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arxiv: 2602.04923 · v2 · submitted 2026-02-04 · 💻 cs.LG

Recognition: 2 theorem links

· Lean Theorem

Imposing Boundary Conditions on Neural Operators via Learned Function Extensions

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Pith reviewed 2026-05-16 07:08 UTC · model grok-4.3

classification 💻 cs.LG
keywords neural operatorsboundary conditionsfunction extensionsPDE surrogatesoperator learningscientific machine learningmixed boundary conditions
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The pith

Mapping boundary data to full-domain latent extensions lets any standard neural operator handle complex mixed-type conditions accurately.

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

The paper establishes that neural operators, which learn mappings between functions to solve PDEs, can be made to respect arbitrary boundary conditions by first learning to extend those boundary values into a pseudo-field defined everywhere in the domain. This extended field is then supplied as an additional input channel to an unmodified neural operator, so the model learns both the interior PDE behavior and the boundary influence simultaneously. The approach is demonstrated across eighteen new benchmark datasets that include Poisson problems, linear elasticity, and hyperelasticity on varied geometries with highly variable, component-wise, and multi-segment boundaries. A reader would care because most engineering PDEs involve non-homogeneous or mixed boundary data that current operator learners handle poorly or only after heavy architecture redesign.

Core claim

By training a separate network to map boundary data into latent pseudo-extensions over the full spatial domain, any off-the-shelf domain-to-domain neural operator can consume boundary information without modification and thereby learn solution operators that depend strongly on complex, non-homogeneous, and mixed-type boundary conditions.

What carries the argument

The learned boundary-to-domain function extension, which converts discrete or partial boundary values into a continuous latent field defined over the entire domain so that a standard neural operator can process it as an input function.

If this is right

  • Existing neural operator architectures can be reused for a much wider class of PDE problems that include complex real-world boundary data.
  • No dataset-specific hyperparameter search is required once the extension network is trained.
  • The same framework applies equally to scalar Poisson problems and vector elasticity problems with component-wise boundary conditions.
  • Training remains stable across geometries that differ in the number and placement of boundary segments.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same extension idea could be tested on time-dependent or parametric PDEs where boundaries vary in time or with parameters.
  • If the extension network is made invertible, it might allow direct enforcement of hard boundary constraints rather than soft learning.
  • Performance on noisy or incomplete boundary measurements would indicate whether the method remains practical for experimental data.

Load-bearing premise

A neural network can learn to produce boundary extensions that are consistent enough for the downstream operator to capture true boundary dependence without introducing spurious artifacts.

What would settle it

On a held-out dataset with multi-segment mixed Dirichlet-Neumann boundaries, if the method produces interior solutions whose boundary traces deviate from the prescribed data by more than the reported error margins while a suitably modified baseline does not, the central claim is falsified.

Figures

Figures reproduced from arXiv: 2602.04923 by Laura De Lorenzis, Sepehr Mousavi, Siddhartha Mishra.

Figure 1
Figure 1. Figure 1: Overview of an extended encode-process-decode OL framework. The bottom row shows the placement of the proposed extender module into the framework; the top row shows our proposed attention￾based architecture as a realization of the extender. Domain features and boundary features are depicted by pink and green dots, respectively. Initial geometrical domain features are progressively informed by the boundary … view at source ↗
Figure 2
Figure 2. Figure 2: Median relative L 2 error [%] of 256 test samples with different methods (columns). Each row corresponds to one dataset, see Appendix C for details. All trainings are done using 8,192 training and 256 validation samples. Geometries containing holes are indicated with H. Extension methods are combined with RIGNO (R) and GAOT (G). The reported errors for the elasticity and hyperelasticity problems are the av… view at source ↗
Figure 3
Figure 3. Figure 3: Scaling of model accuracy with the size of the training dataset. Median relative L 2 test errors on 256 samples are reported. The Pois￾son and elasticity problems are considered on the Circle and the CircleH geometries, respectively. All trainings are done with a model of size 3.6M (1.8M for the extender and 1.8M for the core). 0.3 0.6 1.2 1.8 3.0 Extender parameters [M] 5 10 20 Error [%] 4.8 5.0 5.4 5.9 6… view at source ↗
Figure 5
Figure 5. Figure 5: Results of transfer learning experiments for the Poisson problem on the Circle domain with the Mixed BCs configuration as the target dataset. The extender shows strong generalization to different geometries and previously unseen BC types. The test error of the pre-trained models on the base dataset is marked with a star. The green dots represent the test error on the target dataset after fine-tuning with 5… view at source ↗
Figure 6
Figure 6. Figure 6: Model accuracy on the Poisson problem on the Circle domain against the level of Gaussian noise in the input boundary functions. The y-axis shows relative L 2 test errors on 256 samples, and the x-axis shows the ratio between the mean of the squared noise and the mean of the squared signal in percentage. This metric is the inverse of the widely used signal-to-noise ratio. Further experiments. Additional exp… view at source ↗
read the original abstract

