“…The perturbative corrections to the coefficient of the matrix element of the kinetic operator have been evaluated at order α 2 s for generic observables, such as partial rates and moments [31,32]. Corrections at order α 2 s to the coefficient of the matrix element of the chromomagnetic [39,9,10] 39.54 ± 0.50 exp ± 0.74 th Rome (Lattice quenched ω = 1) [13,14] 37.4 ± 0.5 exp ± 0.8 th HFAG (Sum Rules) [15,16,39] 41.6 ± 0.6 exp ± 1.9 th…”