2025/09/10 by Ayala, Cesar, Cvetič, Gorazd, Kögerler, Reinhart
#FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #High Energy Physics - Theory (hep-th)
paper · doi:10.48550/arxiv.2509.09042
We present a generalisation of our previous approach of a renormalon-motivated resummation of the QCD observables. Previously it was applied to the spacelike observables whose perturbation expansion was D(Q2) = a(Q2) + O(a2), where a(Q2) ≡ αs(Q2)/π is the running QCD coupling. Now we generalise the resummation to spacelike quantities D(Q2) = a(Q2)ν0 + O(aν0+1) and timelike quantities F(σ) = a(σ)ν0 + O(aν0+1), where ν0 is in general a noninteger number (0<ν0 ≤ 1). We evaluate with this approach a timelike quantity, namely the scheme-invariant factor of the Wilson coefficient of the chromomagnetic operator in the heavy-quark effective Lagrangian, and related quantities.