Meson decay in a corrected model
arXiv:0810.0293 · doi:10.1103/PhysRevD.78.076004
Abstract
Extensively applied to both light and heavy meson decay and standing as one of the most successful strong decay models is the model, in which pair production is the dominant mechanism. The pair production can be obtained from the non-relativistic limit of a microscopic interaction Hamiltonian involving Dirac quark fields. The evaluation of the decay amplitude can be performed by a diagrammatic technique for drawing quark lines. In this paper we use an alternative approach which consists in a mapping technique, the Fock-Tani formalism, in order to obtain an effective Hamiltonian starting from same microscopic interaction. An additional effect is manifest in this formalism associated to the extended nature of mesons: bound-state corrections. A corrected is obtained and applied, as an example, to and decays.
3 figures. To appear in Physical Review D
References in corpus (17)
- Big-Bang nucleosynthesis (Particle Data Group mini-review)
- The Cosmological Parameters 2006
- Higher Charmonia
- Glueballs, Hybrids, Multiquarks. Experimental facts versus QCD inspired concepts
- On the Mechanism of Open-Flavor Strong Decays
- Higher Quarkonia
- Strong Decays of Strange Quarkonia
- Scalar Glueball-qqbar Mixing above 1 GeV and implications for Lattice QCD
- Glueball-quarkonia content and decay of scalar-isoscalar mesons
- NN Core Interactions and Differential Cross Sections from One Gluon Exchange
- Mapping of composite hadrons into elementary hadrons and effective hadronic Hamiltonians
- Short-range repulsion and isospin dependence in the KN system
- The XYZs of Charmonium at BES
- Long- and medium-range components of the nuclear force in quark-model based calculations
- Second quantization approach to composite hadron interactions in quark models
- Can quark effects be observed in intermediate heavy ion collisions?
- Do glueballs contribute in heavy ion collisions?