The short-distance expansion of the heavy-light currents qˉγμQ and qˉγμγ5Q is constructed to order 1/mQ, and to
next-to-leading order in renormalization-group improved perturbation theory. It
is shown that the 10×10 anomalous dimension matrix, which describes the
scale dependence of the dimension-four effective current operators in the heavy
quark effective theory, is to a large extent determined by the equations of
motion, heavy quark symmetry, and reparameterization invariance. The
next-to-leading order expressions for the Wilson coefficients at order 1/mQ
depend on only five unknown two-loop anomalous dimensions, among them that of
the chromo-magnetic operator.Comment: 22 pages LaTeX, SLAC-PUB-634