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| 001 | 599764 | ||
| 005 | 20241211214813.0 | ||
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| 024 | 7 | _ | |a arXiv:2401.00216 |2 arXiv |
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| 088 | _ | _ | |a DESY-24-001 |2 DESY |
| 088 | _ | _ | |a arXiv:2401.00216 |2 arXiv |
| 100 | 1 | _ | |a Dalla Brida, Mattia |0 P:(DE-H253)PIP1018317 |b 0 |
| 245 | _ | _ | |a Heavy Wilson quarks and O(a) improvement: nonperturbative results for b$_{g}$ |
| 260 | _ | _ | |c 2024 |
| 336 | 7 | _ | |a Preprint |b preprint |m preprint |0 PUB:(DE-HGF)25 |s 1733908730_2802764 |2 PUB:(DE-HGF) |
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| 500 | _ | _ | |a J. High Energ. Phys. 2024, 188 (2024). 26 pages, 5 figures. Included additional references and fixed some typos. Matches published version The work is supported by the German Research Foundation (DFG) research unit FOR5269 “Futuremethods for studying confined gluons in QCD”. |
| 520 | _ | _ | |a 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. |
| 536 | _ | _ | |a 611 - Fundamental Particles and Forces (POF4-611) |0 G:(DE-HGF)POF4-611 |c POF4-611 |f POF IV |x 0 |
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| 588 | _ | _ | |a Dataset connected to DataCite |
| 650 | _ | 7 | |a quark: Wilson |2 INSPIRE |
| 650 | _ | 7 | |a dimension: 5 |2 INSPIRE |
| 650 | _ | 7 | |a flow: gradient |2 INSPIRE |
| 650 | _ | 7 | |a mass: operator |2 INSPIRE |
| 650 | _ | 7 | |a quantum chromodynamics |2 INSPIRE |
| 650 | _ | 7 | |a lattice field theory: action |2 INSPIRE |
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| 650 | _ | 7 | |a symmetry: chiral |2 INSPIRE |
| 650 | _ | 7 | |a decoupling |2 INSPIRE |
| 650 | _ | 7 | |a nonperturbative |2 INSPIRE |
| 650 | _ | 7 | |a mass dependence |2 INSPIRE |
| 650 | _ | 7 | |a rescaling |2 INSPIRE |
| 650 | _ | 7 | |a perturbation theory |2 INSPIRE |
| 650 | _ | 7 | |a beta function |2 INSPIRE |
| 650 | _ | 7 | |a coupling constant |2 INSPIRE |
| 650 | _ | 7 | |a Algorithms and Theoretical Developments |2 autogen |
| 650 | _ | 7 | |a Lattice QCD |2 autogen |
| 650 | _ | 7 | |a Non-Perturbative Renormalization |2 autogen |
| 650 | _ | 7 | |a Standard Model Parameters |2 autogen |
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| 700 | 1 | _ | |a Höllwieser, Roman |0 P:(DE-H253)PIP1086528 |b 1 |
| 700 | 1 | _ | |a Knechtli, Francesco |0 P:(DE-H253)PIP1093357 |b 2 |
| 700 | 1 | _ | |a Korzec, Tomasz |0 P:(DE-H253)PIP1019728 |b 3 |
| 700 | 1 | _ | |a Sint, Stefan |0 P:(DE-H253)PIP1019836 |b 4 |
| 700 | 1 | _ | |a Sommer, Rainer |0 P:(DE-H253)PIP1003629 |b 5 |u desy |
| 700 | 1 | _ | |a ALPHA Collaboration |0 P:(DE-HGF)0 |b 6 |e Collaboration Author |
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