Abstract
The relation between the phenomenological Hamiltonian as used in dynamical boson-fermion symmetries and the semimicroscopic Hamiltonian of the interacting boson-fermion approximation, both used in the description of odd-mass nuclei, is studied in detail. Predictions are obtained for the parameters of the boson fermion symmetry Hamiltonian. From the microscopic picture behind the interacting boson-fermion approximation model, predictions are also obtained for the regions in the table of isotopes where the boson-fermion symmetries can be expected to occur. In addition we derive the structure of an additional exchange force, which results from the interaction between like particles.
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