Universal Journal of Physics and Application Vol. 7(2), pp. 215 - 226
DOI: 10.13189/ujpa.2013.010222
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Solution of the Relativistic Bound State Problem for Hadrons

H.P. Morsch¹, H.P. Morsch^2,*
1 HOFF, Brockmullerstr. 11,D-52428 Julich, Germany
² National Centre for Nuclear Research, Pl-00681 Warsaw, Poland

ABSTRACT

A second order extension of a generalised QED Lagrangian (including boson-boson coupling) has been used to describe hadrons. Assuming massless elementary fermions (quantons) this results in a finite theory without open parameters, which may be regarded as a fundamental description of the strong interaction. Two potentials are deduced, a boson-exchange potential and one, which can be identified with the known confinement potential in hadrons. This formalism has been applied the mesonic systems ω(782), Φ(1020), J/ψ= (3097) and Υ(9460) with a good description of their masses. The most important results are: 1. The confinement of hadrons is not due to colour, but is a general property of relativistic bound states. 2. Massive quarks in the Standard Model (QCD) are understood as effective fermions with a mass given by the binding energy in the boson-exchange potential.

KEYWORDS
Bound state description of had-rons based on a second order Lagrangian with massless fermions (quantons) and boson-boson coupling, Confinement and boson-exchange potential, Quarks understood as effect

Cite This Paper in IEEE or APA Citation Styles
(a). IEEE Format:
[1] H.P. Morsch , H.P. Morsch , "Solution of the Relativistic Bound State Problem for Hadrons," Universal Journal of Physics and Application, Vol. 7, No. 2, pp. 215 - 226, 2013. DOI: 10.13189/ujpa.2013.010222.

(b). APA Format:
H.P. Morsch , H.P. Morsch (2013). Solution of the Relativistic Bound State Problem for Hadrons. Universal Journal of Physics and Application, 7(2), 215 - 226. DOI: 10.13189/ujpa.2013.010222.