For any purely fermionic system on a lattice in arbitrary space dimens
ion we prove that there is a different but well-defined system on the
same lattice, consisting of both bona fide fermions and bosons with an
interaction depending on a parameter lambda, which characterizes a sa
me-site repulsion between particles. The energy spectrum and the scatt
ering matrix of the former are identical to those in the finite energy
sector of the latter, in the limit lambda --> infinity (i.e., hard-co
re repulsion). This general theorem is applied to a resonance-boson mo
del in a lattice fermion system, whose solution may have relevance to
high-T(c) superconductivity.