Abstract
A technique for estimating the large-order QCD perturbative contributions to the total e+ e total cross section is presented which is based upon the renormalization group and momentum analyticity. Our estimate for the coefficient of (αs)3 has recently been confirmed by two exact calculations. We find that the effective expansion parameter is, in fact, not αs/π but rather 4π2 eb1(αs/π), where b1 is the first coefficient in the expansion of the β function.