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Double-Peak Splitting: The Hidden Structure of Finite-Lattice Phase Transitions in the 3D Ising Model --Verification of the Factor Hierarchy Law on an NP-Complete System: Double-Peak Splitting, Transition Regime, Piecewise Control Function, and Multi-Regime State Decoupling Algorithm

Shuiping Tang

Published Jan 1, 2026• 0 citations
Publisher
DOI
10.2139/ssrn.7196098

Related papers

Double-Peak Splitting: The Hidden Structure of Finite-Lattice Phase Transitions in the 3D Ising Model——Verification of the Factor Hierarchy Law on an NP-Complete System: Double-Peak Splitting, Transition Regime, Piecewise Control Function, and Multi-Regime State

Tang

On the L=64 lattice of the 3D Ising model—an NP-complete problem rigorously proven to have no analytical solution—the six functional dimensions of the Testability Norms were applied, achieving the detection and classification of the ferromagnetic-paramagnetic phase transition with a statistical confidence of p = 3.33×10⁻⁷⁰. Core findings: The Bai-Perron double-break blind test automatically locked T₁ = 4.39 and T₂ = 4.49 (F = 285.7, significantly outperforming the single-break F = 238.3), precisely aligned with the M_sp switch (4.40, F = 1524) and the U₄ switch (4.50, F = 2335), with deviations of 0.01 and 0.01 respectively. This reveals the Double-Peak Splitting of second-order phase transitions on finite lattices—between two sequential regime switches lies an independent Transition Regime (width approximately 0.1), a region commonly dismissed in standard finite-size scaling (FSS) analysis practice as "rounded crossover requiring extrapolation-based elimination," whose boundaries are algorithmically identifiable. The structure was cross-size replicated on the 2D Potts q=4 model: double-break models significantly outperformed single-break models at L = 16, 32, and 64, with the peak separation shrinking from 0.260 at L = 64 to 0.180 at L = 128, evolving according to scaling laws. The traditional gold standard for phase transition detection, magnetic susceptibility χ, fell completely silent under the Chow test (F = 4.8), yet the 1/χ transformation activated it to 324—revealing that the Chow test requires alignment with the correct mathematical structure to capture physical signals. The regime switch temperature in the M_sp dimension remained stable across all lattice sizes (L = 16, 32, 64, 128) at 4.40–4.46, showing no convergence toward the thermodynamic limit Tc = 4.5115 as L increases—pointing to a Precursor Regime Boundary independent of the thermodynamic limit, cross-model replicated in the M_sp dimension of Potts q=4. The first-order transition (Potts q=3) was confirmed as the direction-inverting type (intercept-shift dominated), and the KT transition (XY model) as single-stage continuous crossover—together with the Double-Peak Splitting of second-order transitions, forming a three-category classification framework of the Factor Hierarchy Law. A three-segment piecewise control function constructed from the Bai-Perron double breaks provides, for this NP-complete system, a quantitative description refined directly from data that is functionally equivalent to the Onsager exact solution for the 2D Ising model—requiring no free energy function. The two inflection points of this function were automatically identified by the Bai-Perron algorithm, without relying on any a priori definition of free energy or order parameter, directly demonstrating the capacity of the Testability Norms to extract physical laws from data. Methodological contribution and ultimate asset: This paper distills the entire body of verification into the Multi-Regime State Decoupling Algorithm (MRSD) based on the Factor Hierarchy Law. Its core mathematical logic proceeds in three steps: (1) input any complex high-dimensional dataset; (2) execute the structural optimization operator \left\{T_k\right\}=arg\min_{}{\sum\nolimits^{k+1}_{j=1}{}}\mathrm{RSS}_j(T)+λ⋅k; (3) output a dynamic regime allocation matrix, informing the user at which point the system logic undergoes "rule resetting" and at which point the structure enters "rigid locking." The algorithm has been cross-model verified on the 3D Ising, 2D Potts q=4, and 2D XY models, requiring no free energy function or a priori order parameter definition—only that the data be objective. It redefines finite-size effects from "errors requiring correction" to independent statistical regimes with rigorous boundaries that are algorithmically identifiable, completing the key leap of the information-theoretic duality between the Factor Hierarchy Law and the Ehrenfest classification from analytically solvable systems to systems without analytical solutions. The Testability Norms achieved full verification closure on an NP-complete system across all six functional dimensions. Leave-one-out cross-validation (Tc range [4.47, 4.48], standard deviation 0.0021), Bootstrap threshold regression (95% CI [4.44, 4.48]), and the shrinking external field convergence verification (Tc monotonically shifted from 4.48 to 4.50) jointly confirm the high robustness of the conclusions. Research Paradigm Statement: The core methodology, research direction, and final decisions were independently directed by the author. DeepSeek assisted with code implementation, data presentation, and text drafting. The author takes full academic responsibility for the final content.

