SciPost Submission Page
Theory of Order-Disorder Phase Transitions Induced by Fluctuations Based on Network Models
by Yonglong Ding
Submission summary
Authors (as registered SciPost users): | Yonglong Ding |
Submission information | |
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Preprint Link: | https://arxiv.org/abs/2501.07092v1 (pdf) |
Date submitted: | 2025-01-31 12:57 |
Submitted by: | Ding, Yonglong |
Submitted to: | SciPost Physics |
Ontological classification | |
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Academic field: | Physics |
Specialties: |
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Approaches: | Theoretical, Computational |
Abstract
Both quantum phase transitions and thermodynamic phase transitions are probably induced by fluctuations, yet the specific mechanism through which fluctuations cause phase transitions remains unclear in existing theories. This paper summarizes different phases into combinations of three types of network structures based on lattice models transformed into network models and the principle of maximum entropy. These three network structures correspond to ordered, boundary, and disordered conditions, respectively. By utilizing the transformation relationships satisfied by these three network structures and classical probability, this work derive the high-order detailed balance relationships satisfied by strongly correlated systems. Using the high-order detailed balance formula, this work obtain the weights of the maximum entropy network structures in general cases. Consequently, I clearly describe the process of ordered-disordered phase transitions based on fluctuations and provide critical exponents and phase transition points. Finally, I verify this theory using the Ising model in different dimensions, the frustration scenario of the triangular lattice antiferromagnetic Ising model, and the expectation of ground-state energy in the two-dimensional Edwards-Anderson model.
Author indications on fulfilling journal expectations
- Provide a novel and synergetic link between different research areas.
- Open a new pathway in an existing or a new research direction, with clear potential for multi-pronged follow-up work
- Detail a groundbreaking theoretical/experimental/computational discovery
- Present a breakthrough on a previously-identified and long-standing research stumbling block
Current status:
Reports on this Submission
Strengths
I do not see any strength
Weaknesses
1) the presentation of the methodology is absolutely obscure
2) the presentation of the results is confused and confusing
3) the results seem not be in line with recent literature on the 3D ising model
4) recent literature on the subject is not discussed
Report
The author aims to develop a methodology to transform lattice models
in networks models for the ferromagnetic Ising model, the antiferromagnetic
Ising model and the two-dimensional Edwards-Anderson model. Then he plans
to apply the maximum entropy priciple to obtain the most random structure and from these he seems able to derive critical exponent beta, at least for the Ising model in 2, 3, 4, and 5 dimensions.
1) For me the transformation from infinite lattice model to network model
is unclear.
The following sentence is obscure for various reasons :
"Firstly, all possible
lattice sites in the lattice model are classified according
to the magnitude of their interactions and the spin of the
lattice sites themselves. Let Cij represent the weights of
different types of lattice sites, where i denotes the spin
type of the lattice site itself, and j represents different
types of neighbor interactions. Then, different Cij val-
ues are treated as different network nodes. If there exists
a transformation relationship between different network
nodes caused by fluctuations, the two network nodes are
connected by a line segment. Finally, the different phases
of the lattice model are labeled using the weights of differ-
ent network nodes. If all lattice sites have spins pointing
upwards, the weight of the corresponding network node
is set to 1, while the weights of other network nodes are
set to 0. This method does not focus on the specific po-
sition and momentum of any individual lattice site, but
rather on the weights of different types of lattice sites.
In other words, it attempts to capture the core physical
information by using the weights and changes of different
types of lattice sites."
here a series of doubts :
1i) when the author writes :
"lattice sites in the lattice model are classified according
to the magnitude of their interactions and the spin of the
lattice sites themselves."
I guess that the author means "lattice sites are classified accordingly to the
value of the spin variable occupying the considered lattice site
and the value of the spins in the neighbouring lattices and of the
values of their interactions" . However, I do not think there
is an univoque mapping in such a case. I do not think a
bi-univocal transformation can be constructed between a lattice and C_ij.
1ii) This sentence is absolutely obscure :
" If there exists
a transformation relationship between different network
nodes caused by fluctuations, the two network nodes are
connected by a line segment."
probably it means that depending on the temperature, if the energy
allows for a flipping of two neighbours, then there is a connection
among them ?
