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Chinese Physics B

Third-order transitions in Ising and Potts models on Watts–Strogatz small-world networks

Fangfang Wang, Wei Liu, Ke Zhang, Yongjian He, Kai Qi, Yi Tang, Zengru Di

Published Apr 29, 2026• 0 citations
Publisher

Abstract

Abstract We study third-order transitions in the Ising and Potts models on regular two-dimensional lattices and on Watts—Strogatz small-world networks. Cluster observables are used to track post-critical boundary reorganization and pre-critical cluster breakup. For the Ising model, the critical temperature $T_c$ is calibrated independently from Binder-cumulant crossings and susceptibility peaks, whereas for the Potts model on small-world networks it is identified operationally from the dominant critical peak of $\mathrm d\langle P\rangle/\mathrm dT$ and independently checked against the specific-heat peak. The independent and dependent third-order transitions are identified from the isolated-spin peak and the post-critical structural extremum, respectively. For both lattice and small-world topologies, we find the robust ordering $T_{\mathrm{ind}}<T_c<T_{\mathrm{dep}}$. Increasing the rewiring probability shifts all three characteristic temperatures upward and enhances the visibility of the post-critical transition. The effect is especially clear in the Potts model, where perimeter-based observables are more sensitive to multistate boundary fluctuations. The systematic persistence of the characteristic temperature hierarchy across topologies and finite sizes argues against interpreting these features as incidental finite-size irregularities. Instead, our results support their interpretation as robust third-order precursor transitions whose structural detectability can be amplified by network topology.

