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We propose a theoretical description of superdeformed bands based on the projected shell model. The shell model basis is constructed at the superdeformed minimum and projected onto states of good angular momentum, and a two-body Hamiltonian is then diagonalized in this basis. We take the superdeformed band in Ce 132 as an example. Good agreement with the measured gamma-ray energies allows us to suggest spin values for these superdeformed states. Finally, we propose an explanation for the recently observed Δ I =4 bifurcation disappearance at a rotational frequency of ħω≃0.65 in this nucleus.
Physical Review C – American Physical Society (APS)
Published: Dec 1, 1995
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