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Algebraic formulation of collective models III. The symplectic shell model of collective motion

Journal Article · · Ann. Phys. (N.Y.); (United States)
The symplectic model is a microscopic theory which provides a practical technique for identifying the shell configurations necessary for the description of quadrupole and monopole vibrations as well as collective rotations of the nucleus. The model is based on the non-compact symplectic algebra sp(3, R) and is a natural generalization of Elliott's su(3) model to include many major oscillator shells in addition to core excitations. It is also simultaneously the shell model adaptation of the collective rotational (R/sup 5/)so(3), the Bohr-Mottelson cm(3)=R/sup 6/)sl(3) and the mass quadrupole collective MQC=R/sup 6/)gl(3) models. In contrast to the su(3) algebra, the sp(3, R) algebra makes no 0h..omega.. approximations and treats all observables in the algebra exactly, thereby achieving a microscopic theory of large amplitude collective motion. The observables in the algebra include the quadrupole and monopole moments, the kinetic energy, the harmonic oscillator Hamiltonian and the angular and vibrational momenta. Numerical results are reported for /sup 20/Ne using an 8 h..omega.. truncation and a phenomenological potential V(..beta..,..gamma..). Satisfactory agreement with experiment is obtained for the absolute B(E2) rates without resorting to an effective charge.
Research Organization:
Department of Physics, Tulane University, New Orleans, Louisiana 70118
OSTI ID:
5206504
Journal Information:
Ann. Phys. (N.Y.); (United States), Journal Name: Ann. Phys. (N.Y.); (United States) Journal Issue: 2 Vol. 126:2; ISSN APNYA
Country of Publication:
United States
Language:
English