Abstract
Data from ${\rm e^+e^-}$ annihilation into hadrons, taken with the ALEPH detector at the Z resonance, are analyzed. The four-jet rate is studied as a function of the resolution parameter and compared to next-to-leading order calculations combined with resummation of large logarithms. Angular correlations in four-jet events are measured and compared to next-to-leading order QCD predictions. With these observables two different measurements are performed. In a first analysis the strong coupling constant is measured from the four-jet rate yielding $\alpha_s(M_{\mathrm Z}) = 0.1170 \pm 0.0001 ({\rm stat}) \pm 0.0013 ({\rm sys})$ . In a second measurement the strong coupling constant and the QCD colour factors are determined simultaneously from a fit to the four-jet rate and the four-jet angular correlations, giving $\alpha_s(M_{\rm Z}) = 0.119 \pm 0.006 ({\rm stat}) \pm 0.026 ({\rm sys})$ $C_{\rm A} = 2.93 \pm 0.14 ({\rm stat}) \pm 0.58 ({\rm sys})$ $C_{\rm F} = 1.35 \pm 0.07 ({\rm stat}) \pm 0.26 ({\rm sys})$ in good agreement with the expectation from QCD.
Highlights
Electron-positron annihilation into hadrons at high energy is a well suited process to test Quantum Chromodynamics (QCD) since the initial state is well known and longdistance effects are typically small
The four-jet rate is studied as a function of the resolution parameter and compared to next-toleading order calculations combined with resummation of large logarithms
In a first analysis the strong coupling constant is measured from the four-jet rate yielding αs(MZ) = 0.1170 ± 0.0001(stat) ± 0.0013(sys)
Summary
Electron-positron annihilation into hadrons at high energy is a well suited process to test Quantum Chromodynamics (QCD) since the initial state is well known and longdistance effects are typically small. Many QCD studies have been carried out at LEP, in particular precise measurements of the strong coupling constant αs(MZ) [1] and tests of the structure of the underlying gauge group [2, 3], which is SU(3) in the case of QCD. Four-jet events are interesting, since QCD shows its full gauge structure only from order αs on. A much more powerful method for testing these hypotheses makes use of the different correlations among the final-state particles induced by the various contributions to the cross section. These correlations have their origin in the different angular momentum properties of the final state
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