2) The author should present in a simple case (Ising model ?) the transformations
he has in mind to pass from lattice to network, step by step.
3) I do not understand large part of what written by the author neither
his logic, however Eq (12) I guess is the magnetization per spin as a function of temperature
in a Ising Model (by the way the temperature T has been not introuced as well as the magnetization m ),
for 2 dimensions the solution of this problem has been found by Onsager :
<m> = [ 1 - 1/sinh(2J/KbT)^4]^1/8
this would mean that in 2 dimensions, by assuming J/Kb =1, from eq 12 one gets
the 2 dimensional results for n=4 and k=2, why ? What does it mean ?
4) Furthermore, for what I understand from Eq (12) and Fig 2 the author has analytically solved the problem of Ising in 3, 4 , and 5 dimensions, and found the corresponding critical exponent beta, at least for the magnetization at the critical point.
As far as I know the Ising model in 3d has not yet been solved, see
Ferrenberg, Alan M., Jiahao Xu, and David P. Landau. "Pushing the limits of Monte Carlo simulations for the three-dimensional Ising model."
Physical Review E 97.4 (2018): 043301.
and also more recently :
Liu, Zihua, et al. "Critical dynamical behavior of the Ising model." Physical Review E 108.3 (2023): 034118.
How the results of the author do relate to the above literature ?
4) From wikipedia the best estimation (numerical) of the Beta exponent
for the 3D Ising model is 0.32641871(75) and not 1/3 as reported by the authors.
In summary the paper is extremely confused, the method is not clearly exposed,
and the results found at least for the 3D Ising model are not in line with the recent
literature on the subject. I suggest not to publish this manuscript .
Recommendation
Reject
Report
Although by dealing with lattice models in low dimensions the manuscript falls slightly outside my expertise, I decided to submit the following comments which explain why I think the manuscript is not ready for consideration in SciPost Physics.
- The description of the novel method is very unclear and the arguments often did not make sense to me. If this method works then at least it is not explained well.
- The method is heuristic and it remained unclear what its limitations are.
- There appears to be significant overlap of the Ising model discussion with the results of the author's previous publication in AIP advances 14, 085308 (2024).
- The results, also for the two other models in the appendix, are not compared against existing values in the literature. No side-by side comparison to an existing method is made.
- Concerning the journal acceptance criteria: I did not see why the presented approach would constitute a breakthrough or detail a groundbreaking discovery. To my understanding, fluctuations are not taken into account in basic Landau theory but a large literature exists on extensions to fluctuations and other methods. So the motivation given in the manuscript, that the role of fluctuations in phase transitions would be unclear, appears not justified.
- However, maybe the "opens a new pathway [...] with clear potential for multi-pronged follow-up work" condition may be fulfilled, if the method was more clearly presented and discussed in the light of related literature.
Given these fundamental issues of presentation, I think that the submission currently cannot be constructively considered for the selective SciPost Physics, and aside from my mismatch in specific expertise this is why I did not review in full depth.
A major revision of the manuscript appears necessary before (possibly) resubmitting for more detailed review.
Recommendation
Reject
Author: Yonglong Ding on 2025-03-21 [id 5304]
(in reply to Report 1 on 2025-03-17)I sincerely thank you for reviewing my manuscript and identifying its shortcomings. To address these deficiencies, I have developed a systematic revision strategy structured as follows:
deliberately avoiding speculative assumptions throughout the analysis. Limitation Disclosure: I comprehensively supplemented the discussion to clarify methodological constraints and potential biases inherent in the proposed approach. Contextual Differentiation: I clarified that my previously published work constituted one specific validation case among three experimental benchmarks demonstrated in this study. This manuscript ascends to generalizable principles, particularly focusing on the application of high-order detailed balance theory to describe lattice model phase transitions between order and disorder. Notably, the analytical frameworks and result derivation approaches employed in these two studies demonstrate fundamental differences. Comparative Enhancement: To address the identified lack of comparative analysis, I systematically expanded the evidence base through extensive literature review and comparative experimentation. Benchmarking and Future Directions: The revised manuscript includes comprehensive comparisons with existing methodologies, followed by five distinct research avenues with significant potential for follow-up investigations.
