell-model calculations for the even-even Cadmium isotopes 98 Cd - 108 Cd have been performed with the ANTOINE code in the π(2p 1/2 ; 1g 9/2 ) ν(2d 5/2 ; 3s 1/2 ; 2d 3/2 ; 1g 7/2 ; 1h 11/2 ) model space without further truncation. Known experimental energy levels and B(E2) values could be well reproduced. Taking these calculations as a starting ground we analyze the deformation parameters predicted for the Cd isotopes as a function of neutron number N and spin J using the methods of model independent invariants introduced by K. Kumar and D. Cline.
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Cited by in corpus (16)
- The Neutron-Rich Edge of the Nuclear Landscape. Experiment and Theory
- Constraining the quadrupole deformation of atomic nuclei with relativistic nuclear collisions
- The quest of shape coexistence in Zr isotopes
- Structure of even-even Cadmium isotopes from the beyond-mean-field interacting boson model
- Quadrupole dominance in the light Sn and in the Cd isotopes
- Statistical theory of deformation distributions in nuclear spectra
- Evolution of nuclear structure in and around Z=50 closed shell: Generalized Seniority in Cd, Sn and Te isotopes
- Spectroscopy and excited-state ~factors in weakly collective Cd: confronting collective and microscopic models
- Convergence of electric quadrupole rotational invariants from the nuclear shell model
- Nuclear deformation in the laboratory frame
- Collective-model description of shape coexistence and intruder states in cadmium isotopes based on a relativistic energy density functional
- E2 Rotational Invariants of and states for Cd: the Emergence of Collective Rotation
- Mean-field calculations of charge radii in ground and isomeric states of Cd isotopes
- Systematic shell-model study of Cd isotopes and isomeric states
- Quadrupole dominance in light Cd and Sn isotopes
- Nuclear deformation in the configuration-interaction shell model