From the Feynman-Schwinger representation to the non-perturbative relativistic bound state interaction

Details From the Feynman-Schwinger representation to the non-perturbative relativistic bound state interaction From the Feynman-Schwinger representation to the non-perturbative relativistic bound state interaction

1997-03-20

arxiv.org/abs/hep-ph/9703378v2

Phys.Rev. D56 (1997) 1445-1454

Physics

High Energy Physics

High Energy Physics - Phenomenology

25 pages, RevTex, 3 figures included, typos corrected, to appear in Phys. Rev. D 56

Scientific paper

10.1103/PhysRevD.56.1445

We write the 4-point Green function in QCD in the Feynman-Schwinger
representation and show that all the dynamical information are contained in the
Wilson loop average. We work out the QED case in order to obtain the usual
Bethe-Salpeter kernel. Finally we discuss the QCD case in the non-perturbative
regime giving some insight in the nature of the interaction kernel.

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