Universal Symmetry-Breaking Dynamics at Continuous Phase Transitions: Evidence for a New Dynamical Critical Exponent
Pith reviewed 2026-05-11 03:29 UTC · model grok-4.3
The pith
Order-parameter fluctuations in Ising models collapse temporally after symmetry-breaking quenches via a new dynamical critical exponent.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Following a sudden symmetry-breaking quench at continuous phase transitions, the order-parameter fluctuations in Ising models display a compelling temporal collapse indicative of a single-variable scaling form. This is accounted for by introducing a new dynamical critical exponent. The universal regime appears in the 2D quantum Ising model and the 3D and 4D classical Ising models, but is absent in the 1D quantum and 2D classical cases, consistent with a lower critical effective dimension.
What carries the argument
The emergent single-variable scaling form for order-parameter fluctuations after the quench, carried by a new dynamical critical exponent.
If this is right
- The universal scaling is observed only above a lower critical effective dimension.
- It may characterize systems with non-conserved order parameters more generally.
- New avenues exist for exploring universal dynamics in theoretical models and experimental platforms.
- Finite-size and quench-strength independence suggests robustness of the scaling.
- The breakdown in lower dimensions confirms the critical dimension cutoff.
Where Pith is reading between the lines
- Similar collapses might be testable in other non-conserved order parameter systems like the Heisenberg model.
- Experimental platforms such as ultracold atoms could observe this scaling directly.
- If confirmed, this exponent could be used to classify dynamical universality classes beyond equilibrium critical exponents.
- Extensions to other quench protocols or conserved order parameters might reveal related phenomena.
Load-bearing premise
The numerical temporal collapse is caused by a new universal dynamical exponent rather than by model-specific finite-size effects or choices in the scaling analysis.
What would settle it
Performing larger-scale simulations or experiments in the 2D classical Ising model that still fail to show the collapse, or finding that the required exponent varies with quench details, would falsify the universality claim.
Figures
read the original abstract
Uncovering and understanding universal dynamics in matter far from equilibrium remains a key challenge. In this work, we identify a so far unrecognized form of universal behavior that emerges after a sudden symmetry-breaking quench at continuous phase transitions. Our key observation is that the order-parameter fluctuations in Ising models exhibit a compelling temporal collapse across a wide range of system sizes and quench strengths, indicative of an emergent single-variable scaling form. This phenomenon can be explained by introducing a so far unknown dynamical critical exponent for the underlying continuous phase transition. We find evidence for a lower critical effective dimension of this universal regime: it is observed in the 2D quantum and 3D and 4D classical Ising models, but not in the 1D quantum or 2D classical cases. Our results suggest that our observed universal far-from-equilibrium scaling may extend beyond the Ising models studied here and could more broadly characterize systems with non-conserved order parameters, opening new avenues for exploring universal dynamics both theoretically and in current experimental platforms.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that after a sudden symmetry-breaking quench through a continuous phase transition, order-parameter fluctuations in Ising models exhibit a temporal collapse onto a single-variable scaling form across system sizes and quench strengths. This is observed numerically in 2D quantum and 3D/4D classical Ising models (but not 1D quantum or 2D classical), and is explained by introducing a previously unknown dynamical critical exponent, with evidence for a lower critical effective dimension.
Significance. If the central claim holds, the identification of a new universal far-from-equilibrium scaling regime at continuous phase transitions would be significant for non-equilibrium statistical mechanics and quantum dynamics. The numerical evidence of collapse in multiple Ising variants provides a concrete starting point for exploring universal dynamics beyond equilibrium critical phenomena, with potential relevance to experiments in ultracold atoms or quantum simulators.
major comments (2)
- [Abstract and main results section] Abstract and scaling analysis: The new dynamical critical exponent is introduced specifically to account for the observed single-variable collapse of order-parameter fluctuations, but no independent derivation, renormalization-group analysis, or relation to known static/dynamical exponents is provided; its value appears determined by fitting the same numerical data used to demonstrate the collapse.
- [Abstract] Abstract: The lower critical effective dimension (failure of collapse in 1D quantum and 2D classical Ising models) is diagnosed from the same set of simulations where the scaling is tested, without a prior theoretical prediction or field-theoretic argument for why the regime begins at effective dimension 3.
minor comments (2)
- The manuscript would benefit from explicit discussion of possible alternative explanations for the collapse, such as finite-size corrections or quench-protocol specifics, even if they are ultimately ruled out.
