A constrained Potts antiferromagnet model with an interface representation

We define a 4-state Potts model ensemble on the square lattice, with the constraints that neighbouring spins must have different values, and that no plaquette may contain all four states. The spin configurations may be mapped into those of a two-dimensional interface in a 2 + 5 dimensional space. If this interface is in a Gaussian rough phase (as is the case for most other models with such a mapping) then the spin correlations are critical and their exponents can be related to the stiffness governing the interface fluctuations. Results of our Monte Carlo simulations show height fluctuations with an anomalous dependence on the wavevector, intermediate between the behaviours expected in a rough and in a smooth phase; we argue that the smooth phase (which would imply long-range spin order) is the best interpretation.

[1]  Lipowski,et al.  Critical behavior of spin S antiferromagnetic ising model on triangular lattice. , 1995, Physical Review Letters.

[2]  Stochastic cluster algorithms for discrete gaussian (SOS) models , 1991 .

[3]  David P. Landau,et al.  Phase transitions and critical phenomena , 1989, Computing in Science & Engineering.

[4]  Hasenbusch,et al.  Cluster algorithm for a solid-on-solid model with constraints. , 1992, Physical review. B, Condensed matter.

[5]  Levitov Equivalence of the dimer resonating-valence-bond problem to the quantum roughening problem. , 1990, Physical review letters.

[6]  J. Kolafa,et al.  Monte Carlo study of the three-state square Potts antiferromagnet , 1984 .

[7]  J. Banavar,et al.  Ordering and Phase Transitions in Antiferromagnetic Potts Models , 1980 .

[8]  Huse,et al.  Classical antiferromagnets on the Kagomé lattice. , 1992, Physical review. B, Condensed matter.

[9]  J. Banavar,et al.  Monte Carlo Study of the Antiferromagnetic Potts Model in Two Dimensions , 1981 .

[10]  Henley,et al.  Geometrical exponents of contour loops on random Gaussian surfaces. , 1995, Physical review letters.

[11]  Henk W. J. Blöte,et al.  Triangular SOS models and cubic-crystal shapes , 1984 .

[12]  Sokal,et al.  Comment on "Antiferromagnetic Potts models" , 1993, Physical review letters.

[13]  Wang,et al.  Three-state antiferromagnetic Potts models: A Monte Carlo study. , 1990, Physical review. B, Condensed matter.

[14]  Exact results on the antiferromagnetic three-state Potts model. , 1989, Physical review letters.

[15]  Antiferromagnetic Potts models on the square lattice. , 1994, Physical review. B, Condensed matter.

[16]  H. Blote,et al.  Roughening transitions and the zero-temperature triangular Ising antiferromagnet , 1982 .

[17]  H. Beijeren,et al.  Exactly solvable model for the roughening transition of a crystal surface , 1977 .

[18]  H. S. M. Coxeter On Laves' Graph Of Girth Ten , 1955 .

[19]  C. L. Henley,et al.  New two-color dimer models with critical ground states , 1997 .

[20]  Wang,et al.  Antiferromagnetic Potts models. , 1989, Physical review letters.

[21]  M. Nijs,et al.  Critical fan in the antiferromagnetic three-state Potts model , 1982 .

[22]  Jorge V. José,et al.  Renormalization, vortices, and symmetry-breaking perturbations in the two-dimensional planar model , 1977 .

[23]  Zheng,et al.  Sine-Gordon theory of the non-Néel phase of two-dimensional quantum antiferromagnets. , 1989, Physical review. B, Condensed matter.

[24]  Henley,et al.  Four-coloring model on the square lattice: A critical ground state. , 1995, Physical review. B, Condensed matter.

[25]  G. Wannier,et al.  Antiferromagnetism. The Triangular Ising Net , 1950 .

[26]  Michael E. Fisher,et al.  Statistical Mechanics of Dimers on a Plane Lattice. II. Dimer Correlations and Monomers , 1963 .

[27]  TheXY model and the three-state antiferromagnetic Potts model in three dimensions: Critical properties from fluctuating boundary conditions , 1994, cond-mat/9406092.

[28]  B. Nienhuis CRITICAL SPIN-1 VERTEX MODELS AND O(n) MODELS , 1990 .

[29]  Kac-Moody symmetries of critical ground states , 1995, cond-mat/9511102.