Table of Contents
Fetching ...

QCD Radiative Correction to the Hadronic Annihilation Rate of $1^{+-}$ Heavy Quarkonium

Han-Wen Huang, Kuang-Ta Chao

TL;DR

Hadronic annihilation rate of 1 heavy quarkonium is given to next-to-leading order in αs using a recently developed factorization formalism which base on NRQCD.

Abstract

Hadronic annihilation rate of $1^{+-}$ heavy quarkonium is given to next-to-leading order in $α_s$ and leading order in $v^2$ using a recently developed factorization formalism which is based on NRQCD. The result includes both the annihilation of P-wave color-singlet $Q\bar{Q}$ component, and the annihilation of S-wave color-octet $Q\bar{Q}$ component of the quarkonium. The notorious infrared divergences due to soft gluons, i.e., the Logarithms associated with the binding energy, encountered in previous perturbative calculations of $1^{+-}$ quarkonium decays are found to be explicitly cancelled, and a finite result for the decay width to order $α_s^3$ is then obtained.

QCD Radiative Correction to the Hadronic Annihilation Rate of $1^{+-}$ Heavy Quarkonium

TL;DR

Hadronic annihilation rate of 1 heavy quarkonium is given to next-to-leading order in αs using a recently developed factorization formalism which base on NRQCD.

Abstract

Hadronic annihilation rate of heavy quarkonium is given to next-to-leading order in and leading order in using a recently developed factorization formalism which is based on NRQCD. The result includes both the annihilation of P-wave color-singlet component, and the annihilation of S-wave color-octet component of the quarkonium. The notorious infrared divergences due to soft gluons, i.e., the Logarithms associated with the binding energy, encountered in previous perturbative calculations of quarkonium decays are found to be explicitly cancelled, and a finite result for the decay width to order is then obtained.

Paper Structure

This paper contains 45 equations, 1 table.