Abstract
Following the recent recognition of the SU(3) and O(6) boson-fermion symmetries in the W and Pt regions, it is shown that a simple Hamiltonian can be constructed for the intervening transitional region. The proposed approach represents an extension of the consistent-$Q$ formalism, previously used in the description of even-even nuclei, and its predictions are discussed and compared with the low-lying structure in the odd-mass Os nuclei.
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