Abstract
The use of the elements of the mass quadrupole tensor as generalized, nonredundant variables to describe nuclear collective motions is developed. The Hamiltonian for a group of $n$ identical particles in an oscillator well, which interact with each other by way of quadrupole two-body interactions, is rewritten in terms of the eigenvalues of the mass quadrupole tensor and angular momentum operators. The total angular momentum is separated into a part associated with rotations of the mass quadrupole tensor, and an intrinsic part. A semiclassical argument shows that the energies of states are approximately described by an expression in some respects indistinguishable from that of the empirical variable-moment-of-inertia model, which has been found adequate to represent the energies of the levels of a wide range of even nuclei.
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