We study center vortex free energies and ’t Hooft’s electric fluxes on the lattice in 2+1 dimen-sions, where SU(2) for example, is in the universality class of the 2d Ising model. This places a wealth of exact results at our fingertips. In particular, spacelike center vortices in SU(2) near criticality correspond to spin interfaces in the 2d Ising model, whose universal scaling functions are known exactly. We exploit this to locate the deconfinement transition with unprecedented precision and subsequently for a finite size scaling analysis, where the self-duality of the 2d spin model is reflected in a duality between the spacelike vortices and confining electric fluxes. The corresponding relation between the string tension and its dual in t...
Adding separate chemical potentials λ and γ for Z2 monopoles and vortices, respectively, i...
The vortex state which arises from a projection of SU(2) to $Z_2$ gauge theory is studied at finite ...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
Abstract. The 2+1 dimensional pure SU(N) gauge theories with N ≤ 4 are candidates for applying the p...
We present a precision determination of the critical coupling βc for the deconfinement transition in...
We study the pure SU(3) gauge theory in 2+1 dimensions on the lattice using ’t Hooft’s twisted bound...
AbstractWe present a precision determination of the critical coupling βc for the deconfinement trans...
Engels J, Kehl E, Satz H, Waltl B. Deconfinement for SU(2) gauge theory in 2+1 dimensions. Physical ...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
We calculate the variation with temperature of the vortex free energy in D=2+1 SU(2) lattice gauge t...
We investigate the effect of Z2 magnetic monopoles and vortices on the finite temperature deconfinem...
In the vicinity of the deconfinement transition the behaviour of the interquark potential can be pre...
13 pages, 4 eps figures, LaTeX; reference addedWe study the flux tube thickness in the confining pha...
Adding separate chemical potentials λ and γ for Z2 monopoles and vortices, respectively, i...
Adding separate chemical potentials λ and γ for Z2 monopoles and vortices, respectively, i...
The vortex state which arises from a projection of SU(2) to $Z_2$ gauge theory is studied at finite ...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
Abstract. The 2+1 dimensional pure SU(N) gauge theories with N ≤ 4 are candidates for applying the p...
We present a precision determination of the critical coupling βc for the deconfinement transition in...
We study the pure SU(3) gauge theory in 2+1 dimensions on the lattice using ’t Hooft’s twisted bound...
AbstractWe present a precision determination of the critical coupling βc for the deconfinement trans...
Engels J, Kehl E, Satz H, Waltl B. Deconfinement for SU(2) gauge theory in 2+1 dimensions. Physical ...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...
We calculate the variation with temperature of the vortex free energy in D=2+1 SU(2) lattice gauge t...
We investigate the effect of Z2 magnetic monopoles and vortices on the finite temperature deconfinem...
In the vicinity of the deconfinement transition the behaviour of the interquark potential can be pre...
13 pages, 4 eps figures, LaTeX; reference addedWe study the flux tube thickness in the confining pha...
Adding separate chemical potentials λ and γ for Z2 monopoles and vortices, respectively, i...
Adding separate chemical potentials λ and γ for Z2 monopoles and vortices, respectively, i...
The vortex state which arises from a projection of SU(2) to $Z_2$ gauge theory is studied at finite ...
We study connections between global symmetries, topological objects, and phase transitions in non-ab...