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

Physica A Statistical Mechanics and its Applications

Critical properties of the three-state Potts model on two-dimensional lattices: A finite-size scaling study

Muhammet Arucu

Published Oct 1, 2026• 0 citations
Publisher
DOI
10.1016/j.physa.2026.132160

Related papers

Critical Behaviour of the Two-Dimensional Potts Model with a Continuous Number of States; A Finite Size Scaling Analysis

Henk W. J. Blöte, M. P. Nightingale

Current physics sources and comments•Jan 1, 1988•0 citations

Critical behaviour of the two-dimensional Potts model with a continuous number of states; A finite size scaling analysis

Henk W. J. Blöte, M. P. Nightingale

Physica A Statistical Mechanics and its Applications•Jun 1, 1982•277 citations

Finite-size scaling of the three-state Potts model on a simple cubic lattice

M. Fukugita, H. Mino, Masanori Okawa +1 more

Journal of Statistical Physics•Jun 1, 1990•39 citations

Critical relaxation of the two-dimensional three-state Potts model with conserved dynamics

M. Aydin, M. Cemal Yalabık

The dynamical critical exponent z is obtained using the finite-size scaling method for the two-dimensional three-state Potts model with conserved dynamics. It is observed that there is a change in the dynamical behaviour of the system at the size n=15. For finite lattices of sizes n<or=15, the value of z is predicted as z=2.0+or-0.1. For n>or=15, the asymptotic behaviour is observed and z is calculated as z=2.78+or-0.20.

Journal of Physics A Mathematical and General•Feb 7, 1988•4 citations

Dynamical critical properties of the random-bond three-state Potts model

Anonymous, Ulvi Kanbur, Mohammad Sadra Najafi +2 more

We study the dynamic critical behavior of the two-dimensional random-bond three-state Potts model using large-scale Monte Carlo simulations with the Wolff and Swendsen-Wang cluster algorithms. At the disorder-dependent critical temperature, we compute integrated and exponential autocorrelation times and extract the dynamic critical exponent z via finite-size scaling. Critical slowing down is significantly weakened by bond randomness, with the dynamic exponent decreasing from z≈0.54 in the pure system to z≈0.24 at strong disorder. From the finite-size scaling of the Wolff cluster size, we obtain γ/ν≈1.73, where γ and ν are the susceptibility and correlation-length exponents, respectively, consistent with the universality class of the two-dimensional three-state Potts model. These results indicate that bond randomness strongly affects the critical dynamics but leaves the underlying static universality class unchanged. Furthermore, both static and dynamic observables, including the specific heat and the autocorrelation times, show a lack of self-averaging.

arXiv:2610.01176•Physical review. E•Aug 13, 2026•0 citations

Effective-Geometry Rescaling and Universal Critical Behavior in the Anisotropic Three-State Potts Model on the Square Lattice

Fan Yang, Jian Gao, Lu Liu +1 more

We study the two-dimensional anisotropic three-state Potts ferromagnet on the square lattice using Wolff single-cluster Monte Carlo simulations and finite-size scaling. For coupling ratios $λ=J_y/J_x=0.5$, $0.75$, and $1$, finite-size scaling of the correlation ratio yields critical behavior consistent with the two-dimensional three-state Potts universality class. The scaling of the leading Fisher zeros gives a correlation-length exponent consistent with $ν=5/6$, while their cumulative density is consistent with the expected specific-heat exponent $α=1/3$. We further characterize the anisotropy at criticality using directional correlation ratios $R_x$ and $R_y$ together with directional FK wrapping probabilities. For $λ=0.5$ on a physically square lattice, $R_x$ and $R_y$ approach distinct critical values while yielding a common correlation-length exponent. From the wrapping probabilities, we independently determine an effective aspect ratio $ρ_e^\square=0.6413(5)$, in close agreement with the theoretical value $ρ_e^{\square,\mathrm{th}}\simeq0.64150030$ obtained from the isoradial representation. Using the theoretical value to set the physical aspect ratio restores directional equivalence, $R_x\simeq R_y$, and brings the overall correlation ratio toward the isotropic-square reference. The results show that spatial anisotropy changes the effective critical geometry without altering the bulk three-state Potts universality class.

arXiv:2610.10467•Oct 7, 2026•0 citations
We study the dynamic critical behavior of the two-dimensional random-bond three-state Potts model using large-scale Monte Carlo simulations with the Wolff and Swendsen-Wang cluster algorithms. At the disorder-dependent critical temperature, we compute integrated and exponential autocorrelation times and extract the dynamic critical exponent z via finite-size scaling. Critical slowing down is significantly weakened by bond randomness, with the dynamic exponent decreasing from z≈0.54 in the pure system to z≈0.24 at strong disorder. From the finite-size scaling of the Wolff cluster size, we obtain γ/ν≈1.73, where γ and ν are the susceptibility and correlation-length exponents, respectively, consistent with the universality class of the two-dimensional three-state Potts model. These results indicate that bond randomness strongly affects the critical dynamics but leaves the underlying static universality class unchanged. Furthermore, both static and dynamic observables, including the specific heat and the autocorrelation times, show a lack of self-averaging.
We study the two-dimensional anisotropic three-state Potts ferromagnet on the square lattice using Wolff single-cluster Monte Carlo simulations and finite-size scaling. For coupling ratios λ=Jy/Jx=0.5λ=J_y/J_x=0.5λ=Jy​/Jx​=0.5, 0.750.750.75, and 111, finite-size scaling of the correlation ratio yields critical behavior consistent with the two-dimensional three-state Potts universality class. The scaling of the leading Fisher zeros gives a correlation-length exponent consistent with ν=5/6ν=5/6ν=5/6, while their cumulative density is consistent with the expected specific-heat exponent α=1/3α=1/3α=1/3. We further characterize the anisotropy at criticality using directional correlation ratios RxR_xRx​ and RyR_yRy​ together with directional FK wrapping probabilities. For λ=0.5λ=0.5λ=0.5 on a physically square lattice, RxR_xRx​ and RyR_yRy​ approach distinct critical values while yielding a common correlation-length exponent. From the wrapping probabilities, we independently determine an effective aspect ratio ρe□=0.6413(5)ρ_e^\square=0.6413(5)ρe□​=0.6413(5), in close agreement with the theoretical value ρe□,th≃0.64150030ρ_e^{\square,\mathrm{th}}\simeq0.64150030ρe□,th​≃0.64150030 obtained from the isoradial representation. Using the theoretical value to set the physical aspect ratio restores directional equivalence, Rx≃RyR_x\simeq R_yRx​≃Ry​, and brings the overall correlation ratio toward the isotropic-square reference. The results show that spatial anisotropy changes the effective critical geometry without altering the bulk three-state Potts universality class.