5 Citations
Provable First-Order Transitions for Nonlinear Vector and Gauge Models with Continuous Symmetries
- Physics
- 2003
We consider various sufficiently nonlinear vector models of ferromagnets, of nematic liquid crystals and of nonlinear lattice gauge theories with continuous symmetries. We show, employing the method…
First-order transitions for very nonlinear sigma models.
- Physics
- 2005
In this contribution we discuss the occurrence of first-order transitions in temperature in various short-range lattice models with a rotation symmetry. Such transitions turn out to be widespread…
First-order transitions for very nonlinear sigma models
- Physics
- 2008
In this contribution we discuss the occurrence of first-order transitions in temperature in various short-range lattice models with a rotation symmetry. Such transitions turn out to be widespread…
Light Hadron Masses from Lattice QCD
- Physics
- 2012
This article reviews lattice QCD results for the light hadron spectrum. An overview of different formulations of lattice QCD with discussions on the fermion doubling problem and improvement programs…
References
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FIRST ORDER SIGNATURES IN 4D PURE COMPACT U(1) GAUGE THEORY WITH TOROIDAL AND SPHERICAL TOPOLOGIES
- Physics, Mathematics
- 1998
Softly Broken N = 2 QCD
- Physics
- 1996
We analyze the possible soft breaking of (N = 2)-supersymmetric Yang–Mills theory with and without matter flavor preserving the analyticity properties of the Seiberg–Witten solution. For a small…
Electromagnetic fluxes, monopoles, and the order of 4d compact U(1) phase transition
- Physics, Mathematics
- 2004
Non-Gaussian Fixed Point in Four-Dimensional Pure Compact U(1) Gauge Theory on the Lattice.
- PhysicsPhysical review letters
- 1996
The line of phase transitions separating the confinement phase from the Coulomb phase in the four-dimensional pure compact U(1) gauge theory with extended Wilson action is reconsidered and found that along a part of this line, including the Wilson action the critical scaling behavior is determined by one fixed point with non-Gaussian critical exponent {nu}=0.365(8).