Triaxial-shape dynamics in the low-lying excited $0^{+}$ state: Role of the collective mass

Abstract

Background: Non-yrast states in neutron-rich nuclei are being investigated experimentally. These states reveal various aspects and details of the nuclear structure, such as the fluctuation around the axially symmetric shape. Purpose: The beyond-mean-field effects in neutron-rich nuclei with $N\simeq 28$ are investigated. We focus on the role of collective mass in triaxial-shape dynamics. Method: We employ the five-dimensional quadrupole collective Hamiltonian method with the potential obtained in a constrained Hartree--Fock--Bogoliubov approach with a Skyrme energy-density functional and the collective-mass functions obtained by the cranking approximation. The method includes triaxial deformations. Results: We find that ${}^{42}$Mg, ${}^{40}$Si, ${}^{44}$S, and ${}^{46}$S show $\gamma$-soft: A flat behavior in the potential energy surface along the triaxial deformation. Their low-lying spectra show a strong nucleus dependence, while those obtained with a collective mass assumed as constant are similar to each other. The energy ratio $E(0_2^{+})/E(2_1^{+})$ and the $B(E2)$ ratio $B(E2;0_2^{+}\to 2_1^{+})/B(E2;2_1^{+}\to 0_1^{+})$ show a unique property of the $0_2^{+}$ state, while the energy and $B(E2)$ ratios in neutron-deficient $\gamma$-soft nuclei with $N=78$ do not depend on nucleus so much. Conclusions: Low-lying spectra are determined by not only the potential energy but also the collective mass. We clarify the important role of the collective mass in low-energy dynamics in the neutron-rich $N\sim 28$ nuclei.

8 pages, 9 figures, accepted for publication in Phys. Rev. C

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Cited by in corpus (3)

• Shape transition and coexistence in Te isotopes studied with the quadrupole collective Hamiltonian based on a relativistic energy density functional
• Evolution of giant monopole resonance with triaxial deformation
• Determination of proton and neutron contributions to the $0_{g.s.}^{+}\to 2_1^{+}$ excitations in ${}^{42}$Si and ${}^{44}$S using inelastic proton scattering in inverse kinematics and intermediate energy Coulomb excitation