Beyond-mean-field description of octupolarity in dysprosium isotopes with the Gogny-D1M energy density functional
arXiv:2308.04784 · doi:10.1103/PhysRevC.108.024301
Abstract
The emergence and stability of (static) octupole deformation effects in Dy isotopes from dripline to dripline () is analyzed in this paper using mean-field and beyond-mean-field techniques often used for this purpose. We find static octupole deformations at the Hartree-Fock-Bogoliubov (HFB) level with the Gogny D1M force for isotopes, while nuclei with exhibit reflection-symmetric ground states. It is shown that, given the softness found in the mean-field and parity-projected potential energy surfaces along the octupole direction, neither of these two levels of approximation is suficcient to extract conclusions about the (permanent and/or vibrational) nature of octupole dynamic in Dy isotopes. From the analysis of the collective wave functions as well as the excitation energies of the first negative-parity states and strengths, obtained within the framework of a two-dimensional symmetry-conserving generator coordinate method (2D-GCM), it is concluded that the increased octupole collectivity in Dy isotopes with and is a vibrational-like effect that is not directly related to permanent mean-field octupole deformation in the considered nuclei. A pronounced suppression of the strengths is predicted for isotopes with and . The comparison of results obtained with other parametrizations, show the robustness of the predicted trends with respect to the underlying Gogny energy density functional.
13 pages, 7 figures, published in Phys Rev C. arXiv admin note: text overlap with arXiv:2104.08063
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