Abstract
When expanded in powers of α¯ where α¯ is chosen to satisfy α¯(Q02)=4πβ0ln(Q02Λ2)=αMS(Q02) with Q0210 GeV2, the quantum chromodynamics (QCD) perturbation series seems to be extremely well behaved. In particular, the large third-order corrections discussed recently by Moshe do not appear when this α¯ is used as the QCD expansion parameter.