We discuss the leptonic decay constants of heavy--light mesons by means of
Borel QCD sum~rules in the local-duality (LD) limit of infinitely large Borel
mass parameter. In this limit, for an appropriate choice of the invariant
structures in the QCD correlation functions, all vacuum-condensate
contributions vanish and all nonperturbative effects are contained in only one
quantity, the effective threshold. We study properties of the LD effective
thresholds in the limits of large heavy-quark mass mQ and small light-quark
mass mq. In the heavy-quark limit, we clarify the role played by the
radiative corrections in the effective threshold for reproducing the pQCD
expansion of the decay constants of pseudoscalar and vector mesons. We show
that the dependence of the meson decay constants on mq arises predominantly
(at the level of 70--80%) from the calculable mq-dependence of the
perturbative spectral densities. Making use of the lattice QCD results for the
decay constants of nonstrange and strange pseudoscalar and vector heavy mesons,
we obtain solid predictions for the decay constants of heavy--light mesons as
functions of mq in the range from a few to 100 MeV and evaluate the
corresponding strong isospin-breaking effects: fD+−fD0=(0.96±0.09)MeV, fD∗+−fD∗0=(1.18±0.35)MeV,
fB0−fB+=(1.01±0.10)MeV, fB∗0−fB∗+=(0.89±0.30)MeV.Comment: 14 pages. Typo corrected: the term describing power corrections in
Eq.(1.1), which was lost when updating v2 -> v3, is restored. Notice that
this term is also lost in the EPJC version (to be corrected via Erratum