Lattice gauge theory

Quantum mechanics

Quark

Functional renormalization group

Mathematical physics

Lattice QCD

Particle physics

Gluon

Gauge theory

Observable

Physics

Renormalization group

Quantum electrodynamics

Propagator

Renormalization

Lattice field theory

Quantum chromodynamics

Physical review. D/Physical review. D.

We present a comprehensive study of the quark sector of $2+1$ flavor QCD, based on a self-consistent treatment of the coupled system of Schwinger-Dyson equations for the quark propagator and the full quark-gluon vertex in the one-loop dressed approximation. The individual form factors of the quark-gluon vertex are expressed in a special tensor basis obtained from a set of gauge-invariant operators. The sole external ingredient used as input to our equations is the Landau gauge gluon propagator with $2+1$ dynamical quark flavors, obtained from studies with Schwinger-Dyson equations, the functional renormalization group approach, and large volume lattice simulations. The appropriate renormalization procedure required in order to self-consistently accommodate external inputs stemming from other functional approaches or the lattice is discussed in detail, and the value of the gauge coupling is accurately determined at two vastly separated renormalization group scales. Our analysis establishes a clear hierarchy among the vertex form factors. We identify only three dominant ones, in agreement with previous results. The components of the quark propagator obtained from our approach are in excellent agreement with the results from Schwinger-Dyson equations, the functional renormalization group, and lattice QCD simulation, a simple benchmark observable being the chiral condensate in the chiral limit, which is computed as $(245\text{ }\text{ }\mathrm{MeV}{)}^{3}$. The present approach has a wide range of applications, including the self-consistent computation of bound-state properties and finite temperature and density physics, which are briefly discussed.

Fully coupled functional equations for the quark sector of QCD