BKT phase transitions in two-dimensional systems with internal symmetries

Abstract

The Berezinsky-Kosterlitz-Thouless (BKT) type phase transitions in two-dimensional systems with internal abelian continuous symmetries are investigated. The necessary conditions for they can take place are: 1) conformal invariance of the kinetic part of the model action, 2) vacuum manifold must be degenerated with abelian discrete homotopy group pi1. Then topological excitations have a logarithmically divergent energy and they can be described by effective field theories generalizing the two-dimensional euclidean sine-Gordon theory, which is an effective theory of the initial XY-model. In particular, the effective actions for the two-dimensional chiral models on maximal abelian tori TG of simple compact groups G are found. Critical properties of possible effective theories are determined and it is shown that they are characterized by the Coxeter number hG of lattices from the series A,D,E,Z and can be interpreted as those of conformal field theories with integer central charge C=n, where n is a rank of the groups pi1 and G. A possibility of restoration of full symmetry group G in massive phase is also dicussed.

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