Quarks in Coulomb gauge perturbation theory
arXiv:0810.4887 · doi:10.1103/PhysRevD.79.045006
Abstract
Coulomb gauge quantum chromodynamics within the first order functional formalism is considered. The quark contributions to the Dyson-Schwinger equations are derived and one-loop perturbative results for the two-point functions are presented.
20 pages, 2 figures
References in corpus (7)
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- Dielectric function of the QCD vacuum
- Propagator Dyson-Schwinger Equations of Coulomb Gauge Yang-Mills Theory Within the First Order Formalism
- Two-Point Functions of Coulomb Gauge Yang-Mills Theory
- Perturbation Theory of Coulomb Gauge Yang-Mills Theory Within the First Order Formalism
- The 't Hooft loop in the Hamiltonian approach to Yang-Mills theory in Coulomb gauge
- Topological susceptibility in SU(2) Yang-Mills theory in the Hamiltonian approach in Coulomb gauge
Cited by in corpus (8)
- The Coulomb gauge ghost Dyson-Schwinger equation
- Running mass, effective energy and confinement: the lattice quark propagator in Coulomb gauge
- Higher order heavy quark Green's functions in Coulomb gauge
- Three-quark confinement potential from the Faddeev equation
- Overlap Quark Propagator in Coulomb Gauge QCD and the Interrelation of Confinement and Chiral Symmetry Breaking
- Heavy tetraquark confining potential in Coulomb gauge QCD
- From asymptotic freedom toward heavy quarkonia within the renormalization group procedure for effective particles
- Quark sector of Coulomb gauge Quantum Chromodynamics