-.The description of the novel method is very unclear and the arguments often did not make sense to me. If this method works then at least it is not explained well.
The following sections detail the network model construction through concrete examples and schematic illustrations.
Network Model Construction
Example: 2D Ising Model with Nearest-Neighbor Interactions Consider a 2D Ising model where each lattice site exhibits spin-up/down states. Sites are classified based on their own spin state and the number of nearest-neighbor sites (4 neighbors) sharing the same spin: Spin-up classification: 5 categories (0-4 matching neighbors) Spin-down classification: 5 categories (0-4 matching neighbors) This results in 10 distinct classes (C₁₅-C₂₅). Mathematically, for the Hamiltonian H=1/2∑<i,j> Si Sj, I reorganize terms by these classes. The factor of 1/2 accounts for double-counting interactions. Importantly, this classification covers all possible configurations in the infinite 2D Ising model through 10 network nodes, where node weights represent configuration probabilities.
State Transitions and Network Dynamics Case 1: Spin Flip of Central Site
Initial State: Central site has spin-up with 4 matching neighbors (Class C₁₅). Active Transformation: Flipping the central site changes its state to spin-down with 0 matches (Class C₂₁). Passive Transformation: This flip simultaneously alters neighboring sites' classes from C₁₅ → C₁₄ (each neighbor loses one match). Case 2: Neighbor Spin Flip
Initial State: Central site remains spin-up with 4 matches (C₁₅). Passive Transformation: Flipping a neighboring site reduces its match count to 3 (Class C₁₄ for the neighbor), indirectly modifying the central site's class to C₁₄. These two cases illustrate all possible transformations under nearest-neighbor interactions. The complete network structure emerges from considering all such transitions.
Network Node Labeling Convention Nodes are labeled Cij : i∈{1,2}: Spin state (1=up, 2=down) j∈{1,5}: Number of matching neighbors (1=0 matches, 5=4 matches) Example: C₁₅: Spin-up with 4 matches C₁₃: Spin-down with 2 matches
Generalization to Higher Dimensions 3D Ising Model: Classifies sites into 14 nodes (7 match counts × 2 spins) N-dimensional Models: Follows similar classification logic with 2(N+1) nodes This framework applies to various lattice models through analogous interaction-based classifications. Active vs. Passive Transformations
Transformation Type Definition Network Impact
Active Direct spin flip of target site Horizontal transition between nodes Passive Indirect flip via neighbor changes Vertical transition within nodes
Key Insight: A single active transformation (e.g., flipping site A) corresponds to four simultaneous passive transformations (its four neighbors' state changes). Deriving High-Order Detailed Balance Unlike Monte Carlo simulations that use active transformations, this work focuses on passive transformations to establish:
Microstate Transition Probabilities: Calculate joint probabilities for four-site passive transformations Balance Equations: Derive relationships between node weights during phase transitions
Phase Transition Analysis Using Waterfall Metaphor
This demonstrates how passive transformations effectively capture critical transition dynamics missed by traditional active-only approaches.
-. The method is heuristic and it remained unclear what its limitations are.
Network Model Transformation I systematically convert lattice models into network representations to study phase transitions. This transformation process adheres to strict mathematical rigor:
Single-node structures: Correspond to 0 K ground states Boundary structures: Intermediate configurations during phase transitions Maximum entropy structures: Represent disordered states post-transition
Thermodynamic Interpretation
(Note: Potential fractal connections remain unexplored in this work)
Special Case Analysis: 1D Ising Model The strictly converted network model for 1D Ising system: Lacks boundary structures Explains absence of phase transitions Maintains consistency with theoretical predictions
Methodological Advantages No algorithmic rules or additional assumptions introduced Focus on macroscopic phenomenon generation mechanisms Avoids conventional phase transition parameter calculations (e.g., critical exponents)
Limitations and Challenges 1)Complex Interactions Handling: Multiple spin interactions (aligning/opposing) in Ising model increase node complexity Systems with multi-spin orientations lead to exponential growth of network nodes 2)Mathematical Rigor Constraints: Angular interaction calculations (e.g., spin deflection angles) result in infinitely large network models No general solution exists for continuous interaction spectra
-. There appears to be significant overlap of the Ising model discussion with the results of the author's previous publication in AIP advances 14, 085308 (2024).
