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$α_s$ at Zinnowitz 2004

Siegfried Bethke

TL;DR

α_s is reviewed with status up to April 2004, confirming its energy-scale dependence in agreement with QCD. The paper compiles results from DIS, e+e− annihilation, and hadron colliders, emphasizing NNLO calculations and a careful world-average methodology. A world average of α_s(M_Z) = 0.1182 ± 0.0027 is reported, with Λ_MS̄ values provided for different flavor counts, illustrating consistency across processes. The findings reinforce the QCD prediction for the running of α_s and deliver a precise global value for future phenomenology.

Abstract

A review of measurements of $α_s$ is given, representing the status of April 2004. The results prove the energy dependence of $α_s$ and are in excellent agreement with the expectations of Quantum Chromodynamics, QCD. Evolving all results to the rest energy of the $Z^0$ boson, the world average of $α_s(M_Z)$ is determined from measurements which are based on QCD calculations in complete NNLO perturbation theory, giving $α_s(M_Z) = 0.1182 \pm 0.0027 .$

$α_s$ at Zinnowitz 2004

TL;DR

α_s is reviewed with status up to April 2004, confirming its energy-scale dependence in agreement with QCD. The paper compiles results from DIS, e+e− annihilation, and hadron colliders, emphasizing NNLO calculations and a careful world-average methodology. A world average of α_s(M_Z) = 0.1182 ± 0.0027 is reported, with Λ_MS̄ values provided for different flavor counts, illustrating consistency across processes. The findings reinforce the QCD prediction for the running of α_s and deliver a precise global value for future phenomenology.

Abstract

A review of measurements of is given, representing the status of April 2004. The results prove the energy dependence of and are in excellent agreement with the expectations of Quantum Chromodynamics, QCD. Evolving all results to the rest energy of the boson, the world average of is determined from measurements which are based on QCD calculations in complete NNLO perturbation theory, giving

Paper Structure

This paper contains 6 sections, 14 equations, 4 figures, 2 tables.

Figures (4)

  • Figure 1: $\alpha_{\rm s} (E^{jet}_T )$ values determined from QCD fits of the measured $d \sigma \over dE^{jet}_T$ from ZEUS zeus03. The solid line corresponds to the central value of $\alpha_{\rm s}(M_{\rm Z^0})$ determined in zeus03, the dashed line represents the world average as2002.
  • Figure 2: Summary of measurements of $\alpha_{\rm s} (Q^2 )$ from electroweak precision measurements (filled symbols; in NNLO QCD) and from jet and event shape observables (open symbols; in resummed NLO QCD) in ${\rm e^+\rm e^-}$ annihilation. The dashed curves represent the world average of $\alpha_{\rm s}(M_{\rm Z^0})$lepqcd04.
  • Figure 3: Summary of measurements of $\alpha_{\rm s} (Q^2 )$. Results which are based on fits of $\alpha_{\rm s}(M_{\rm Z^0})$ to data in $ranges$ of $Q$, assuming the QCD running of $\alpha_{\rm s}$, are not shown here but are included in the overall summary of $\alpha_{\rm s}(M_{\rm Z^0})$, see Figure 4 and Table 1.
  • Figure 4: Summary of measurements of $\alpha_{\rm s}(M_{\rm Z^0})$. Filled symbols represent results based on complete NNLO QCD calculations.