Within an effective field theory framework we study heavy-quark--antiquark
systems with a typical distance between the heavy quark and the antiquark
smaller than $1/\Lambda_{\rm QCD}$. A suitable definition of the potential is
given within this framework, while non-potential (retardation) effects are
taken into account in a systematic way. We explore different physical systems.
Model-independent results on the short distance behavior of the energies of the
gluonic excitations between static quarks are obtained. Finally, we show how
infrared renormalons affecting the static potential get cancelled in the
effective theory.Comment: 39 pages, LaTeX, 12 figures. Journal version. Some explanatory
remarks and references adde
This article reviews recent theoretical developments in heavy-quarkonium physics from the point of view of effective-field theories of QCD. We discuss nonrelativistic QCD and concentrate on potential nonrelativistic QCD. The main goal will be to derive Schrödinger equations based on QCD that govern heavy-quarkonium physics in the weak-and strong-coupling regimes. Finally, the review discusses a selected set of applications, which include spectroscopy, inclusive decays, and electromagnetic threshold production.
CONTENTS
We propose an effective field theory for heavy quark-antiquark bound states once the soft gluons have been integrated out. We also give new results for the matching between QCD (QED) and NRQCD (NRQED).
Within an effective field theory framework, we obtain an expression for the next-to-leading term in the 1/m expansion of the singlet QQ QCD potential in terms of Wilson loops, which holds beyond perturbation theory. The ambiguities in the definition of the QCD potential beyond leading order in 1/m are discussed and a specific expression for the 1/m potential is given. We explicitly evaluate this expression at one loop and compare the outcome with the existing perturbative results. On general grounds we show that for quenched QED and fully Abelian-like models this expression exactly vanishes.
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