A Covariant Light-Front Model of Heavy Mesons within HQET
arXiv:hep-ph/9709412 · doi:10.1103/PhysRevD.57.5598
Abstract
In this paper we construct a covariant light-front model of heavy mesons within the framework of heavy quark effective theory (HQET). The covariant model consists of the light-front heavy meson bound states constructed in the heavy quark limit with heavy quark symmetry and heavy quark effective theory as its basis. Within this model, the Isgur-Wise function and decay constants in the infinite quark mass limit can be evaluated in a very simple and the most general way. The results are ensured to be consistent with heavy quark symmetry. From the heavy-quark-limit bound states, we can further develop a systematic approach to calculate corrections from the expansion of QCD. This covariant model can serve as a quasi-first-principles description of heavy meson dynamics, namely, a phenomenological covariant bound state in the heavy quark limit which is consistent with heavy quark symmetry, plus a reliable first-principles computation of the corrections in HQET in terms of the expansion of the fundamental QCD theory.
23 pages, 6 figures, revised for its publication in Phys. Rev. D
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Cited by in corpus (24)
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- Electroweak form factors of heavy-light mesons -- a relativistic point-form approach
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- SU(3) symmetry breaking in decay constants and electromagnetic properties of pseudoscalar heavy mesons
- Angular distribution of the FCNC process
- Radiative leptonic decays of heavy mesons in heavy quark limit
- Numerical analysis of the production of , and their partners through the semileptonic decays of mesons in terms of the light-front quark model
- Nonperturbative Determination of Heavy Meson Bound States
- Spectroscopy of excited quarkonium states in the light-front quark model
- to Transition Form Factors and Semileptonic Decays in Self-consistent Covariant Light-front Approach
- Effective Field Theory of Heavy Mesons
- Three symmetry breakings in strong and radiative decays of strange heavy mesons
- Heavy-light quark systems from the QCD instanton vacuum: light flavor case