Abstract

We introduce the running coupling constant of QCD in the high temperature phase, g 2(T) , through a renormalization scheme where the dimensional reduction is optimal at the one-loop level. We then calculate the relevant scale parameter, Λ T , which characterizes the running of g 2(T) with T, using the background field method in the static sector. It is found that Λ T/Λ=e( γE+ 1 22 )/(4π) ≈ 0.148 . We further verify that the coupling g 2(T) is also optimal for lattice perturbative calculations. Our result naturally explains why the high temperature limit of QCD sets in at temperatures as low as a few times the critical temperature. In addition, our Λ t agrees remarkably well with the scale parameter determined from the lattice measurement of the spatial string tension of the SU(2) gauge theory at high T.

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