We theoretically study the conductance spectra of metal/ferromagnetic material junctions. There is a change in slope of the conductance spectrum at the energy equivalent to the bottom of the minority band. This feature is most prominent in one-dimensional (1D) systems. For any dimensionality, the interfacial spin-flip scattering can suppress or enhance the conductance, depending on the quality of the junction. When the non-spin-flip or normal scattering is weak, the spin-flip scattering always suppresses the conductance. On the contrary, in the limit where the normal scattering is strong, the conductance can be enhanced to a maximum value, when the strength of the spin-flip and the normal scattering are equal. As for the spin polarization of the conductance, it is largest in the limit where the normal scattering is strong and depends on junction dimensionality. In this limit, the 1D spin polarization is independent of the spin-flip scattering strength, whereas the 2D and 3D spin polarizations can be increased with the strength of the spin-flip scattering up to a maximum value, at which both types of scattering are about the same strength.