Key points are not available for this paper at this time.
We employ a Dyson-Schwinger equation model to effect a unified and uniformly accurate description of light- and heavy-meson observables, which we characterize by heavy-meson leptonic decays, semileptonic heavy-to-heavy and heavy-to-light transitions, BD^*, D, , ; DK^*, K, , radiative and strong decays, B (ₒ) ^*B (ₒ) ; D (ₒ) ^*D (ₒ), D, and the rare BK^* flavor-changing neutral-current process. We elucidate the heavy-quark limit of these processes and, using a model-independent mass formula valid for all nonsinglet pseudoscalar mesons, demonstrate that their mass rises linearly with the mass of their heaviest constituent. In our numerical calculations we eschew a heavy-quark expansion and rely instead on the observation that the dressed c, b-quark mass functions are well approximated by a constant, interpreted as their constituent mass: we find M₂=1. 32 GeV and M₁=4. 65 GeV. The calculated heavy-meson leptonic decay constants and transition form factors are a necessary element in the experimental determination of CKM matrix elements. The results also show that this framework, as employed hitherto, is able to describe vector meson polarization observables well.
Ivanov et al. (Wed,) studied this question.