Abstract
Abstract Spin (6) boson-fermion dynamical symmetry is extended to odd-odd nuclei. An algorithm is constructed for a subsequent reduction appropriate for the boson-fermion group chain associated with odd protons and neutrons in j = 3 2 configurations and with SO(6) boson symmetry of the core. The corresponding energy formula for the odd-odd system is constructed and discussed. The possibility of generalization to extended supersymmetry encompassing even-even, odd-even and odd-odd nuclei is pointed out.
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