We revisit the extraction of s ðM 2 Þ from the QCD perturbative corrections to the hadronic branching ratio, using an improved fixed-order perturbation theory based on the explicit summation of all renormalization-group accessible logarithms, proposed some time ago in the literature. In this approach, the powers of the coupling in the expansion of the QCD Adler function are multiplied by a set of functions D n , which depend themselves on the coupling and can be written in a closed form by iteratively solving a sequence of differential equations. We find that the new expansion has an improved behavior in the complex energy plane compared to that of the standard fixed-order perturbation theory (FOPT), and is similar but not identical to the contour-improved perturbation theory (CIPT). With five terms in the perturbative expansion we obtain in the MS scheme s ðM 2 Þ ¼ 0:338 AE 0:010, using as input a precise value for the perturbative contribution to the hadronic width of the lepton reported recently in the literature.