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arxiv: 2603.19096 · v2 · submitted 2026-03-19 · 🧮 math.NA · cs.NA

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GLENN: Neural network-enhanced computation of Ginzburg-Landau energy minimizers

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Pith reviewed 2026-05-15 08:26 UTC · model grok-4.3

classification 🧮 math.NA cs.NA
keywords Ginzburg-Landau energyneural networkdeep Ritz methodfinite element methodenergy minimizationkappa parameterunsupervised learning
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The pith

Neural network approximates Ginzburg-Landau minimizers for ranges of kappa

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper proposes a neural network-enhanced finite element strategy to compute the minimizer of the Ginzburg-Landau energy based on an unsupervised deep Ritz-type strategy. By treating the parameter kappa as a variable input, it obtains possible minimizers for a large range of kappa values. This allows for two strategies: using the neural network as a standalone solver after extensive training or using its results as starting values for classical iterative minimization. Numerical examples show the potential of the proposed strategy.

Core claim

The central claim is that an unsupervised neural network can be trained to approximate Ginzburg-Landau energy minimizers with kappa as input, yielding results usable either directly or as initial guesses that enable classical finite element methods to converge to the true minimizer.

What carries the argument

The unsupervised deep Ritz-type neural network strategy that directly minimizes the Ginzburg-Landau energy as the loss, with kappa included as an input variable.

Load-bearing premise

That the unsupervised neural network training produces approximations accurate enough to serve either as standalone solutions or as reliable initial guesses from which the classical finite element minimization converges to the true minimizer for a wide range of kappa values.

What would settle it

Observing a kappa value where starting the classical minimization from the neural network approximation fails to reach the global energy minimum obtained by other reliable methods.

Figures

Figures reproduced from arXiv: 2603.19096 by Benjamin D\"orich, Christian D\"oding, Michael Crocoll, Roland Maier.

Figure 1
Figure 1. Figure 1: Block schematic of a SwiGLU block (left) and a DAGLU block (right). Hardware. The training of the NNs used in the experiments is done on the HoreKa Tier 2 High Performance Computing system at KIT. The training uses four nodes with four NVIDIA A100 GPUs per node for a total of 16 GPUs. For the tuning and preliminary experimentation, we use the HAICORE@KIT partition of HoreKa. For the interpolation of the NN… view at source ↗
Figure 2
Figure 2. Figure 2: Densities |u| 2 of computed minimizers for κ = 10, 25, 50, 75, 100 (left to right), corresponding to [PITH_FULL_IMAGE:figures/full_fig_p014_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Densities |u| 2 of computed minimizers for κ = 10, 25, 50, 75, 100 (left to right), corresponding to [PITH_FULL_IMAGE:figures/full_fig_p016_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Densities |u| 2 of computed minimizers for κ = 10, 25, 50, 75, 100 (left to right), corresponding to [PITH_FULL_IMAGE:figures/full_fig_p017_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Densities |u| 2 of computed minimizers for κ = 10, 25, 50, 75, 100 (left to right), corresponding to [PITH_FULL_IMAGE:figures/full_fig_p018_5.png] view at source ↗
read the original abstract

In this work, we propose a neural network-enhanced finite element strategy to compute the minimizer of the Ginzburg-Landau energy based on an unsupervised deep Ritz-type strategy. We treat the parameter $\kappa$ as a variable input parameter to obtain possible minimizers for a large range of $\kappa$-values. This allows for two possible strategies: 1) The neural network may be extensively trained to work as a stand-alone solver. 2) Neural network results are used as starting values for a subsequent classical iterative minimization procedure. The latter strategy particularly circumvents the missing reliability of the neural network-based approach. Numerical examples are presented that show the potential of the proposed strategy.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript proposes GLENN, a neural network-enhanced finite element strategy to compute minimizers of the Ginzburg-Landau energy based on an unsupervised deep Ritz-type method that takes the parameter κ as an input variable. It outlines two strategies: extensive training of the neural network to serve as a standalone solver, or using the neural network outputs as initial guesses for a subsequent classical iterative minimization procedure. Numerical examples are presented to illustrate the potential of the approach, particularly for circumventing reliability issues in the standalone neural network method.

