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The short-distance expansion of the heavy-light currents $\bar q,\gamma^\mu Q\bar q,\gamma^\mu\gamma_5,Q1/m_Q$, and to next-to-leading order in renormalization-group improved perturbation theory. It is shown that the 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 depend on only five unknown two-loop anomalous dimensions, among them that of the chromo-magnetic operator.

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