Abstract

The QCD coupling αs is determined at NLO*+NMLLA accuracy from the comparison of experimental jet data to theoretical predictions of the energy-evolution of the parton-to-hadron fragmentation function moments (multiplicity, peak, width, skewness) at low fractional hadron momentum z. From the existing e+e− and e±p jet data, we obtain αs(mZ2)=0.1195±0.0021(exp)−0.0+0.0015(scale) at the Z mass. The uncertainties of the extracted αs value are discussed.

Highlights

  • In the chiral limit, the theory of the strong interaction –quantum chromodynamics (QCD)–has a single fundamental parameter: its coupling αs which decreases logarithmically with increasing energy scale Q, i.e. αs ∝ln(Q2/Λ2 ), starting from a value QCDΛQCD ≈ 0.2 GeV where the perturbatively-defined coupling diverges

  • In Ref. [5] we have presented a novel extraction of αs from the energy evolution of the first four moments of the parton-to-hadron fragmentation functions (FFs) including, for the first time, resummations of higher-order (NNLL or NMLLA) logarithms and NLO running-coupling corrections

  • hump-backed plateau” (HBP) moments which depend only on ΛQCD. Such an approach is justified for infrared-safe observables by the “local parton-hadron duality” hypothesis which states that the distribution of partons in jets is identical to that of the final hadrons

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Summary

Introduction

In the chiral (massless quark) limit, the theory of the strong interaction –quantum chromodynamics (QCD)–. [3]) to try to measure ΛQCD (or, equivalently, αs) using partonto-hadron fragmentation functions (FFs) in the region of low fractional momenta z = ph/pparton via the Modified Leading Logarithmic Approximation (MLLA) [4] which resums the soft and collinear singularities present in this region of phase-space These older calculations were limited to LO approximations with a number of simplifying assumptions: (i) ad hoc cuts in the experimental distributions, (ii) simple fits in a restricted FF range, (iii) number of quark-flavours fixed to N f = 3, and (iv) use of only one or two FF moments (Gaussian approximation). S= 3.8 GeV [ZEUS'95] s= 5.3 GeV [ZEUS'95] s= 7.3 GeV [ZEUS'95] s= 10.4 GeV [ZEUS'95]

2: Charged-hadron distributions in jets as a function of ξ
Experimental uncertainties on αs
Theoretical uncertainties on αs
Conclusions
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