Abstract
The potential energy of a nucleus is calculated as a function of its shape using the method of Strutinski. The nuclear shapes are composed of two spheroids (centres z = ± z 1 ; z-axis = symmetry axis) smoothly joined by a central hyperboloid (neck) or a central spheroid (belly). The corresponding shell-model potential is constructed from two harmonic oscillators centered around z = ± z 1 and smoothly joined by a third oscillator centered around z = 0. A generalized form of Nilssons's spin-orbit and l 2 term is used.
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