Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:cond-mat/9811345 · Journal of Statistical Physics

Antiferromagnetic Potts Models on the Square Lattice: A High-Precision Monte Carlo Study

Sabino José Ferreira, Alan D. Sokal

Published Aug 1, 1999• 64 citations
arXivHTMLPDF
DOI
10.1023/a:1004599121565

Related papers

The antiferromagnetic transition for the square-lattice Potts model

Jesper Lykke Jacobsen, Hubert Saleur

arXiv:cond-mat/0512058•Nuclear Physics B•Mar 23, 2006•84 citations

Antiferromagnetic potts models on the square lattice: A high-precision Monte Carlo study

Ferreira, SJ, Alan D. Sokal

study the antiferromagnetic q-state Potts model on the square lattice for q = 3 and q = 4, using the Wang-Swendsen-Kotecky (WSK) Monte Carlo algorithm and a powerful finite-size-scaling extrapolation method. For q=3 we obtain good control up to correlation length xi similar to 5000; the data are consistent with xi(B)=Ae(2 beta)beta(P)(1 + a(1)e(-beta) + ...) as beta--> infinity, with p approximate to 1. The staggered susceptibility behaves as chi(stagg) similar to xi(5/3). For q = 4 the model is disordered (xi less than or similar to 2) even at zero temperature. In appendices we prove a correlation inequality for Potts antiferromagnets on a bipartite lattice, and we prove ergodicity of the WSK algorithm at zero temperature for Potts antiferromagnets on a bipartite lattice.

•Aug 1, 1999•33 citations

Monte-Carlo Simulations of High-q Anti-ferromagnetic Potts Models

Shafiqur M. Rahman, Suvarshi Bhadra, Joshua D. Monk

Bulletin of the American Physical Society•Mar 8, 2007•0 citations

Monte Carlo renormalization-group analysis of the antiferromagnetic three-state Potts model on a square lattice

Ciriyam Jayaprakash, Jan Tobochnik

Monte Carlo renormalization-group calculations have been performed on the three-state anti-ferromagnetic Potts model on a square lattice. The results are consistent with the conclusion that there is no transition as a function of temperature.

Physical review. B, Condensed matter•Apr 1, 1982•26 citations

Field Theory of Scaling Lattice Models: The Potts Antiferromagnet

Gesualdo Delfino A

arXiv:hep-th/0110181•Springer eBooks•Jan 1, 2002•5 citations

Monte Carlo Study of the Antiferromagnetic Potts Model in Two Dimensions

Gary S. Grest, Jayanth R. Banavar

Results of Monte Carlo studies of the $q$-state Potts model on a square lattice with antiferromagnetic nearest-neighbor coupling and ferromagnetic next-nearest-neighbor coupling are presented for $q>~3$. The three-state Potts model shows a variety of unusual transitions whereas for $q>~4$, we find two first-order phase transitions separated by a broken sublattice symmetry state.

Physical Review Letters•Jun 1, 1981•52 citations
study the antiferromagnetic q-state Potts model on the square lattice for q = 3 and q = 4, using the Wang-Swendsen-Kotecky (WSK) Monte Carlo algorithm and a powerful finite-size-scaling extrapolation method. For q=3 we obtain good control up to correlation length xi similar to 5000; the data are consistent with xi(B)=Ae(2 beta)beta(P)(1 + a(1)e(-beta) + ...) as beta--> infinity, with p approximate to 1. The staggered susceptibility behaves as chi(stagg) similar to xi(5/3). For q = 4 the model is disordered (xi less than or similar to 2) even at zero temperature. In appendices we prove a correlation inequality for Potts antiferromagnets on a bipartite lattice, and we prove ergodicity of the WSK algorithm at zero temperature for Potts antiferromagnets on a bipartite lattice.
Results of Monte Carlo studies of the qqq-state Potts model on a square lattice with antiferromagnetic nearest-neighbor coupling and ferromagnetic next-nearest-neighbor coupling are presented for q> 3q>~3q> 3. The three-state Potts model shows a variety of unusual transitions whereas for q> 4q>~4q> 4, we find two first-order phase transitions separated by a broken sublattice symmetry state.