  Spectroscopic properties of odd-mass nuclei are studied within the framework
of the interacting boson-fermion model (IBFM) with parameters based on the
Hartree-Fock-Bogoliubov (HFB) approximation. The parametrization D1M of the
Gogny energy density functional (EDF) has been used at the mean-field level to
obtain the deformation energy surfaces for the considered nuclei in terms of
the quadrupole deformations ($\beta,\gamma$). In addition to the energy
surfaces, both single particle energies and occupation probabilities have been
used as a microscopic input for building the IBFM Hamiltonian. Only three
strength parameters for the particle-boson-core coupling are fitted to
experimental spectra. The IBFM Hamiltonian is then used to compute the energy
spectra and electromagnetic transition rates for selected odd-mass Eu and Sm
nuclei as well as for $^{195}$Pt and $^{195}$Au. A reasonable agreement with
the available experimental data is obtained for the considered odd-mass nuclei.
