Confinement, quark mass functions, and spontaneous chiral symmetry breaking in Minkowski space

Abstract

We formulate the covariant equations for quark-antiquark bound states in Minkowski space in the framework of the Covariant Spectator Theory. The quark propagators are dressed with the same kernel that describes the interaction between different quarks. We show that these equations are charge-conjugation invariant, and that in the chiral limit of vanishing bare quark mass, a massless pseudoscalar bound state is produced in a Nambu-Jona-Lasinio (NJL) mechanism, which is associated with the Goldstone boson of spontaneous chiral symmetry breaking. In this introductory paper, we test the formalism by using a simplified kernel consisting of a momentum-space delta-function with a vector Lorentz structure, to which one adds a mixed scalar and vector confining interaction. The scalar part of the confining interaction is not chirally invariant by itself, but decouples from the equations in the chiral limit and therefore allows the NJL mechanism to work. With this model we calculate the quark mass function, and we compare our Minkowski-space results to lattice QCD data obtained in Euclidean space. In a companion paper, we apply this formalism to a calculation of the pion form factor.

17 pages, 12 figures, version published in Phys. Rev. D

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• Infrared Properties of QCD from Dyson-Schwinger equations
• The Flavor Structure of the Excited Baryon Spectra from Lattice QCD
• Covariant spectator theory of np scattering: Phase shifts obtained from precision fits to data below 350 MeV
• Nucleon Compton scattering in the Dyson-Schwinger approach
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