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Journal Article | PUBDB-2024-06646 |
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2024
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Please use a persistent id in citations: doi:10.1007/JHEP01(2024)188 doi:10.3204/PUBDB-2024-06646
Report No.: DESY-24-001; arXiv:2401.00216
Abstract: With Wilson quarks, on-shell O(a) improvement of the lattice QCD action is achieved by including the Sheikholeslami-Wohlert term and two further operators of mass dimension 5, which amount to a mass-dependent rescaling of the bare parameters. We here focus on the rescaled bare coupling, $ {\tilde{g}}_0^2={g}_0^2\left(1+{b}_{\textrm{g}}a{m}_{\textrm{q}}\right) $, and the determination of $ {b}_{\textrm{g}}\left({g}_0^2\right) $ which is currently only known to 1-loop order of perturbation theory. We derive suitable improvement conditions in the chiral limit and in a finite space-time volume and evaluate these for different gluonic observables, both with and without the gradient flow. The choice of β-values and the line of constant physics are motivated by the ALPHA collaboration’s decoupling strategy to determine α$_{s}$(m$_{Z}$) [1]. However, the improvement conditions and some insight into systematic effects may prove useful in other contexts, too.
Keyword(s): quark: Wilson ; dimension: 5 ; flow: gradient ; mass: operator ; quantum chromodynamics ; lattice field theory: action ; space-time ; symmetry: chiral ; decoupling ; nonperturbative ; mass dependence ; rescaling ; perturbation theory ; beta function ; coupling constant ; Algorithms and Theoretical Developments ; Lattice QCD ; Non-Perturbative Renormalization ; Standard Model Parameters
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Preprint
Heavy Wilson quarks and O(a) improvement: nonperturbative results for b$_{g}$
[10.3204/PUBDB-2023-07490]
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