The Nf3 g6 term in the pressure of hot QCD

Abstract

We determine the first independent part of the g6 coefficient in the weak coupling expansion of the QCD pressure at high temperatures, the one proportional to the maximal power of the number of quark flavors Nf. In addition to introducing and developing computational methods that can be used in evaluating other parts of the expansion, our calculation provides a result that becomes dominant in the limit of large Nf and a fixed effective coupling geff2 = g2 Nf/2.

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