The parametrization $\alpha_s = \alpha_s (Q^2)$ in the DGLAP evolution equations comes from the parametrization $\alpha_s = \alpha_s(k_T^2)$ in every rung of the ladder graphs. Such a
parametrization comes from analysis of QCD reactions in the Hard kinematics. I address it as Standard Parametrization.
However, our analysis demonstrates that actually this expression should be replaced by an effective coupling $\alpha_s^{eff}$ given by a much more involved expression. Nevertheless, when the starting point $\mu^2$ of the $Q^2$ -evolution is chosen high enough, Standard Parametrization can be used. The criterion is $\mu^2 \gg \Lambda^2_{QCD} \exp(\pi)$