Determination of $\alpha _s(m_Z)$ by the non-perturbative decoupling method
Autor: | Dalla Brida, Mattia, Höllwieser, Roman, Knechtli, Francesco, Korzec, Tomasz, Nada, Alessandro, Ramos, Alberto, Sint, Stefan, Sommer, Rainer, ALPHA Collaboration |
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Jazyk: | angličtina |
Rok vydání: | 2022 |
Předmět: |
hep-lat
nonperturbative 12.38.Gc decoupling 3 [flavor] 12.38.Aw High Energy Physics - Lattice strong interaction: coupling constant quantum chromodynamics flavor: 3 ddc:530 heavy quark continuum limit Particle Physics - Phenomenology lattice field theory hep-ph Particle Physics - Lattice 11.10.Jj 11.10.Hi ALPHA High Energy Physics - Phenomenology 12.38.Bx statistics correlation gauge field theory renormalization group coupling constant [strong interaction] |
Zdroj: | The European physical journal / C 82(12), 1092 (2022). doi:10.1140/epjc/s10052-022-10998-3 |
DOI: | 10.1140/epjc/s10052-022-10998-3 |
Popis: | The European physical journal / C 82(12), 1092 (2022). doi:10.1140/epjc/s10052-022-10998-3 We present the details and first results of a new strategy for the determination of $\alpha _s(m_Z)$ (ALPHA Collaboration et al. in Phys. Lett. B 807:135571, 2020). By simultaneously decoupling 3 fictitious heavy quarks we establish a relation between the $\Lambda $-parameters of three-flavor QCD and pure gauge theory. Very precise recent results in the pure gauge theory (Dalla Brida and Ramos in Eur. Phys. J. C 79(8):720, 2019; Nada and Ramos in Eur Phys J C 81(1):1, 2021) can thus be leveraged to obtain the three-flavour $\Lambda $-parameter in units of a common decoupling scale. Connecting this scale to hadronic physics in 3-flavour QCD leads to our result in physical units, $\Lambda ^{(3)}_{\overline{\textrm{MS}}} = 336(12)\, {\textrm{MeV}}$, which translates to $\alpha _s(m_Z) = 0.11823(84)$. This is compatible with both the FLAG average (Aoki et al. in FLAG review 2021. arXiv:2111.09849 [hep-lat]) and the previous ALPHA result (ALPHA Collaboration et al., Phys. Rev. Lett. 119(10):102001, 2017), with a comparable, yet still statistics dominated, error. This constitutes a highly non-trivial check, as the decoupling strategy is conceptually very different from the 3-flavour QCD step-scaling method, and so are their systematic errors. These include the uncertainties of the combined decoupling and continuum limits, which we discuss in some detail. We also quantify the correlation between both results, due to some common elements, such as the scale determination in physical units and the definition of the energy scale where we apply decoupling. Published by Springer, Heidelberg |
Databáze: | OpenAIRE |
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