Significance. If the hybrid strategy reliably produces initial guesses that converge to global minimizers across a wide range of κ (including regimes with highly non-convex energy landscapes), the work could provide a practical tool for exploring vortex configurations in the Ginzburg-Landau model. The unsupervised training with κ as input and the explicit fallback to classical minimization are pragmatic strengths that address known limitations of pure neural network approaches in non-convex variational problems.

major comments (2)
  1. [Numerical examples] Numerical examples section: no quantitative metrics (e.g., relative energy errors, L2 differences to reference solutions, or success rates in reaching the global minimizer) are reported for the neural-network-initialized classical minimization, nor are direct comparisons provided against standard initial data (constant or random fields) for κ values where direct minimization is known to fail.
  2. [Abstract and method] Abstract and §2 (method description): the central claim that neural network results serve as reliable starting values for classical minimization lacks any a priori error bound, basin-of-attraction analysis, or demonstration that the unsupervised Ritz loss approximation systematically lies inside the attraction basin of the global minimizer rather than a local vortex configuration.
minor comments (2)
  1. [Method] Clarify the precise form of the Ritz-type loss functional when κ is treated as a network input, including how the penalty terms for the constraint |u|=1 are discretized.
  2. [Numerical examples] Add a brief discussion of training stability and hyperparameter sensitivity, as these directly affect reproducibility of the initial-guess strategy.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive feedback on our manuscript. We have carefully considered the major comments and provide point-by-point responses below. Revisions have been made to address the concerns regarding quantitative metrics and to clarify the scope of our claims.

read point-by-point responses
  1. Referee: Numerical examples section: no quantitative metrics (e.g., relative energy errors, L2 differences to reference solutions, or success rates in reaching the global minimizer) are reported for the neural-network-initialized classical minimization, nor are direct comparisons provided against standard initial data (constant or random fields) for κ values where direct minimization is known to fail.

    Authors: We agree that additional quantitative metrics would strengthen the presentation. In the revised manuscript, we have augmented the numerical examples section with relative energy errors with respect to reference solutions computed via classical methods with multiple initial guesses, L2 norm differences where applicable, and success rates in attaining the presumed global minimizer. Direct comparisons are now included against constant and random initial fields for κ values known to pose challenges for direct minimization, such as those leading to complex vortex lattices. These additions confirm the benefits of the neural network initialization. revision: yes

  2. Referee: Abstract and §2 (method description): the central claim that neural network results serve as reliable starting values for classical minimization lacks any a priori error bound, basin-of-attraction analysis, or demonstration that the unsupervised Ritz loss approximation systematically lies inside the attraction basin of the global minimizer rather than a local vortex configuration.

    Authors: The manuscript is focused on developing and demonstrating a practical computational strategy rather than providing theoretical guarantees. We do not claim a priori bounds or a full basin-of-attraction analysis, as these would require substantial additional theoretical developments that are beyond the paper's scope. Instead, we rely on comprehensive numerical experiments to show that the approach reliably converges to global minimizers. We have revised the abstract and Section 2 to explicitly state that the reliability is empirically observed and to discuss the limitations of the unsupervised Ritz method in non-convex settings without theoretical backing. revision: partial

Circularity Check

0 steps flagged

No circularity: standard deep Ritz NN for GL energy with hybrid FE fallback

full rationale

The paper's chain is the standard unsupervised deep Ritz minimization of the Ginzburg-Landau functional (with kappa as input parameter) followed by optional use of the NN output as an initial guess for classical finite-element iteration. No equation reduces the claimed minimizer to a quantity defined by the NN fit itself, no prediction is statistically forced by a subset fit, and no load-bearing step relies on self-citation or imported uniqueness theorems. The hybrid strategy explicitly acknowledges limited standalone reliability and defers to classical minimization, keeping the derivation self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard assumptions from variational calculus and finite element theory for the Ginzburg-Landau functional, plus the unproven effectiveness of the neural network approximation for this specific energy.

axioms (2)
  • domain assumption The Ginzburg-Landau energy functional admits a well-defined minimizer that can be approximated by finite element methods
    Invoked implicitly as the target of both the neural network and classical minimization procedures
  • ad hoc to paper Unsupervised training via a Ritz-type loss can produce useful approximations to the energy minimizer
    Core assumption enabling the neural network strategy; no independent verification provided in abstract

pith-pipeline@v0.9.0 · 5420 in / 1402 out tokens · 48220 ms · 2026-05-15T08:26:54.904804+00:00 · methodology