- Notation for the scaling variable and the new exponent should be introduced with a clear equation early in the text to improve readability.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of the potential significance of our work and for the constructive comments. We respond to each major comment below, indicating where revisions will be made to clarify the phenomenological nature of our findings.
read point-by-point responses
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Referee: [Abstract and main results section] Abstract and scaling analysis: The new dynamical critical exponent is introduced specifically to account for the observed single-variable collapse of order-parameter fluctuations, but no independent derivation, renormalization-group analysis, or relation to known static/dynamical exponents is provided; its value appears determined by fitting the same numerical data used to demonstrate the collapse.
Authors: We acknowledge that the dynamical critical exponent is introduced phenomenologically based on the observed collapse and is fitted from the numerical data. The primary evidence for its relevance is the robust single-variable scaling that holds across independent models (2D quantum, 3D and 4D classical Ising) with the same exponent value. This cross-model consistency is non-trivial and supports the claim of universality, even without a microscopic derivation. No renormalization-group analysis is provided because the phenomenon is far from equilibrium and lacks an established theoretical framework. In the revised manuscript we will expand the discussion section to explicitly state the phenomenological basis, note the absence of an independent derivation, and outline possible connections to known exponents while emphasizing that a full theoretical treatment remains an open question. revision: partial
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Referee: [Abstract] Abstract: The lower critical effective dimension (failure of collapse in 1D quantum and 2D classical Ising models) is diagnosed from the same set of simulations where the scaling is tested, without a prior theoretical prediction or field-theoretic argument for why the regime begins at effective dimension 3.
Authors: The lower critical effective dimension is identified empirically from the numerical observation that the collapse fails in the 1D quantum and 2D classical cases while succeeding in higher-dimensional analogs. We do not present a prior field-theoretic prediction; the finding is reported as a numerical result suggesting that the universal regime requires a minimum effective dimensionality. In the revised version we will modify the abstract and main text to make this empirical character explicit, remove any implication of a theoretical prediction, and add a statement calling for future theoretical work to explain the origin of the lower critical dimension of 3. revision: partial
Circularity Check
New dynamical critical exponent fitted to observed collapse without independent derivation; lower-critical-dimension cutoff diagnosed from same data
specific steps
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fitted input called prediction
[Abstract]
"Our key observation is that the order-parameter fluctuations in Ising models exhibit a compelling temporal collapse across a wide range of system sizes and quench strengths, indicative of an emergent single-variable scaling form. This phenomenon can be explained by introducing a so far unknown dynamical critical exponent for the underlying continuous phase transition. We find evidence for a lower critical effective dimension of this universal regime: it is observed in the 2D quantum and 3D and 4D classical Ising models, but not in the 1D quantum or 2D classical cases."
The single-variable scaling form is presented as evidence for a new exponent, yet the exponent is defined and its value chosen to produce the collapse in the same numerical data. The lower-critical-dimension cutoff is likewise extracted from the identical simulations where collapse is or is not observed, so both the exponent and the universality claim are statistically forced by the fitting procedure rather than independently derived or predicted.
full rationale
The paper's central claim is that order-parameter fluctuations exhibit a temporal collapse indicative of a single-variable scaling form, which is explained by a new dynamical critical exponent. This exponent is introduced specifically to account for the collapse observed in numerical simulations across system sizes and quenches. The lower critical effective dimension is identified by where collapse succeeds or fails in the identical set of simulations (2D quantum/3D-4D classical yes; 1D quantum/2D classical no). No renormalization-group derivation, relation to known exponents, or first-principles prediction of the exponent value is provided; the scaling variable is adjusted to produce the reported collapse. This makes the 'universal' scaling form and the new exponent reduce to a post-hoc fit to the data they are meant to describe, satisfying the fitted-input-called-prediction pattern.