Theoretical Framework and Validation This work derives a general phase transition formula based on high-order detailed balance principles. Three specific experimental benchmarks validate this formulation: 1)Ising model in different dimensions (overlapping with AIP Advances 14, 085308 (2024)) 2)Frustrated triangular Ising model 3)Edwards-Anderson Model Comparison with AIP Advances 14, 085308 (2024)
The referenced study focuses on: Constructing network models for 2D/3D/ND Ising systems Performing dimension-specific analyses Deriving phase transition formulas through case-by-case treatments No application of high-order detailed balance principles No general lattice model framework
Methodological Differentiation Feature Present Work AIP Advances 14, 085308 (2024) Core Objective General lattice model phase equations Dimension-specific Ising system analysis Theoretical Foundation High-order detailed balance Empirical case studies Applicability Universal lattice models Restricted to Ising families Derivation Approach Abstract generalization Case-specific parameterization Innovation and Progression
1)Generalization from Specific Cases: Previous works analyzed particular instances (e.g., 2D Ising) This research establishes universal phase transition equations applicable to any lattice model
2)Theoretical Unification:
Derives general formula → Specializes for Ising models through variable substitution Contrasts with the referenced study's dimension-specific derivations
3)Methodological Advancement:
Utilizes high-order detailed balance for analytical solutions Avoids empirical fitting procedures used in AIP Advances approach Validation Strategy Dimensional Consistency Check: Validates formula predictions across 2D/3D/ND systems Network Model Cross-Validation: Compares analytical results with network-based simulations Critical Exponent Comparison: Demonstrates agreement with known thermodynamic limits
-. The results, also for the two other models in the appendix, are not compared against existing values in the literature. No side-by side comparison to an existing method is made.
Validation Results Across Dimensional Ising Models The phase transition formulas derived in this work have been validated through three-dimensional lattice systems: 1) 2D Ising Model: Achieves quantitative agreement with the analytical solutions by Yang-Zheng and Onsager (Physical Review 85, 808 (1952)).
2)3D Ising Model: No analytical solution exists; comparison with Monte Carlo simulations shows: Phase transition temperature difference: 0.7%(established theoretically in Physical Review B 62, 14837 (2000)) Critical exponent deviation: 1/3 Note: Monte Carlo results remain empirical references due to lack of analytical benchmarks. 2)≥4D Ising Models: Confirms critical exponent α = 1/2 , matching our general formula predictions.
Appendix A: Frustrated triangular Ising model For systems with spin restricted to z-direction (±1), I prove: Existence of Minimum Energy Configuration: Total energy Etotal≥N⋅Emin, where N = total lattice sites. Achievability: Configurations with all spins aligned (either all +1 or all -1) realize this minimum. Formula Derivation: All results strictly follow from the phase transition equations proposed in this work.
Appendix B: Edwards-Anderson Model Validation W. F. Wreszinski's 2012 ground-state calculation for the 2D Edwards-Anderson model (with double-peaked distribution): Experimental Result: Egs=−1.5 (Journal of Statistical Physics 146, 118 (2012)) Theoretical Prediction: This formula yields identical result through parameter substitution.
Methodological Distinction This work does not employ numerical simulation algorithms but instead: Proposes a universal phase transition formula eq 10 Derives specific results through dimensional parameterization Focuses on analytical derivations rather than empirical validation
-. Concerning the journal acceptance criteria: I did not see why the presented approach would constitute a breakthrough or detail a groundbreaking discovery. To my understanding, fluctuations are not taken into account in basic Landau theory but a large literature exists on extensions to fluctuations and other methods. So the motivation given in the manuscript, that the role of fluctuations in phase transitions would be unclear, appears not justified.
