Abstract

The microscopic energy density method is applied to the study of nuclei with N ⩾ 50 and Z = 32−40. The experimental Subshell effect at N = 56, which is not found in many previous works about this region, is well reproduced by the present self-consistent calculation. The existence of strongly deformed prolate isotopes of Zr and Sr for N ⩾ 60 is also explained. A wide region of oblate shapes is predicted for N ⩾ 60 and Z ⩽ 36. The results also support the interpretation of low-energy isomers in the shape transition region as shape isomers.

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