Adjoint Wilson Line in SU(2) Lattice Gauge Theory
arXiv:hep-lat/9307012 · doi:10.1103/PhysRevD.49.528
Abstract
The behavior of the adjoint Wilson line in finite-temperature, , lattice gauge theory is discussed. The expectation value of the line and the associated excess free energy reveal the response of the finite-temperature gauge field to the presence of an adjoint source. The value of the adjoint line at the critical point of the deconfining phase transition is highlighted. This is not calculable in weak or strong coupling. It receives contributions from all scales and is nonanalytic at the critical point. We determine the general form of the free energy. It includes a linearly divergent term that is perturbative in the bare coupling and a finite, nonperturbative piece. We use a simple flux tube model to estimate the value of the nonperturbative piece. This provides the normalization needed to estimate the behavior of the line as one moves along the critical curve into the weak coupling region.
21 pages, no figures, Latex/Revtex 3, UCD-93-19
References in corpus (1)
Cited by in corpus (10)
- Quark-Gluon Plasma as a Condensate of Z(3) Wilson Lines
- Deconfining Phase Transition as a Matrix Model of Renormalized Polyakov Loops
- Polyakov Loops versus Hadronic States
- Critical Behavior of Non Order-Parameter Fields
- Induced Universal Properties and Deconfinement
- Screening and Deconfinement of Sources in Finite Temperature SU(2) Lattice Gauge Theory
- Partial Deconfinement in Color Superconductivity
- The decay of unstable k-strings in SU(N) gauge theories at zero and finite temperature
- Critical Exponent for the Density of Percolating Flux
- Critical exponents for higher-representation sources in 3D SU(3) gauge theory from CFT