Abstract
It is proposed that nuclei (away from closed shells and from regions of large deformation) be described as a boson gas. Exploiting the underlying O(5) symmetry analytic expressions for the eigenvalues of the boson Hamiltonian and for the transition matrix elements are obtained. The computed energy levels are in surprisingly good agreement with those recently observed in the ( α, xn γ) and (heavy ions, xn γ)
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