Neural operators have emerged as powerful surrogates for the solution of partial differential equations (PDEs), yet their ability to handle general, highly variable boundary conditions (BCs) remains limited. Existing approaches often fail when the solution operator exhibits strong sensitivity to boundary forcings. We propose a general framework for conditioning neural operators on complex non-homogeneous BCs through function extensions. Our key idea is to map boundary data to latent pseudo-extensions defined over the entire spatial domain, enabling any standard operator learning architecture to consume boundary information. The resulting operator, coupled with an arbitrary domain-to-domain neural operator, can learn rich dependencies on complex BCs and input domain functions at the same time. To benchmark this setting, we construct 18 challenging datasets spanning Poisson, linear elasticity, and hyperelasticity problems, with highly variable, mixed-type, component-wise, and multi-segment BCs on diverse geometries. Our approach achieves state-of-the-art accuracy, outperforming baselines by large margins, while requiring no hyperparameter tuning across datasets. Overall, our results demonstrate that learning boundary-to-domain extensions is an effective and practical strategy for imposing complex BCs in existing neural operator frameworks, enabling accurate and robust scientific machine learning models for a broader range of PDE-governed problems.

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 paper proposes a general framework for conditioning neural operators on complex, non-homogeneous boundary conditions by learning latent pseudo-extensions over the full spatial domain from boundary data. This allows any standard domain-to-domain neural operator to ingest the boundary information without architecture-specific modifications. The authors construct 18 datasets spanning Poisson, linear elasticity, and hyperelasticity problems with highly variable, mixed-type, component-wise, and multi-segment BCs on diverse geometries, and report state-of-the-art accuracy that outperforms baselines by large margins with no hyperparameter tuning required across datasets.

Significance. If the central empirical claims hold under rigorous verification, the work would address a key limitation in neural operator applicability to PDEs with general boundary conditions, enabling broader use in scientific machine learning without custom architectures. The construction of 18 challenging benchmark datasets is a positive contribution that could serve the community, and the no-tuning aspect would enhance practical utility if the performance gains prove robust.

major comments (2)
  1. [Section 3 (Method)] The core construction maps boundary data to learned latent pseudo-extensions without an explicit boundary-matching loss or hard constraint that would enforce exact agreement between the extension and the prescribed data on the boundary (see the training objective and extension network description). This assumption is load-bearing for the SOTA claim on BC-sensitive problems, as any systematic residual could propagate into the learned operator.
  2. [Section 4 (Experiments)] The experimental section asserts large-margin outperformance on all 18 datasets but provides insufficient detail on baseline architectures, quantitative metrics (e.g., relative L2 errors with error bars), ablation studies, or dataset construction protocols to rule out post-hoc tuning or artifacts in the benchmark creation.
minor comments (2)
  1. [Section 2 (Preliminaries)] Notation for the latent pseudo-extension versus the input domain function could be clarified to avoid potential confusion in the operator definition.
  2. [Figure 2] Figure captions for the dataset visualizations should explicitly state the range of BC variability shown in each panel.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive comments on our manuscript. We address each major comment below and describe the revisions we will incorporate.

read point-by-point responses
  1. Referee: [Section 3 (Method)] The core construction maps boundary data to learned latent pseudo-extensions without an explicit boundary-matching loss or hard constraint that would enforce exact agreement between the extension and the prescribed data on the boundary (see the training objective and extension network description). This assumption is load-bearing for the SOTA claim on BC-sensitive problems, as any systematic residual could propagate into the learned operator.

