Cranked Skyrme-Hartree-Fock-Bogoliubov approach for a mean-field description of nuclear rotations near the drip line

Abstract

To describe the yrast states in weakly bound nuclei, I directly solve the coordinate-space cranked Skyrme-Hartree-Fock-Bogoliubov equation on a three-dimensional lattice with the continuum states discretized in a box. After the numerical demonstration for the ground-state band in a medium-mass nucleus, I apply the newly-developed method to neutron-rich even-$N$ Mg isotopes. I find that the appearance of the significantly low $I^{\pi }=2^{+}$ state in ${}^{40}$Mg is mainly due to the suppression of pairing. The calculation predicts that the $2^{+}$ state in ${}^{42}$Mg appears as high in energy as in ${}^{34\text{-}38}$Mg whereas the triaxial deformation is enhanced in non-zero spin states. The present numerical framework offers a practical approach for investigating the near yrast states systematically and revealing structures unique in drip-line nuclei.

arXiv comment7 pages, 5 figures; accepted version

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Cited by in corpus (3)

• Triaxial-shape dynamics in the low-lying excited $0^{+}$ state: Role of the collective mass
• Super- and hyper-deformation in ${}^{60}$Zn, ${}^{62}$Zn, and ${}^{64}$Ge at high spins
• Enhanced moments of inertia for rotation in neutron-rich nuclei