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Renormalon Ambiguities in NRQCD Operator Matrix Elements
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ANL-HEP-PR-98-29
OHSTPY-HEP-T-98-008
June, 1999
Renormalon Ambiguities in NRQCD Operator Matrix Elements
Geoffrey T. Bodwin
High Energy Physics Division, Argonne National Laboratory, Argonne, IL 60439
Yu-Qi Chen
Physics Department, Ohio State University, Columbus, Ohio 43210
Abstract
We analyze the renormalon ambiguities that appear in factorization formu-
las in QCD. Our analysis contains a simple argument that the ambiguities
in the short-distance coefficients and operator matrix elements are artifacts
of dimensional-regularization factorization schemes and are absent in cutoff
schemes. We also present a method for computing the renormalon ambiguities
in operator matrix elements and apply it to a computation of the ambigui-
ties in the matrix elements that appear in the NRQCD factorization formulas
for the annihilation decays of S-wave quarkonia. Our results, combined with
those of Braaten and Chen for the short-distance coefficients [1], provide an
explicit demonstration that the ambiguities cancel in the physical decay rates.
In addition, we analyze the renormalon ambiguities in the Gremm-Kapustin
relation and in various definitions of the heavy-quark mass.
Typeset using REVTEX
1
I. INTRODUCTION
In Quantum Chromodynamics (QCD), it is often useful to describe physical processes
involving more than one distance scale by making use of a factorization formalism. In such
a formalism, a physical observable is written as a sum of products of short-distance coeffi-
cients with long-distance operator matrix elements. The short-distance coefficients may be
calculated as a perturbative series in the strong coupling constant αs, evaluated at the short-
distance scale. The operator matrix elements contain all of the sensitivity of the physical
observable to low-momentum (infrared) processes. Because of this infrared (IR) sensitivity,
the operator matrix elements are generally not amenable to a perturbative calc
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