    Authors: We agree with the referee that the absence of an explicit boundary-matching term is a limitation in the current formulation. Although the joint PDE-residual training provides implicit pressure toward boundary consistency, this is insufficient to guarantee exact matching. In the revised manuscript we will augment the training objective in Section 3 with an explicit boundary-matching loss (L2 discrepancy between the learned extension and the prescribed boundary data on the boundary), and we will report the updated results. This change directly addresses the concern and strengthens the reliability of the SOTA claims. revision: yes

  2. Referee: [Section 4 (Experiments)] The experimental section asserts large-margin outperformance on all 18 datasets but provides insufficient detail on baseline architectures, quantitative metrics (e.g., relative L2 errors with error bars), ablation studies, or dataset construction protocols to rule out post-hoc tuning or artifacts in the benchmark creation.

    Authors: We acknowledge that the experimental section requires substantially more detail to allow independent verification. In the revision we will expand Section 4 (and add a supplementary section) with: complete architectural specifications and hyperparameter values for every baseline; tables of relative L2 errors accompanied by standard deviations over at least five random seeds; systematic ablation studies isolating the contribution of the extension network; and a precise description of dataset construction, including BC sampling distributions, geometry generation procedures, and train/validation/test splits. These additions will eliminate any ambiguity regarding post-hoc tuning or benchmark artifacts. revision: yes

Circularity Check

0 steps flagged

No circularity: empirical framework validated on external benchmarks

full rationale

The paper describes a practical framework that learns boundary-to-domain extensions to condition standard neural operators on complex BCs. It introduces no mathematical derivation chain; instead it constructs 18 new datasets spanning Poisson, elasticity and hyperelasticity problems and reports accuracy against external baselines. No equations, fitted parameters, or self-citations are presented that would make any claimed prediction equivalent to its own inputs by construction. The central performance claim rests on measured generalization across held-out test cases rather than on internal redefinitions or load-bearing self-references.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

The central claim rests on the empirical effectiveness of the learned extension mapping; no explicit free parameters beyond standard neural network weights are declared, and the only invented entity is the latent pseudo-extension itself.

axioms (1)
  • domain assumption Standard neural operator architectures can consume additional input channels defined over the domain
    Implicit in the statement that any standard operator learning architecture can be used after the extension step.
invented entities (1)
  • latent pseudo-extensions no independent evidence
    purpose: Map boundary data to a function defined over the entire spatial domain so that boundary information can be consumed by domain-to-domain neural operators
    New construct introduced to enable the conditioning mechanism; no independent evidence outside the learned model is provided.

pith-pipeline@v0.9.0 · 5523 in / 1314 out tokens · 39590 ms · 2026-05-16T07:08:01.575027+00:00 · methodology

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Reference graph

Works this paper leans on

37 extracted references · 37 canonical work pages · 3 internal anchors

  1. [1]

    Alkin, A

    B. Alkin, A. Fürst, S. Schmid, L. Gruber, M. Holzleitner, and J. Brandstetter. Universal physics transformers: A framework for efficiently scaling neural operators. In A. Globerson, L. Mackey, D. Belgrave, A. Fan, U. Paquet, J. Tomczak, and C. Zhang, editors,Advances in Neural Information Processing Systems, volume 37, pages 25152–25194. Curran Associates...

  2. [3]

    J. L. Ba, J. R. Kiros, and G. E. Hinton. Layer normalization.arXiv preprint arXiv:1607.06450, 2016

  3. [4]

    I. A. Baratta, J. P. Dean, J. S. Dokken, M. Habera, J. S. Hale, C. N. Richardson, M. E. Rognes, M. W. Scroggs, N. Sime, and G. N. Wells. DOLFINx: the next generation FEniCS problem solving environment. preprint, 2023

  4. [5]

    Bartolucci, E

    F. Bartolucci, E. de Bezenac, B. Raonic, R. Molinaro, S. Mishra, and R. Alaifari. Representation equivalent neural operators: a framework for alias-free operator learning.Advances in Neural Information Processing Systems, 37, 2023

  5. [6]

    Brandstetter, D

    J. Brandstetter, D. E. Worrall, and M. Welling. Message passing neural PDE solvers. InInternational Conference on Learning Representations, 2022

  6. [7]

    Brock, S

    A. Brock, S. De, S. L. Smith, and K. Simonyan. High-performance large-scale image recognition without normalization.arXiv preprint arXiv:2102.06171, 2021

