In a series of publications (Nucl. Phys. B384 (1994) 168; B389 (1994)
247), Luscher et al. have demonstrated the usefulness of the Schroding
er functional in pure SU(2) and SU(3) gauge theory. In this paper, it
is shown how their formalism can be extended to include fermions. In t
he framework of Wilson's lattice QCD, we define the Schrodinger functi
onal by making use of the transfer matrix formalism. Boundary conditio
ns for the fermions arise naturally. We then take the naive continuum
limit of the action and show that no lattice peculiarities are left ov
er. The corresponding free Dirac operator has a unique self-adjoint ex
tension with purely discrete spectrum and no zero-modes.