Bethe--Salpeter equation in QCD
arXiv:hep-ph/9504229 · doi:10.1103/PhysRevD.54.3506
Abstract
We extend to regular QCD the derivation of a confining Bethe--Salpeter equation previously given for the simplest model of scalar QCD in which quarks are treated as spinless particles. We start from the same assumptions on the Wilson loop integral already adopted in the derivation of a semirelativistic heavy quark potential. We show that, by standard approximations, an effective meson squared mass operator can be obtained from our BS kernel and that, from this, by expansion the corresponding Wilson loop potential can be reobtained, spin--dependent and velocity--dependent terms included. We also show that, on the contrary, neglecting spin--dependent terms, relativistic flux tube model is reproduced.
23 pages, revtex
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- Three-body relativistic flux tube model from QCD Wilson-loop approach
- Bound state equation in the Wilson loop approach with minimal surfaces
- Note on universal description of heavy and light mesons
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- Integral equation for gauge invariant quark two-point Green's function in QCD
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- Gauge invariant bound state equations for quark-antiquark systems in QCD
- Confining Bethe--Salpeter equation in QCD