Fluctuation-Driven Phase Transitions: theoretical perspectives and unresolved questions Yes, while fundamental Landau theory neglects fluctuations, most phase transitions originate from thermodynamic or quantum fluctuations. The mechanism of topological phase transitions remains unclear to me within this framework. Current Research Limitations
The vast literature on fluctuation propagation and interaction methods: Fails to provide clear mechanisms linking fluctuations to phase transitions Primarily focuses on symmetry principles as explanatory frameworks In my view, symmetry considerations alone prove insufficient for complete understanding Fundamental Challenge If we were to fully understand how fluctuations drive phase transitions, we would presumably possess: The analytical solution for the 3D Ising model A generalized theory transcending traditional symmetry-based approaches
-. However, maybe the "opens a new pathway [...] with clear potential for multi-pronged follow-up work" condition may be fulfilled, if the method was more clearly presented and discussed in the light of related literature.
Innovative Framework and Future Perspectives This work presents the first systematic formulation of higher-order detailed balance equations. By combining these equations with network modeling, I demonstrate: Clear visualization of physical mechanisms in strongly correlated systems Vast potential for deriving analytical solutions for various lattice models
Key Validation Achievements Successful application to Ising models demonstrates theoretical consistency Network structure analysis reveals critical transition pathways Predictions align with experimental results in specific cases (See Appendices A-B)
Five Promising Research Directions
1) External Field Effects Unresolved Question: How do external fields modify node weight distributions in this network model? Potential Impact: Could enable control of phase transition thresholds through field manipulation
2) Frustration Phenomena Studies Application Basis: Appendix A's uniaxial spin framework Target Systems: Wannier's antiferromagnetism (Phys. Rev. 79, 357 (1950)) Anderson's localized spin systems (Mater. Res. Bull. 8, 153 (1973)) Modern frustrated systems (PRL 123, 207203 (2019); PRX 9, 031026 (2019))
3) Glassy Systems Analysis Methodological Transfer: Adapt network model to study: Aging effects Non-equilibrium dynamics Appendix B's Edwards-Anderson model extension (J. Stat. Phys. 146, 118 (2012))
4) Fractal Critical Phenomena New Insight: Boundary structures (e.g., C₁₄ in 2D Ising) exhibit: Nonlinear weight evolution near critical points Fractal dimension signatures (Complementary to: AIP Adv. 14, 085107 (2024); Phys. Rev. E 110, L062107 (2024))
5) Quantum Circuit Error Analysis Interdisciplinary Potential: Map quantum error processes to network models: Local bit flips
Correlated error propagation Reference frameworks: Quantum Error Mitigation (PRL 119, 180509 (2017),Rev. Mod. Phys. 95, 045005 (2023),Phys. Rev. X 7, 021050 (2017)) Theoretical and Practical Significance Analytical Power: Unifies microscopic mechanisms with macroscopic observables through network formalism Interdisciplinary applicability: Provides common mathematical framework for: Classical spin systems Quantum information devices Disordered materials Computational Efficiency: Enables analytical treatment of complex correlations previously requiring numerical simulations
Manuscript Revision Plan I will perform substantial revisions to the manuscript as follows:
1)Reference Integration
Systematically incorporate all cited works into: Introduction (contextual framing) Conclusion (theoretical implications and future directions) Ensure seamless integration with existing narrative flow
2)Methodological Appendix Transfer detailed model construction procedures and case study demonstrations to: Appendix C: Comprehensive derivation of network model formalism Step-by-step validation with Ising model examples Comparative analysis with Monte Carlo simulations Include: Schematic diagrams illustrating transformation pathways Tabular summaries of critical exponent comparisons
3)Structural Optimization Streamline main text by: Removing redundant technical explanations Concentrating core innovations in theoretical framework Reserving experimental validations for dedicated sections Enhance reader navigation through: Updated table of contents Cross-referencing between main text and appendices Strategically placed summary paragraphs
I will submit the revised manuscript in the near future.
Sincerely, Yonglong Ding
Attachment:
SciPost_Physics_Reply.pdf