  7. [8]

    S. Cao. Choose a transformer: Fourier or Galerkin. In35th Conference on Neural Information Processing Systems, 2021

  8. [9]

    L. C. Evans.Partial differential equations, volume 19. American Mathematical Society, 2022

  9. [10]

    Gmsh, 2024

    Geuzaine, Christophe and Remacle, Jean-Francois. Gmsh, 2024. URL http://http://gmsh. info/

  10. [11]

    Z. Hao, C. Su, S. Liu, J. Berner, C. Ying, H. Su, A. Anandkumar, J. Song, and J. Zhu. Dpot: auto- regressive denoising operator transformer for large-scale PDE pre-training. InProceedings of the 41st International Conference on Machine Learning, ICML’24, 2024

  11. [12]

    Herde, B

    M. Herde, B. Raoni ´c, T. Rohner, R. Käppeli, R. Molinaro, E. de Bézenac, and S. Mishra. Poseidon: Efficient foundation models for PDEs. In A. Globerson, L. Mackey, D. Belgrave, A. Fan, U. Paquet, J. Tomczak, and C. Zhang, editors,Advances in Neural Information Processing Systems, volume 37, pages 72525–72624. Curran Associates, Inc., 2024. doi: 10.52202/...

  12. [13]

    Horie and N

    M. Horie and N. Mitsume. Physics-embedded neural networks: Graph neural PDE solvers with mixed boundary conditions.Advances in Neural Information Processing Systems, 35:23218–23229, 2022

  13. [14]

    Scaling Laws for Neural Language Models

    J. Kaplan, S. McCandlish, T. Henighan, T. B. Brown, B. Chess, R. Child, S. Gray, A. Radford, J. Wu, and D. Amodei. Scaling laws for neural language models.CoRR, abs/2001.08361, 2020. 11

  14. [15]

    Kashi, A

    A. Kashi, A. Daw, M. G. Meena, and H. Lu. Learning the boundary-to-domain mapping using lifting product Fourier neural operators for partial differential equations. InAI for Science Workshop of International Conference on Machine Learning, 2024

  15. [16]

    Kovachki, Z

    N. Kovachki, Z. Li, B. Liu, K. Azizzadenesheli, K. Bhattacharya, A. Stuart, and A. Anandkumar. Neural operator: Learning maps between function spaces with applications to PDEs.Journal of Machine Learning Research, 24(89):1–97, 2023

  16. [17]

    Lanthaler, S

    S. Lanthaler, S. Mishra, and G. E. Karniadakis. Error estimates for DeepONets: A deep learning framework in infinite dimensions.Transactions of Mathematics and Its Applications, 6(1):tnac001, 2022

  17. [18]

    Z. Li, N. B. Kovachki, K. Azizzadenesheli, B. Liu, K. Bhattacharya, A. Stuart, and A. Anandkumar. Fourier neural operator for parametric partial differential equations. InInternational Conference on Learning Representations, 2021

  18. [19]

    Z. Li, N. B. Kovachki, C. Choy, B. Li, J. Kossaifi, S. P. Otta, M. A. Nabian, M. Stadler, C. Hundt, K. Azizzadenesheli, and A. Anandkumar. Geometry-informed neural operator for large-scale 3D PDEs. In37th Conference on Neural Information Processing Systems, 2023

  19. [20]

    Z. Liu, Y . Wu, D. Z. Huang, H. Zhang, X. Qian, and S. Song. SPFNO: Spectral operator learning for pdes with Dirichlet and Neumann boundary conditions.arXiv preprint arXiv:2312.06980, 2023

  20. [21]

    Loshchilov and F

    I. Loshchilov and F. Hutter. Decoupled weight decay regularization. InInternational Conference on Learning Representations, 2019

  21. [22]

    Lötzsch, S

    W. Lötzsch, S. Ohler, and J. Otterbach. Learning the solution operator of boundary value problems using graph neural networks. InAI for Science Workshop of International Conference on Machine Learning, 2022

  22. [23]

    L. Lu, P. Jin, G. Pang, Z. Zhang, and G. E. Karniadakis. Learning nonlinear operators via DeepONet based on the universal approximation theorem of operators.Nature Machine Intelligence, 2021

  23. [24]

