Confinement in the q-state Potts field theory
arXiv:0706.1020 · doi:10.1016/j.nuclphysb.2007.09.003
Abstract
The q-state Potts field theory describes the universality class associated to the spontaneous breaking of the permutation symmetry of q colors. In two dimensions it is defined up to q=4 and exhibits duality and integrability away from critical temperature in absence of magnetic field. We show how, when a magnetic field is switched on, it provides the simplest model of confinement allowing for both mesons and baryons. Deconfined quarks (kinks) exist in a phase bounded by a first order transition on one side, and a second order transition on the other. The evolution of the mass spectrum with temperature and magnetic field is discussed.
21 pages, 8 figures. v2: references added
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- Fields, particles and universality in two dimensions
- Field theory of Ising percolating clusters
- On superuniversality in the -state Potts model with quenched disorder
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- Radiative corrections to the quark masses in the ferromagnetic Ising and Potts field theories
- Quasi-particle spectrum and entanglement generation after a quench in the quantum Potts spin chain
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- Bound States of Majorana Fermions in Semi-classical Approximation
- Even-odd effects in the SU() Heisenberg spin chain
- Escaping fronts in local quenches of a confining spin chain
- Critical points in coupled Potts models and correlated percolation
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