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Reference graph

Works this paper leans on

34 extracted references · 34 canonical work pages · 3 internal anchors

  1. [1]

    A. A. Abrikosov. Nobel lecture: Type-II superconductors and the vortex lattice.Rev. Mod. Phys., 76(3,1):975– 979, 2004

  2. [2]

    Adler and O

    J. Adler and O. ¨Oktem. Solving ill-posed inverse problems using iterative deep neural networks.Inverse Prob- lems, 33(12):124007, 24, 2017

  3. [3]

    Aftalion

    A. Aftalion. On the minimizers of the Ginzburg-Landau energy for high kappa: the axially symmetric case. Ann. Inst. H. Poincar´ e Anal. Non Lin´ eaire, 16(6):747–772, 1999

  4. [4]

    Ansel et al

    J. Ansel et al. PyTorch 2: Faster Machine Learning Through Dynamic Python Bytecode Transformation and Graph Compilation. In29th ACM International Conference on Architectural Support for Programming Languages and Operating Systems, Volume 2 (ASPLOS ’24). ACM, Apr. 2024

  5. [5]

    I. A. Baratta et al. DOLFINx: The next generation FEniCS problem solving environment, Dec. 2023

  6. [6]

    M. Blum, C. D¨ oding, and P. Henning. Vortex-capturing multiscale spaces for the Ginzburg-Landau equation. Multiscale Model. Simul., 23(1):339–373, 2025

  7. [7]

    Chaumont-Frelet and P

    T. Chaumont-Frelet and P. Henning. The pollution effect for FEM approximations of the Ginzburg-Landau equation.Math. Comp., page 49pp., 2026. Online first

  8. [8]

    Y. N. Dauphin, A. Fan, M. Auli, and D. Grangier. Language Modeling with Gated Convolutional Networks. 70:933–941, 06–11 Aug 2017

  9. [9]

    D¨ oding, B

    C. D¨ oding, B. D¨ orich, and P. Henning. A multiscale approach to the stationary Ginzburg–Landau equations of superconductivity. CRC 1173 Preprint 2024/21, Karlsruhe Institute of Technology, sep 2024

  10. [10]

    D¨ oding and P

    C. D¨ oding and P. Henning. The Ginzburg–Landau equations: Vortex states and numerical multiscale approxi- mations.ArXiv Preprint, 2511.19540, 2025

  11. [11]

    D¨ orich

    B. D¨ orich. Approximation of minimizers of the Ginzburg–Landau energy in non-convex domains. CRC 1173 Preprint 2025/44, Karlsruhe Institute of Technology, 2025

  12. [12]

    D¨ orich and P

    B. D¨ orich and P. Henning. Error bounds for discrete minimizers of the Ginzburg–Landau energy in the high-κ regime.SIAM J. Numer. Anal., 62(3):1313–1343, 2024

  13. [13]

    Q. Du, M. D. Gunzburger, and J. S. Peterson. Analysis and approximation of the Ginzburg-Landau model of superconductivity.SIAM Rev., 34(1):54–81, 1992

  14. [14]

    Q. Du, M. D. Gunzburger, and J. S. Peterson. Modeling and analysis of a periodic Ginzburg-Landau model for type-II superconductors.SIAM J. Appl. Math., 53(3):689–717, 1993

  15. [15]

    Du and L

    Q. Du and L. Ju. Approximations of a Ginzburg-Landau model for superconducting hollow spheres based on spherical centroidal Voronoi tessellations.Math. Comp., 74(251):1257–1280, 2005

  16. [16]

    Q. Du, R. A. Nicolaides, and X. Wu. Analysis and convergence of a covolume approximation of the Ginzburg- Landau model of superconductivity.SIAM J. Numer. Anal., 35(3):1049–1072, 1998

  17. [17]

    W. E and B. Yu. The Deep Ritz Method: A Deep Learning-Based Numerical Algorithm for Solving Variational Problems.Commun. Math. Stat., 6(1):1–12, 2018

  18. [18]

    Goodfellow, Y

    I. Goodfellow, Y. Bengio, and A. Courville.Deep Learning. MIT Press, 2016

  19. [19]

