Heavy Wilson Quarks and O($a$) Improvement: Nonperturbative Results for $b_{\mathrm{g}}$

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, ${\tilde{g}}_0^2=g_0^2(1+b_{\mathrm{g}}a{m}_{\mathrm{q}})$, and the determination of $b_{\mathrm{g}}(g_0^2)$, 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 $\beta$-values and the line of constant physics are motivated by the ALPHA collaboration's decoupling strategy to determine ${\alpha }_s(m_Z)$. However, the improvement conditions and some insight into systematic effects may prove useful in other contexts, too.

26 pages, 5 figures. Included additional references and fixed some typos. Matches published version

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