Abstract

We study the flavorless gluon propagator in the Landau gauge from high statistics lattice calculations. Hypercubic artifacts are efficiently eliminated by taking the ∑pμ4→0\sum p_μ^4 \to 0 limit. The propagator is fitted to the three-loops perturbative formula in an energy window ranging form ∼\sim 2.5 GeV up to ∼\sim 5.5 GeV. αsα_s is extracted from the best fit in a continuous set of renormalisation schemes. The fits are very good, with a χ2χ^2 per d.o.f smaller than 1. We propose a more stringent test of asymptotic scaling based on scheme independence of the resulting ΛMˉSΛ_{\bar MS}. This method shows that asymptotic scaling at three loops is not reached by the gluon propagator although we use rather large energies. We are only able to obtain an effective flavorless three-loops estimate ΛMˉS(3)=353±2−10+25Λ_{\bar MS}^{(3)}= 353 \pm 2 ^{+25}_{-10} MeV. We argue that the real asymptotic value for ΛMˉSΛ_{\bar MS} should plausibly be smaller.

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