“…For completeness, we recall the definitions of the four angular variables [43,44,45,46] introduced in the previous Section. One first orders the jets in energy such that…”
Section: (I J ) Represent Gluon(quark) Colour Indices Yieldingmentioning
confidence: 99%
“…[48] (hereafter denoted by Φ * KSW ), which is more sensitive than the original to the flavour composition (see Refs. [44,48]). Thus, in events for which…”
Section: (I J ) Represent Gluon(quark) Colour Indices Yieldingmentioning
Existence of discrepancies between experimental data and Monte Carlo predictions for angular distributions in four-jet production via e + e − annihilation has been known for some time at LEP1. As such QCD processes constitute significant backgrounds to e + e − → W + W − → 4-jet production at LEP2, we consider the possibility that an erroneous modelling of the helicity structure of the finalstate partons could affect the accuracy of experimental measurements of the W ± boson parameters.
“…For completeness, we recall the definitions of the four angular variables [43,44,45,46] introduced in the previous Section. One first orders the jets in energy such that…”
Section: (I J ) Represent Gluon(quark) Colour Indices Yieldingmentioning
confidence: 99%
“…[48] (hereafter denoted by Φ * KSW ), which is more sensitive than the original to the flavour composition (see Refs. [44,48]). Thus, in events for which…”
Section: (I J ) Represent Gluon(quark) Colour Indices Yieldingmentioning
Existence of discrepancies between experimental data and Monte Carlo predictions for angular distributions in four-jet production via e + e − annihilation has been known for some time at LEP1. As such QCD processes constitute significant backgrounds to e + e − → W + W − → 4-jet production at LEP2, we consider the possibility that an erroneous modelling of the helicity structure of the finalstate partons could affect the accuracy of experimental measurements of the W ± boson parameters.
“…The polar angle G between the thrust axis in (2.1)(respectively the photon momentum in {2.2)) and the beam axis should be easy to measure experimentally, how the nonabelian structure of QCO influences the predictions for these polar correlations are discussed in section 4. In section 5 we study azimuthal angular correlations between event planes which have been discussed also in four jet oroduction in the e+e-continuum [9].…”
Section: Desy Behiilt Sich Aile Rechte Fur Den Fall Der Schutzrechtsementioning
“…The 4-jet angles measured are the Bengtsson-Zerwas [11] angle, χ BZ , the modified Nachtmann-Reiter [12] angle, Θ NR , the Körner-Schierholtz-Willrodt [13] angle, Φ KSW , and the angle between the two lowest energy jets, α 34 . Fig.…”
Section: Determination Of α S From 4-jet Ratesmentioning
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