We study the conformal window of QCD using perturbation theory, starting from the perturbative upper edge and going down as much as we can towards the strongly coupled regime. We do so by exploiting the available five-loop computation of the MS ̄ β-function and employing Borel resummation techniques both for the ordinary perturbative series and for the Banks-Zaks conformal expansion. Large-nf results are also used. We argue that the perturbative series for the MS ̄ β-function is most likely asymptotic and non -Borel resummable, yet Borel resummation techniques allow to improve on ordinary perturbation theory. We find substantial evidence that QCD with nf = 12 flavours flows in the IR to a conformal field theory. Though the evidence is weaker, we find indications that also nf = 11 might sit within the conformal window. We also compute the anomalous dimensions γ and γg of respectively the fermion mass bilinear and the gauge kinetic term operator at the fixed point, and compare them with the available lattice results. The conformal window might extend for lower values of nf , but our methods break down for nf< 11, where we expect that non-perturbative effects become important. A similar analysis is performed in the Veneziano limit.
