Abstract
We compute the running QCD coupling on the lattice by evaluating two-point and three-point off-shell gluon Green's functions in a fixed gauge and imposing non-perturbatioe renormalisation conditions on them. Our exploratory study is performed in the quenched approximation at β = 6.0 on 16 4 and 24 4 lattices. We show that, for momenta in the range 1.8–2.3 GeV, our coupling runs according to the two-loop asymptotic formula, allowing a precise determination of the corresponding Λ parameter. The role of lattice artifacts and finite-volume effects is carefully analysed and these appear to be under control in the momentum range of interest. Our renormalisation procedure corresponds to a momentum subtraction scheme in continuum field theory, and therefore lattice perturbation theory is not needed in order to match our results to the MS scheme, thus eliminating a major source of uncertainty in the determination of α MS Our method can be applied directly to the unquenched case.
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