Abstract
A recently proposed microscopic version of the Bohr-Mottelson collective model, defined by the following dynamical symmetry chain \(Sp(12,R) \supset SU(1,1) \otimes SO(6) \supset U(1) \otimes SU_{pn}(3) \otimes SO(2) \supset SO(3)\) of the proton-neutron symplectic model (PNSM), is applied to the microscopic shell-model description of the low-lying collective excitations in two transitional nuclei, namely \(^{104}\)Ru and \(^{192}\)Os. Detailed shell-model results are presented for the excitation levels of the ground and \(\gamma \) bands in \(^{104}\)Ru, and the ground, \(\gamma \), and \(\beta \) bands in \(^{192}\)Os, as well as for the probability distributions and the quadrupole collectivity. A good overall description is obtained for the excitation energies of the bands under consideration for the two transitional nuclei without using an adjustable kinetic-energy term, as well as for the ground state intraband B(E2) quadrupole collectivity and the known interband B(E2) transition probabilities between the low-lying collective states without the use of an effective charge.
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Ganev, H.G. Microscopic shell-model description of transitional nuclei. Eur. Phys. J. A 58, 182 (2022). https://doi.org/10.1140/epja/s10050-022-00834-3
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DOI: https://doi.org/10.1140/epja/s10050-022-00834-3