“…Broadly speaking, there are two approaches: (i) an inclusive one employing the operator product expansion (OPE), which expands in powers of Λ QCD /m c , as in the heavy quark expansion (HQE), and assumes that local quark-hadron duality holds [206][207][208][209]; and (ii) an exclusive one in which y is estimated by summing over contributions of exclusive states, and x is estimated via a dispersion relation which relates it to y. In the first approach, the HQE applied to Γ D 12 , combined with the relevant non-perturbative dimension six operator matrix elements evaluated in [210][211][212][213], yields contributions of the individual Γ ij to y that are five times larger than the experimental value [214]. This corresponds to Γ ij ∼ Γ D , which is not surprising, given that the HQE can accommodate the charm meson lifetimes [213,215].…”