1990
DOI: 10.1016/0370-2693(90)90323-x
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Determination of αs from jet multiplicities measured on the Z0 resonance

Abstract: General rightsIt is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulationsIf you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, … Show more

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Cited by 82 publications
(15 citation statements)
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“…The PYTHIA 6.421 [29] event generator is used for the baseline comparisons and corrections. It implements leading-order (LO) pQCD matrix elements for 2 → 2 processes, p T -ordered parton showers calculated in a leading-logarithmic approximation, an underlying event 3 simulation using multiple-parton interactions, and uses the Lund string model for hadronisation. For studies of systematic uncertainties, jet samples were produced using the HERWIG 6 [30] generator, which also employs LO pQCD matrix elements, but uses an angle-ordered parton shower model and a cluster hadronisation model.…”
Section: Monte Carlo Samplesmentioning
confidence: 99%
See 1 more Smart Citation
“…The PYTHIA 6.421 [29] event generator is used for the baseline comparisons and corrections. It implements leading-order (LO) pQCD matrix elements for 2 → 2 processes, p T -ordered parton showers calculated in a leading-logarithmic approximation, an underlying event 3 simulation using multiple-parton interactions, and uses the Lund string model for hadronisation. For studies of systematic uncertainties, jet samples were produced using the HERWIG 6 [30] generator, which also employs LO pQCD matrix elements, but uses an angle-ordered parton shower model and a cluster hadronisation model.…”
Section: Monte Carlo Samplesmentioning
confidence: 99%
“…They have been measured at e + e − , ep, pp, and pp colliders, as well as in γp and γ γ collisions. They have provided precise measurements of the strong coupling constant, have been used to obtain information about the structure of the proton and photon, and have become important tools for understanding the strong interaction and searching for physics beyond the Standard Model (see, for example, [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]). Searches for new physics using jets in 7 TeV collisions were recently published [20,21].…”
Section: Introductionmentioning
confidence: 99%
“…The matrix element squared for the two quark and two gluon process (2), can be split into two gauge invariant parts as follows [25]:…”
Section: Calculationmentioning
confidence: 99%
“…Important results have been achieved. The strong coupling constant α s has been determined from jet rates and from shape variables [2] and both the flavour independence [3] and the running with √ s [4] have been verified. Three- [5] and four-jet [6] distributions have been studied and their behaviour agrees with QCD predictions calculated to second order in α s .…”
Section: Introductionmentioning
confidence: 96%
“…We proceed by collecting various measurements spanning PETRA, PEP, TRIS-TAN, LEP 102,103,52,104,105,106,107], and in our case, SLC. These measurements represent energies Vs=22-92 GeV in ee-machines.…”
Section: Running Of Amentioning
confidence: 99%