Abstract

In this Letter, we provide a determination of the coupling constant in three-flavor quantum chromodynamics (QCD), α_{s}^{MS[over ¯]}(μ), for MS[over ¯] renormalization scales μ∈(1,2) GeV. The computation uses gauge field configuration ensembles with O(a)-improved Wilson-clover fermions generated by the Coordinated Lattice Simulations (CLS) consortium. Our approach is based on current-current correlation functions and has never been applied before in this context. We convert the results perturbatively to the QCD Λ parameter and obtain Λ_{MS[over ¯]}^{N_{f}=3}=342±17 MeV, which agrees with the world average published by the Particle Data Group and has competing precision. The latter was made possible by a unique combination of state-of-the-art CLS ensembles with very fine lattice spacings, further reduction of discretization effects from a dedicated numerical stochastic perturbation theory simulation, combining data from vector and axial-vector channels, and matching to high-order perturbation theory.

Highlights

  • The Particle Data Group and has competing precision

  • In this Letter, we provide a determination of the coupling constant in three-flavor quantum chromodynamics (QCD), αMs SðμÞ, for MS renormalization scales μ ∈ ð1; 2Þ GeV

  • We convert the results perturbatively to the QCD Λ parameter and obtain ΛNf1⁄43 1⁄4 342 Æ 17 MeV, which agrees with the world average published by the Particle Data Group and has competing precision

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Summary

Introduction

The Particle Data Group and has competing precision. The latter was made possible by a unique combination of state-of-the-art CLS ensembles with very fine lattice spacings, further reduction of discretization effects from a dedicated numerical stochastic perturbation theory simulation, combining data from vector and axial-vector channels, and matching to high-order perturbation theory. Running Coupling Constant from Position-Space Current-Current Correlation Functions in Three-Flavor Lattice QCD The one-loop-corrected correlators are very close to the four-loop continuum perturbative curve [27], indicating that the remaining discretization effects are small at this lattice spacing.

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