We present a determination of the strong coupling constant αs(mZ) based on the NNPDF3.1 determination of parton distributions, which for the first time includes constraints from jet production, top-quark pair differential distributions, and the ZpTdistributions using exact NNLO theory. Our result is based on a novel extension of the NNPDF methodology – the correlated replica method – which allows for a simultaneous determination of αsand the PDFs with all correlations between them fully taken into account. We study in detail all relevant sources of experimental, methodological and theoretical uncertainty. At NNLO we find αs(mZ) = 0.1185 ± 0. 0005(exp)± 0. 0001(meth), showing that methodological uncertainties are negligible. We conservatively estimate the theoretical uncertainty due to missing higher order QCD corrections (N3LO and beyond) from half the shift between the NLO and NNLO αsvalues, finding Δαsth=0.0011.
Precision determination of the strong coupling constant within a global PDF analysis: NNPDF Collaboration / R.D. Ball, S. Carrazza, L.D. Debbio, S. Forte, Z. Kassabov, J. Rojo, E. Slade, M. Ubiali. - In: THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS. - ISSN 1434-6044. - 78:5(2018 May 24). [10.1140/epjc/s10052-018-5897-7]
Precision determination of the strong coupling constant within a global PDF analysis: NNPDF Collaboration
S. Carrazza;S. Forte
;Z. Kassabov;
2018
Abstract
We present a determination of the strong coupling constant αs(mZ) based on the NNPDF3.1 determination of parton distributions, which for the first time includes constraints from jet production, top-quark pair differential distributions, and the ZpTdistributions using exact NNLO theory. Our result is based on a novel extension of the NNPDF methodology – the correlated replica method – which allows for a simultaneous determination of αsand the PDFs with all correlations between them fully taken into account. We study in detail all relevant sources of experimental, methodological and theoretical uncertainty. At NNLO we find αs(mZ) = 0.1185 ± 0. 0005(exp)± 0. 0001(meth), showing that methodological uncertainties are negligible. We conservatively estimate the theoretical uncertainty due to missing higher order QCD corrections (N3LO and beyond) from half the shift between the NLO and NNLO αsvalues, finding Δαsth=0.0011.File | Dimensione | Formato | |
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Ball2018_Article_PrecisionDeterminationOfTheStr.pdf
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