DOI
10.1088/1674-1056/ae6639

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Abstract We study third-order transitions in the Ising and Potts models on regular two-dimensional lattices and on Watts—Strogatz small-world networks. Cluster observables are used to track post-critical boundary reorganization and pre-critical cluster breakup. For the Ising model, the critical temperature TcT_cTc​ is calibrated independently from Binder-cumulant crossings and susceptibility peaks, whereas for the Potts model on small-world networks it is identified operationally from the dominant critical peak of d⟨P⟩/dT\mathrm d\langle P\rangle/\mathrm dTd⟨P⟩/dT and independently checked against the specific-heat peak. The independent and dependent third-order transitions are identified from the isolated-spin peak and the post-critical structural extremum, respectively. For both lattice and small-world topologies, we find the robust ordering Tind<Tc<TdepT_{\mathrm{ind}}<T_c<T_{\mathrm{dep}}Tind​<Tc​<Tdep​. Increasing the rewiring probability shifts all three characteristic temperatures upward and enhances the visibility of the post-critical transition. The effect is especially clear in the Potts model, where perimeter-based observables are more sensitive to multistate boundary fluctuations. The systematic persistence of the characteristic temperature hierarchy across topologies and finite sizes argues against interpreting these features as incidental finite-size irregularities. Instead, our results support their interpretation as robust third-order precursor transitions whose structural detectability can be amplified by network topology.
Third-order pseudo-transitions in finite systems reflect reorganization beyond conventional criticality, yet their identification usually relies on microcanonical entropy, which is often inaccessible in practice. Here we introduce a spectral generalized response within the eigen-microstate framework. From the distribution of normalized spectral weights, we construct the third-order ratio R3=K3/(K2)3R_3=K_3/(K_2)^3R3​=K3​/(K2​)3, which probes asymmetric redistribution among fluctuation modes beyond leading-mode condensation. Across Ising and Potts models on regular lattices and random regular networks, extrema of R3R_3R3​ consistently track higher-order anomalies. Combined with spectral projection, the method further distinguishes dependent and independent branches: the former remain tied to the dominant ordering channel, whereas the latter arise from redistribution within the subleading fluctuation subspace. The effective spectral dimension ReffR_{\mathrm{eff}}Reff​ provides the participation background in which these anomalies develop. These results establish a geometric characterization of third-order pseudo-transitions as reorganizations of statistical weight in configuration space and provide an order-parameter-free route to finite-size structural criticality.
Within the canonical ensemble framework, this paper investigates the presence of higher-order transition signals in the q-state Potts model (for q≥3), using two geometric order parameters: isolated spins number and the average perimeter of clusters. Our results confirm that higher-order transitions exist in the Potts model, where the number of isolated spins reliably indicates third-order independent transitions. This signal persists regardless of the system's phase transition order, even at higher values of q. In contrast, the average perimeter of clusters, used as an order parameter for detecting third-order dependent transitions, shows that for q=6 and 8, the signal for third-order dependent transitions disappears, indicating its absence in systems undergoing first-order transitions. These findings are consistent with results from microcanonical inflection-point analysis, further validating the robustness of this approach.
We study the Ising phase transition on a three-dimensional cubic lattice augmented with sparse, distance-dependent shortcuts whose density decays as P(r) proportional to r^(-2). This network ensemble, characterized by geometric embedding, sparse additive quenched shortcuts, and power-law distance dependence, falls outside the scope of existing results for both uniform small-world networks (Barrat-Weigt, Herrero) and dense long-range Ising models (Fisher-Ma-Nickel, Sak). We present partial analytical results. The effective propagator exhibits three regimes: a Wilson-Fisher intermediate regime (standard Laplacian dominant), a Levy IR regime (wormhole term dominant), and a biharmonic UV regime, with propagator crossover at approximately 125 lattice units. A scaling estimate suggests the nonlocal operator is only marginally relevant at Wilson-Fisher, implying a potentially very slow RG flow. A mean free path analysis yields a finite effective signal velocity of approximately 2.4 times the local propagation speed, with the exponent alpha = 2 lying at the apparent boundary for finite-speed propagation on sparse shortcut networks. We propose a concrete Monte Carlo simulation protocol (approximately 500 CPU-hours) using Wolff cluster algorithm and finite-size scaling with Binder cumulant analysis to definitively determine the universality class. The key observable is U4*, which unambiguously distinguishes 3D Ising (U4* approximately 0.61) from mean-field (U4* approximately 0.47) universality. Control simulations on pure 3D lattice and uniform shortcut networks are specified. The problem is relevant to discrete quantum gravity models with holographic connectivity, network science, and the theory of phase transitions on complex geometries. All analytical results are clearly labeled as scaling estimates or conjectures where appropriate, and five explicit unresolved issues are identified.
The phase transitions in 2D ferro- and antiferromagnetic Potts models with number of spin states q = 3 on a triangular lattice are investigated by the cluster and classical Monte Carlo methods. Systems with linear sizes L = 20–120 are considered. Fourth-order Binder cumulants and histogram data analysis are used to show that second- and first-order phase transitions are observed in the ferromagnetic and antiferromagnetic Potts models, respectively. The static critical indices are calculated for specific heat α, susceptibility γ, magnetization β, and correlation length ν on the basis of finite-size scaling theory for a ferromagnetic Potts model.
We employ the microcanonical inflection-point analysis method, developed for the systematic identification and classification of phase transitions in systems of any size, to study the two-dimensional Ising model at various lattice sizes and in the thermodynamic limit. Exact results for the density of states, which were obtained by exact algorithmic computation, provide evidence for higher-order transitions in addition to the well-studied second-order ferromagnetic-paramagnetic phase transition. An independent third-order phase transition is identified in the ferromagnetic phase, whereas another third-order transition resides in the paramagnetic phase. The latter is a dependent transition, i.e., it is inevitably associated with the critical transition, but it remains separate from the critical point in the thermodynamic limit. For a deeper insight into the nature of these additional transitions, a detailed analysis of spin clusters is performed.
The phase transitions in the two-dimensional ferro- and antiferromagnetic Potts models with q = 3 states of spin on a triangular lattice are studied using cluster algorithms and the classical Monte Carlo method. Systems with linear sizes L = 20–120 are considered. The method of fourth-order Binder cumulants and histogram analysis are used to discover that a second-order phase transition occurs in the ferromagnetic Potts model and a first-order phase transition takes place in the antiferromagnetic Potts model. The static critical indices of heat capacity (α), magnetic susceptibility (γ), magnetization (β), and correlation radius index (ν) are calculated for the ferromagnetic Potts model using the finite-size scaling theory.