Renormalization of HQET at Three Loops
Abstract
Three-loop propagator diagrams in HQET can be reduced, using integration by parts, to 8 basis integrals: 5 trivial ones, two expressible via 3F2, and one only known up to ε0. Calculation of the heavy-quark propagator in HQET is considerably simplified by the non-abelian exponentiation theorem.
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