Color-octet nonrelativistic QCD matrix elements for heavy quarkonium decays in the refined Gribov-Zwanziger theory
arXiv:2312.10601 · doi:10.1103/PhysRevD.109.054001
Abstract
We determine color-octet nonrelativistic QCD matrix elements for quarkonium decays from moments of the two-point correlation function of the QCD field-strength tensor computed in the refined Gribov-Zwanziger theory. We find that a tree-level calculation in the refined Gribov-Zwanziger theory can give a suitable description of the QCD field-strength correlation function at both short and long distances, which leads to moments that are infrared finite and can be properly renormalized. By using the color-octet matrix elements we obtain, we quantitatively improve the nonrelativistic effective field theory description of quarkonium decay rates, especially for the and states, where or .
21 pages, 3 figures, minor revisions, version published in Phys. Rev. D
References in corpus (12)
- A refinement of the Gribov-Zwanziger approach in the Landau gauge: infrared propagators in harmony with the lattice results
- New features of the gluon and ghost propagator in the infrared region from the Gribov-Zwanziger approach
- Indirect lattice evidence for the Refined Gribov-Zwanziger formalism and the gluon condensate in the Landau gauge
- Scaling behavior and positivity violation of the gluon propagator in full QCD
- The Landau gauge gluon and ghost propagator in the refined Gribov-Zwanziger framework in 3 dimensions
- Three-Loop Chromomagnetic Interaction in HQET
- The effects of Gribov copies in 2D gauge theories
- Next-to-next-to-leading-order QCD corrections to hadronic width of pseudoscalar quarkonium
- Inclusive Charm Production in chi_b Decays
- Precise determination of decay rates for , and from lattice QCD
- -wave quarkonium wavefunctions at the origin in the scheme
- Operator product expansion for the non-local gluon condensate