•Jul 8, 2026•0 citations

The Reduction of Universality: A Regime Boundary Theory for Finite-System Phase Transitions -Cross-Model Evidence for Bimodal Splitting, the Precursor Regime Boundary, and the Tool-Dependence Theorem

Shuiping Tang

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Phase transition of the Ising model on a fractal lattice

Jozef Genzor, Andrej Gendiar, Tomotoshi Nishino

The phase transition of the Ising model is investigated on a planar lattice that has a fractal structure. On the lattice, the number of bonds that cross the border of a finite area is doubled when the linear size of the area is extended by a factor of 4. The free energy and the spontaneous magnetization of the system are obtained by means of the higher-order tensor renormalization group method. The system exhibits the order-disorder phase transition, where the critical indices are different from those of the square-lattice Ising model. An exponential decay is observed in the density-matrix spectrum even at the critical point. It is possible to interpret that the system is less entangled because of the fractal geometry.

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The phase transition of the two dimensional Ising model according to a Landau theory of phase transition of second order

H. Stenschke

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Shape effects of finite-size scaling functions for anisotropic three-dimensional Ising models

Kazuhisa Kaneda, Yutaka Okabe, Macoto Kikuchi

The finite-size scaling (FSS) functions for anisotropic three-dimensional (3D) Ising models of size L 1 × L 1 × aL 1 ( a : anisotropy parameter) are studied by Monte Carlo simulations. We study the a dependence of FSS functions of the Binder parameter g and the magnetization distribution function p ( m ). We have shown that the FSS functions for p ( m ) at the critical temperature change from a two-peak structure to a single-peak one by increasing or decreasing a from 1. We also study the FSS near the critical temperature of the layered square-lattice Ising model, when the systems have a large two-dimensional (2D) anisotropy. We have found the 3D and 2D FSS behaviour depending on the parameter which is fixed; a unified view of 3D and 2D FSS behaviour has been obtained for the anisotropic 3D Ising models.

arXiv:cond-mat/9909262•Journal of Physics A Mathematical and General•Oct 13, 1999•14 citations

Computational Analysis of 3D Ising Model Using Metropolis Algorithms

Artur Falqueto Sonsin, M R Cortes, D.R.M. Nunes +2 more

We simulate the Ising Model with the Monte Carlo method and use the algorithms of Metropolis to update the distribution of spins. We found that, in the specific case of the three-dimensional Ising Model, methods of Metropolis are efficient. Studying the system near the point of phase transition, we observe that the magnetization goes to zero. In our simulations we analyzed the behavior of the magnetization and magnetic susceptibility to verify the phase transition in a paramagnetic to ferromagnetic material. The behavior of the magnetization and of the magnetic susceptibility as a function of the temperature suggest a phase transition around KT/J ≈ 4.5 and was evidenced the problem of finite size of the lattice to work with large lattice.

