  We demonstrate an exact local transformation which maps a purely Fermionic
manybody system to a system of spinfull Bosons and spinless Fermions,
demonstrating a possible path to a non-Fermi liquid state. We apply this to the
half-filled Hubbard model and show how the transformation maps the ordinary
spin half Fermionic degrees of freedom exactly and without introducing Hilbert
space constraints to a charge-like ``quasicharge'' fermion and a spin-like
``quasispin'' Boson while preserving all the symmetries of the model. We
present approximate solutions with localized charge which emerge naturally from
the Hubbard model in this form. Our results strongly suggest that charge tends
to remain localized for large values of the Hubbard U.
