Revised variational approach to QCD in Coulomb gauge

Abstract

The variational approach to QCD in Coulomb gauge is revisited. By assuming the non-Abelian Coulomb potential to be given by the sum of its infrared and ultraviolet parts, i.e.~by a linearly rising potential and an ordinary Coulomb potential, and by using a Slater determinant ansatz for the quark wave functional, which contains the coupling of the quarks and the gluons with two different Dirac structures, we obtain variational equations for the kernels of the fermionic vacuum wave functional, which are free of ultraviolet divergences. Thereby, a Gaussian type wave functional is assumed for the gluonic part of the vacuum. By using the results of the pure Yang--Mills sector for the gluon propagator as input, we solve the equations for the fermionic kernels numerically and calculate the quark condensate and the effective quark mass in leading order. Assuming a value of ${\sigma }_{\mathrm{C}}=2.5\sigma$ for the Coulomb string tension (where $\sigma$ is the usual Wilsonian string tension) the phenomenological value of the quark condensate $⟨\bar{\psi }\psi ⟩\simeq (-235\mathrm{MeV}{)}^3$ is reproduced with a value of $g\simeq 2.1$ for the strong coupling constant of the quark-gluon vertex.

References in corpus (7)

• Confining Solution of the Dyson-Schwinger Equations in Coulomb Gauge
• Coulomb gauge gluon propagator and the Gribov formula
• $\bar{q}q$ condensate for light quarks beyond the chiral limit
• The effective Coulomb potential in SU(3) lattice Yang-Mills theory
• Hamiltonian Flow in Coulomb Gauge Yang-Mills Theory
• Scaling study of the gluon propagator in Coulomb gauge QCD on isotropic and anisotropic lattices
• Coulomb string tension, asymptotic string tension, and the gluon chain

Cited by in corpus (1)

• The Equal-Time Quark Propagator in Coulomb Gauge