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We provide here all the procedures in which are needed for the computation of the analytic images of the strong coupling constant powers in Minkowski ( and ${\mathfrak A_{\nu}^(s)}{\bar{\mathcal A}{\nu}(Q^2;n_f)}{\mathcal A{\nu}^(Q^2)}$) domains at arbitrary energy scales ( and , correspondingly) for both schemes — with fixed number of active flavours and the global one with taking into account all heavy-quark thresholds. These singularity-free couplings are inevitable elements of Analytic Perturbation Theory (APT) in QCD and its generalization — Fractional APT, needed to apply the APT imperative for renormalization-group improved hadronic observables.

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