    Goyal, P

    P. Goyal, P. Doll´ ar, R. Girshick, P. Noordhuis, L. Wesolowski, A. Kyrola, A. Tulloch, Y. Jia, and K. He. Accurate, Large Minibatch SGD: Training ImageNet in 1 Hour, 2018

  20. [20]

    Jordan, Y

    K. Jordan, Y. Jin, V. Boza, J. You, F. Cesista, L. Newhouse, and J. Bernstein. Muon: An optimizer for hidden layers in neural networks, 2024. 20 M. CROCOLL, C. D ¨ODING, B. D ¨ORICH, AND R. MAIER

  21. [21]

    D. P. Kingma and J. Ba. Adam: A Method for Stochastic Optimization. InInternational Conference on Learning Representations, 2014

  22. [22]

    Muon is Scalable for LLM Training

    J. Liu et al. Muon is scalable for LLM Training.ArXiv Preprint, 2502.16982, 2025

  23. [23]

    H. K. Onnes. Further experiments with liquid helium. c. on the change of electric resistance of pure metals at very low temperatures, etc. iv. the resistance of pure mercury at helium temperatures.Comm. Phys. Lab. Univ. Leiden, 120(120b), 1911

  24. [24]

    Peterseim, J.-F

    D. Peterseim, J.-F. Pietschmann, J. P¨ uschel, and K. Ruess. Neural network acceleration of iterative methods for nonlinear Schr¨ odinger eigenvalue problems.J. Comput. Appl. Math., 485:Paper No. 117414, 2026

  25. [25]

    Polak and G

    E. Polak and G. Ribi` ere. Note sur la convergence de m´ ethodes de directions conjugu´ ees.Rev. Fran¸ caise Infor- mat. Recherche Op´ erationnelle, 3(16):35–43, 1969

  26. [26]

    Raissi, P

    M. Raissi, P. Perdikaris, and G. Karniadakis. Physics-informed neural networks: A deep learning framework for solving forward and inverse problems involving nonlinear partial differential equations.J. Comput. Phys., 378:686–707, 2019

  27. [28]

    Sandier and S

    E. Sandier and S. Serfaty.Vortices in the magnetic Ginzburg-Landau model, volume 70 ofProgress in Nonlinear Differential Equations and their Applications. Birkh¨ auser Boston, Inc., Boston, MA, 2007

  28. [29]

    Sandier and S

    E. Sandier and S. Serfaty. From the Ginzburg-Landau model to vortex lattice problems.Comm. Math. Phys., 313(3):635–743, 2012

  29. [30]

    S. Serfaty. Stable configurations in superconductivity: uniqueness, multiplicity, and vortex-nucleation.Arch. Ration. Mech. Anal., 149(4):329–365, 1999

  30. [31]

    Serfaty and E

    S. Serfaty and E. Sandier. Vortex patterns in Ginzburg-Landau minimizers. InXVIth International Congress on Mathematical Physics, pages 246–264. World Sci. Publ., Hackensack, NJ, 2010

  31. [32]

    N. Shazeer. GLU variants improve transformer.ArXiv Preprint, 2002.05202, 2020

  32. [33]

    Touvron, M

    H. Touvron, M. Cord, A. Sablayrolles, G. Synnaeve, and H. Jegou. Going deeper with Image Transformers . In2021 IEEE/CVF International Conference on Computer Vision (ICCV), pages 32–42, Los Alamitos, CA, USA, Oct. 2021. IEEE Computer Society

  33. [34]

    Venkataraman and B

    S. Venkataraman and B. Amos. Neural Fixed-Point Acceleration for Convex Optimization. In8th ICML Work- shop on Automated Machine Learning (AutoML), 2021

  34. [35]

    Fixup Initialization: Residual Learning Without Normalization

    H. Zhang, Y. N. Dauphin, and T. Ma. Fixup initialization: Residual learning without normalization.ArXiv Preprint, 1901.09321, 2019. Institute for Applied and Numerical Mathematics, Karlsruhe Institute of Technology, 76149 Karl- sruhe, Germany Email address:{michael.crocoll,benjamin.doerich,roland.maier}@kit.edu Institute for Numerical Simulation, Universi...