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Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data

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Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data. / JADE Collaboration ; Bowdery, Christopher; Foster, Frank et al.
In: European Physical Journal C: Particles and Fields, Vol. 64, No. 3, 12.2009, p. 351-360.

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JADE Collaboration, Bowdery C, Foster F, Hughes G. Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data. European Physical Journal C: Particles and Fields. 2009 Dec;64(3):351-360. doi: 10.1140/epjc/s10052-009-1149-1

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JADE Collaboration ; Bowdery, Christopher ; Foster, Frank et al. / Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data. In: European Physical Journal C: Particles and Fields. 2009 ; Vol. 64, No. 3. pp. 351-360.

Bibtex

@article{d799c57fd00f4f33984b98d4bed0fea6,
title = "Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data",
abstract = "Event Shape Data from e+e− annihilation into hadrons collected by the JADE experiment at centre-of-mass energies between 14 GeV and 44 GeV are used to determine the strong coupling αS. QCD predictions complete to next-to-next-to-leading order (NNLO), alternatively combined with resummed next-to-leading-log-approximation (NNLO + NLLA) calculations, are used. The combined value from six different event shape observables at the six JADE centre-of-mass energies using the NNLO calculations is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1210±0.0007\ensuremath(stat.)±0.0021\ensuremath(exp.)±0.0044\ensuremath(had.)±0.0036\ensuremath(theo.) and with the NNLO + NLLA calculations the combined value is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1172±0.0006\ensuremath(stat.)±0.0020\ensuremath(exp.)±0.0035\ensuremath(had.)±0.0030\ensuremath(theo.). The stability of the NNLO and NNLO + NLLA results with respect to missing higher order contributions, studied by variations of the renormalisation scale, is improved compared to previous results obtained with NLO + NLLA or with NLO predictions only. The observed energy dependence of αS agrees with the QCD prediction of asymptotic freedom and excludes absence of running with 99% confidence level.",
author = "{JADE Collaboration} and Christopher Bowdery and Alexander Finch and Frank Foster and Gareth Hughes",
year = "2009",
month = dec,
doi = "10.1140/epjc/s10052-009-1149-1",
language = "English",
volume = "64",
pages = "351--360",
journal = "European Physical Journal C: Particles and Fields",
issn = "1434-6044",
publisher = "SPRINGER",
number = "3",

}

RIS

TY - JOUR

T1 - Determination of the strong coupling αS from hadronic event shapes with O(\ensuremathαS3) and resummed QCD predictions using JADE data

AU - JADE Collaboration

AU - Bowdery, Christopher

AU - Finch, Alexander

AU - Foster, Frank

AU - Hughes, Gareth

PY - 2009/12

Y1 - 2009/12

N2 - Event Shape Data from e+e− annihilation into hadrons collected by the JADE experiment at centre-of-mass energies between 14 GeV and 44 GeV are used to determine the strong coupling αS. QCD predictions complete to next-to-next-to-leading order (NNLO), alternatively combined with resummed next-to-leading-log-approximation (NNLO + NLLA) calculations, are used. The combined value from six different event shape observables at the six JADE centre-of-mass energies using the NNLO calculations is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1210±0.0007\ensuremath(stat.)±0.0021\ensuremath(exp.)±0.0044\ensuremath(had.)±0.0036\ensuremath(theo.) and with the NNLO + NLLA calculations the combined value is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1172±0.0006\ensuremath(stat.)±0.0020\ensuremath(exp.)±0.0035\ensuremath(had.)±0.0030\ensuremath(theo.). The stability of the NNLO and NNLO + NLLA results with respect to missing higher order contributions, studied by variations of the renormalisation scale, is improved compared to previous results obtained with NLO + NLLA or with NLO predictions only. The observed energy dependence of αS agrees with the QCD prediction of asymptotic freedom and excludes absence of running with 99% confidence level.

AB - Event Shape Data from e+e− annihilation into hadrons collected by the JADE experiment at centre-of-mass energies between 14 GeV and 44 GeV are used to determine the strong coupling αS. QCD predictions complete to next-to-next-to-leading order (NNLO), alternatively combined with resummed next-to-leading-log-approximation (NNLO + NLLA) calculations, are used. The combined value from six different event shape observables at the six JADE centre-of-mass energies using the NNLO calculations is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1210±0.0007\ensuremath(stat.)±0.0021\ensuremath(exp.)±0.0044\ensuremath(had.)±0.0036\ensuremath(theo.) and with the NNLO + NLLA calculations the combined value is \ensuremath\ensuremathαS(\ensuremathm\ensuremathZ0)=0.1172±0.0006\ensuremath(stat.)±0.0020\ensuremath(exp.)±0.0035\ensuremath(had.)±0.0030\ensuremath(theo.). The stability of the NNLO and NNLO + NLLA results with respect to missing higher order contributions, studied by variations of the renormalisation scale, is improved compared to previous results obtained with NLO + NLLA or with NLO predictions only. The observed energy dependence of αS agrees with the QCD prediction of asymptotic freedom and excludes absence of running with 99% confidence level.

U2 - 10.1140/epjc/s10052-009-1149-1

DO - 10.1140/epjc/s10052-009-1149-1

M3 - Journal article

VL - 64

SP - 351

EP - 360

JO - European Physical Journal C: Particles and Fields

JF - European Physical Journal C: Particles and Fields

SN - 1434-6044

IS - 3

ER -