    McCabe, B

    M. McCabe, B. R.-S. Blancard, L. H. Parker, R. Ohana, M. Cranmer, A. Bietti, M. Eickenberg, S. Golkar, G. Krawezik, F. Lanusse, M. Pettee, T. Tesileanu, K. Cho, and S. Ho. Multiple physics pretraining for spatiotemporal surrogate models. In38th Annual Conference on Neural Information Processing Systems, 2024

  24. [25]

    Mishra and A

    S. Mishra and A. E. Townsend.Numerical analysis meets machine learning. Handbook of Numerical Analysis. Springer, 2024

  25. [26]

    Mousavi, S

    S. Mousavi, S. Wen, L. Lingsch, M. Herde, B. Raoni ´c, and S. Mishra. RIGNO: A graph-based framework for robust and accurate operator learning for PDEs on arbitrary domains. InAdvances in Neural Information Processing Systems, volume 38, 2025

  26. [27]

    Pfaff, M

    T. Pfaff, M. Fortunato, A. Sanchez-Gonzalez, and P. Battaglia. Learning mesh-based simulation with graph networks. InInternational Conference on Learning Representations, 2021

  27. [28]

    Quarteroni, A

    A. Quarteroni, A. Manzoni, and F. Negri.Reduced basis methods for partial differential equations: an introduction, volume 92. Springer, 2015

  28. [29]

    Searching for Activation Functions

    P. Ramachandran, B. Zoph, and Q. V . Le. Searching for activation functions.arXiv preprint arXiv:1710.05941, 2017

  29. [30]

    Raonic, R

    B. Raonic, R. Molinaro, T. De Ryck, T. Rohner, F. Bartolucci, R. Alaifari, S. Mishra, and E. de Bézenac. Convolutional neural operators for robust and accurate learning of PDEs. InAdvances in Neural Information Processing Systems, 2024. 12

  30. [31]

    N. Saad, G. Gupta, S. Alizadeh, and D. C. Maddix. Guiding continuous operator learning through physics-based boundary constraints. InInternational Conference on Learning Representations, 2023

  31. [32]

    Sanchez-Gonzalez, J

    A. Sanchez-Gonzalez, J. Godwin, T. Pfaff, R. Ying, J. Leskovec, and P. Battaglia. Learning to simulate complex physics with graph networks. InInternational Conference on Machine Learning, pages 8459–8468. PMLR, 2020

  32. [33]

    Subramanian, P

    S. Subramanian, P. Harrington, K. Keutzer, W. Bhimji, D. Morozov, M. W. Mahoney, and A. Gholami. Towards foundation models for scientific machine learning: Characterizing scaling and transfer behavior. InAdvances in Neural Information Processing Systems, volume 36, pages 71242–71262. Curran Associates, Inc., 2023

  33. [34]

    H. Wang, J. LI, A. Dwivedi, K. Hara, and T. Wu. BENO: Boundary-embedded neural operators for elliptic PDEs. InInternational Conference on Learning Representations, 2024

  34. [35]

    S. Wen, A. Kumbhat, L. Lingsch, S. Mousavi, Y . Zhao, P. Chandrashekar, and S. Mishra. Geometry aware operator transformer as an efficient and accurate neural surrogate for PDEs on arbitrary domains. InAdvances in Neural Information Processing Systems, volume 38, 2025

  35. [36]

    H. Wu, H. Luo, H. Wang, J. Wang, and M. Long. Transolver: A fast transformer solver for PDEs on general geometries. InInternational Conference on Machine Learning, 2024

  36. [37]

    B. Zeng, Q. Wang, M. Yan, Y . Liu, R. Chengze, Y . Zhang, H. Liu, Z. Wang, and H. Sun. PhyMPGN: Physics-encoded message passing graph network for spatiotemporal PDE systems. InInternational Conference on Learning Representations, 2025. 13 Appendix A Theory A.1 The Poisson equation with non-homogeneous BCs Let us consider the Poisson equation with non-homo...

  37. [38]

    The masking procedure in described in detail in Appendix E

    for obtaining resolution invariance, we repeat each training with masked CA blocks with a masking ratio of0.3. The masking procedure in described in detail in Appendix E. The results are presented in Figure F.5. The models trained with regular CA exhibit strong dependence on the training resolution, with a slightly milder drop in the performance for highe...