Abstract

We examine, in the `t Hooft renormalization scheme, the analytic running coupling αˉt(Q2)\barα_t(Q^2) in QCD, using the two-loop ββ-function with positive expansion parameters β0β_0 and β1β_1. An exact integral representation is derived for this causal coupling, which is fully expressed in terms of the imaginary part of the Lambert function WW. This integral form manifestly accounts for the universal value of the infrared limit αˉt(Q2=0)=4π/β0\barα_t(Q^2=0)= 4 π/β_0.

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