Starting from the Schr\"odinger functional, we give a non-perturbative
definition of the running coupling constant in QCD. The spatial boundary
conditions for the quark fields are chosen such that the massless Dirac
operator in the classical background field has a large smallest eigenvalue. At
one-loop order of perturbation theory, we determine the matching coefficient to
the \MSbar-scheme and discuss the quark mass effects in the β-function.
To this order, we also compute the Symanzik improvement coefficient necessary
to remove the \Oa lattice artefacts originating from the boundaries. For
reasonable lattice resolutions and the standard Wilson action, lattice
artefacts are found to be only weakly dependent on the lattice spacing a,
while they vanish quickly with the improved action of Sheikholeslami and
Wohlert.Comment: 29 pages; uuencoded, complete postscript fil