Axiom & Free-Parameter Ledger
free parameters (1)
- new dynamical critical exponent
axioms (1)
- domain assumption Standard Ising Hamiltonian and dynamics (quantum or classical) govern the post-quench evolution
invented entities (1)
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new dynamical critical exponent
no independent evidence
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the data are plotted as a function of the single variable ĥ t̂^w … best collapse is obtained for w=1.86±0.05
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
evidence for a lower critical effective dimension … observed in the 2D quantum and 3D and 4D classical Ising models, but not in the 1D quantum or 2D classical cases
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
P. C. Hohenberg and B. I. Halperin, Reviews of Modern Physics49, 435 (1977)
work page 1977
-
[2]
U. C. Täuber,Critical Dynamics: A Field Theory Ap- proach to Equilibrium and Non-Equilibrium Scaling Be- havior(Cambridge University Press, Cambridge, 2014)
work page 2014
-
[3]
A. Pelissetto, D. Rossini, and E. Vicari, Phys. Rev. E97, 052148 (2018)
work page 2018
-
[4]
T. W. B. Kibble, Journal of Physics A: Mathematical and General9, 1387 (1976)
work page 1976
-
[5]
W. H. Zurek, Nature317, 505 (1985)
work page 1985
-
[6]
W. H. Zurek, Physics Reports276, 177 (1996)
work page 1996
-
[7]
W. H. Zurek, U. Dorner, and P. Zoller, Physical Review Letters95, 105701 (2005)
work page 2005
-
[8]
A. del Campo and W. H. Zurek, International Journal of Modern Physics A29, 1430018 (2014)
work page 2014
-
[9]
A. Keesling, A. Omran, H. Levine, H. Bernien, H. Pich- ler, S. Choi, R. Samajdar, S. Schwartz, P. Silvi, S. Sachdev, P. Zoller, M. Endres, M. Greiner, V. Vuletić, and M. D. Lukin, Nature568, 207 (2019)
work page 2019
-
[10]
H. K. Janssen, B. Schaub, and B. Schmittmann, Z. Phys. B73, 539 (1989)
work page 1989
- [11]
- [12]
- [13]
- [14]
-
[15]
A. Chiocchetta, M. Tavora, A. Gambassi, and A. Mitra, Phys. Rev. B91, 220302 (2015)
work page 2015
-
[16]
A. Chiocchetta, M. Tavora, A. Gambassi, and A. Mitra, Phys. Rev. B94, 134311 (2016)
work page 2016
-
[17]
C.-M. Schmied, A. N. Mikheev, and T. Gasenzer, Int. J. Mod. Phys. A34, 1941006 (2019)
work page 2019
- [18]
-
[19]
R. J. Glauber, J. Math. Phys.4, 294 (1963)
work page 1963
- [20]
- [21]
- [22]
-
[23]
H. W. J. Blöte and Y. Deng, Physical Review E66, 066110 (2002)
work page 2002
- [24]
-
[25]
A. M. Ferrenberg, J. Xu, and D. P. Landau, Phys. Rev. E97, 043301 (2018)
work page 2018
-
[26]
P. H. Lundow and K. Markström, Nucl. Phys. B993, 116256 (2023)
work page 2023
-
[27]
Verstraete, Physical Review Letters107, 070601 (2011)
J.Haegeman, J.I.Cirac, T.J.Osborne, I.Pižorn, H.Ver- schelde, and F. Verstraete, Physical Review Letters107, 070601 (2011)
work page 2011
- [28]
-
[29]
H. Bernien, S. Schwartz, A. Keesling, H. Levine, A. Om- ran, H. Pichler, S. Choi, A. S. Zibrov, M. Endres, M. Greiner, V. Vuletić, and M. D. Lukin, Nature551, 579 (2017)
work page 2017
- [30]
- [31]
-
[32]
J. W. Britton, B. C. Sawyer, A. C. Keith, C.-C. J. Wang, J.K.Freericks, H.Uys, M.J.Biercuk,andJ.J.Bollinger, Nature484, 489 (2012)
work page 2012
- [33]
- [34]
- [35]
-
[36]
S. Czischek, M. Gärttner, and T. Gasenzer, Physical Re- view B98, 024311 (2018)
work page 2018
- [37]
- [38]
- [39]
-
[40]
K. Choo, T. Neupert, and G. Carleo, Physical Review B 100, 125124 (2019). S1 Supplemental Material: Universal Dynamics for Symmetry-Breaking Quenches at Continuous Phase Transitions: Evidence for a New Dynamical Exponent Section I summarizes the Neural Quantum State (NQS) ansatz and TDVP accuracy diagnostics underlying the quantum data in Figs. 1 and 2. S...
work page 2019
discussion (0)
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