Journal of Physics Conference Series•Jul 15, 2015•9 citations
On the L=64 lattice of the 3D Ising model—an NP-complete problem rigorously proven to have no analytical solution—the six functional dimensions of the Testability Norms were applied, achieving the detection and classification of the ferromagnetic-paramagnetic phase transition with a statistical confidence of p = 3.33×10⁻⁷⁰. Core findings: The Bai-Perron double-break blind test automatically locked T₁ = 4.39 and T₂ = 4.49 (F = 285.7, significantly outperforming the single-break F = 238.3), precisely aligned with the M_sp switch (4.40, F = 1524) and the U₄ switch (4.50, F = 2335), with deviations of 0.01 and 0.01 respectively. This reveals the Double-Peak Splitting of second-order phase transitions on finite lattices—between two sequential regime switches lies an independent Transition Regime (width approximately 0.1), a region commonly dismissed in standard finite-size scaling (FSS) analysis practice as "rounded crossover requiring extrapolation-based elimination," whose boundaries are algorithmically identifiable. The structure was cross-size replicated on the 2D Potts q=4 model: double-break models significantly outperformed single-break models at L = 16, 32, and 64, with the peak separation shrinking from 0.260 at L = 64 to 0.180 at L = 128, evolving according to scaling laws. The traditional gold standard for phase transition detection, magnetic susceptibility χ, fell completely silent under the Chow test (F = 4.8), yet the 1/χ transformation activated it to 324—revealing that the Chow test requires alignment with the correct mathematical structure to capture physical signals. The regime switch temperature in the M_sp dimension remained stable across all lattice sizes (L = 16, 32, 64, 128) at 4.40–4.46, showing no convergence toward the thermodynamic limit Tc = 4.5115 as L increases—pointing to a Precursor Regime Boundary independent of the thermodynamic limit, cross-model replicated in the M_sp dimension of Potts q=4. The first-order transition (Potts q=3) was confirmed as the direction-inverting type (intercept-shift dominated), and the KT transition (XY model) as single-stage continuous crossover—together with the Double-Peak Splitting of second-order transitions, forming a three-category classification framework of the Factor Hierarchy Law. A three-segment piecewise control function constructed from the Bai-Perron double breaks provides, for this NP-complete system, a quantitative description refined directly from data that is functionally equivalent to the Onsager exact solution for the 2D Ising model—requiring no free energy function. The two inflection points of this function were automatically identified by the Bai-Perron algorithm, without relying on any a priori definition of free energy or order parameter, directly demonstrating the capacity of the Testability Norms to extract physical laws from data. Methodological contribution and ultimate asset: This paper distills the entire body of verification into the Multi-Regime State Decoupling Algorithm (MRSD) based on the Factor Hierarchy Law. Its core mathematical logic proceeds in three steps: (1) input any complex high-dimensional dataset; (2) execute the structural optimization operator \left\{T_k\right\}=arg\min_{}{\sum\nolimits^{k+1}_{j=1}{}}\mathrm{RSS}_j(T)+λ⋅k; (3) output a dynamic regime allocation matrix, informing the user at which point the system logic undergoes "rule resetting" and at which point the structure enters "rigid locking." The algorithm has been cross-model verified on the 3D Ising, 2D Potts q=4, and 2D XY models, requiring no free energy function or a priori order parameter definition—only that the data be objective. It redefines finite-size effects from "errors requiring correction" to independent statistical regimes with rigorous boundaries that are algorithmically identifiable, completing the key leap of the information-theoretic duality between the Factor Hierarchy Law and the Ehrenfest classification from analytically solvable systems to systems without analytical solutions. The Testability Norms achieved full verification closure on an NP-complete system across all six functional dimensions. Leave-one-out cross-validation (Tc range [4.47, 4.48], standard deviation 0.0021), Bootstrap threshold regression (95% CI [4.44, 4.48]), and the shrinking external field convergence verification (Tc monotonically shifted from 4.48 to 4.50) jointly confirm the high robustness of the conclusions. Research Paradigm Statement: The core methodology, research direction, and final decisions were independently directed by the author. DeepSeek assisted with code implementation, data presentation, and text drafting. The author takes full academic responsibility for the final content.
The phase transition of the Ising model is investigated on a planar lattice that has a fractal structure. On the lattice, the number of bonds that cross the border of a finite area is doubled when the linear size of the area is extended by a factor of 4. The free energy and the spontaneous magnetization of the system are obtained by means of the higher-order tensor renormalization group method. The system exhibits the order-disorder phase transition, where the critical indices are different from those of the square-lattice Ising model. An exponential decay is observed in the density-matrix spectrum even at the critical point. It is possible to interpret that the system is less entangled because of the fractal geometry.
The finite-size scaling (FSS) functions for anisotropic three-dimensional (3D) Ising models of size L 1 × L 1 × aL 1 ( a : anisotropy parameter) are studied by Monte Carlo simulations. We study the a dependence of FSS functions of the Binder parameter g and the magnetization distribution function p ( m ). We have shown that the FSS functions for p ( m ) at the critical temperature change from a two-peak structure to a single-peak one by increasing or decreasing a from 1. We also study the FSS near the critical temperature of the layered square-lattice Ising model, when the systems have a large two-dimensional (2D) anisotropy. We have found the 3D and 2D FSS behaviour depending on the parameter which is fixed; a unified view of 3D and 2D FSS behaviour has been obtained for the anisotropic 3D Ising models.
We simulate the Ising Model with the Monte Carlo method and use the algorithms of Metropolis to update the distribution of spins. We found that, in the specific case of the three-dimensional Ising Model, methods of Metropolis are efficient. Studying the system near the point of phase transition, we observe that the magnetization goes to zero. In our simulations we analyzed the behavior of the magnetization and magnetic susceptibility to verify the phase transition in a paramagnetic to ferromagnetic material. The behavior of the magnetization and of the magnetic susceptibility as a function of the temperature suggest a phase transition around KT/J ≈ 4.5 and was evidenced the problem of finite size of the lattice to work with large lattice.