Where to Compute and How to Interact: Operator-Readable Adaptation with Gauge-Aware Transport
Not on the map. Why?
Abstract (arXiv)
Adaptive meshes enable neural operators for partial differential equations (PDEs) to allocate spatial samples and computation according to local physical structures. Existing approaches, however, mainly address where to compute, with less attention to how information should interact after node relocation. Mesh adaptation changes local sampling scales, neighborhood structures, and geometric contexts, so representations formed at different nodes may not be directly comparable. Direct aggregation can therefore entangle physical variation with discretization-induced representation variation. Because allocation and interaction are jointly optimized through the same output objective, their individual roles are also difficult to distinguish from final errors alone. We introduce operator readability, requiring an adaptive operator to account for and test why computation is allocated to particular locations and how representations interact under the resulting nonuniform discretization. Based on this principle, we propose the Gauge-Aware Adaptive Mesh Neural Operator (GA-AMNO). Physics-informed adaptive allocation answers where to compute, while geometry-conditioned low-rank Gauge transport maps source features into target representation contexts before aggregation, answering how to interact. This makes mesh-to-solver information exchange inspectable and intervenable. We establish sufficient conditions for representation-consistent aggregation and analyze approximate transport errors and continuity under topology-preserving mesh deformations. Experiments on five PDE benchmarks demonstrate improved predictive accuracy, while controlled interventions and geometric-mismatch analyses verify the roles of allocation and interaction and show that Gauge transport improves cross-discretization representation compatibility under strong geometric mismatch.
Key facts. No citing papers in the map yet (data through 14 Oct 2026). Builds on 35 of its 47 references that are in the map. First posted on arXiv 14 Sep 2026.
Builds on
35 of 47 references.
References · 35
- 2015U-Net: Convolutional Networks for Biomedical Image Segmentationcited by 19,713
- 2020Fourier Neural Operator for Parametric Partial Differential Equationscited by 2,908
- 2019DeepONet: Learning nonlinear operators for identifying differential equations based on the universal approximation theorem of operatorscited by 2,018
- 2021Geometric Deep Learning: Grids, Groups, Graphs, Geodesics, and Gaugescited by 1,167
- 2021E(n) Equivariant Graph Neural Networkscited by 965
- 2020Learning to Simulate Complex Physics with Graph Networkscited by 880
- 2020Learning Mesh-Based Simulation with Graph Networkscited by 868
- 2020Neural Operator: Graph Kernel Network for Partial Differential Equationscited by 734
- 2020SE(3)-Transformers: 3D Roto-Translation Equivariant Attention Networkscited by 607
- 2021Physics-Informed Neural Operator for Learning Partial Differential Equationscited by 527
- 2022Fourier Neural Operator with Learned Deformations for PDEs on General Geometriescited by 427
- 2022Message Passing Neural PDE Solverscited by 386
23 more
- 20183D Steerable CNNs: Learning Rotationally Equivariant Features in Volumetric Datacited by 354
- 2023GNOT: A General Neural Operator Transformer for Operator Learningcited by 336
- 2024Transolver: A Fast Transformer Solver for PDEs on General Geometriescited by 326
- 2023Geometry-Informed Neural Operator for Large-Scale 3D PDEscited by 303
- 2019Gauge Equivariant Convolutional Networks and the Icosahedral CNNcited by 267
- 2021Factorized Fourier Neural Operatorscited by 249
- 2022U-NO: U-shaped Neural Operatorscited by 230
- 2023PDE-Refiner: Achieving Accurate Long Rollouts with Neural PDE Solverscited by 216
- 2024Poseidon: Efficient Foundation Models for PDEscited by 200
- 2020Combining Differentiable PDE Solvers and Graph Neural Networks for Fluid Flow Predictioncited by 138
- 2023Score-based Data Assimilationcited by 96
- 2020Gauge Equivariant Mesh CNNs: Anisotropic convolutions on geometric graphscited by 92
- 2024On conditional diffusion models for PDE simulationscited by 60
- 2023Representation Equivalent Neural Operators: a Framework for Alias-free Operator Learningcited by 57
- 2023Group Equivariant Fourier Neural Operators for Partial Differential Equationscited by 45
- 2019Graph Element Networks: adaptive, structured computation and memorycited by 41
- 2022Partial Differential Equations Meet Deep Neural Networks: A Surveycited by 25
- 2021Steerable Partial Differential Operators for Equivariant Neural Networkscited by 22
- 2023Learning Controllable Adaptive Simulation for Multi-resolution Physicscited by 20
- 2022M2N: Mesh Movement Networks for PDE Solverscited by 16
- 2023Better Neural PDE Solvers Through Data-Free Mesh Moverscited by 9
- 2023Modeling Dynamics over Meshes with Gauge Equivariant Nonlinear Message Passingcited by 3
- 2025UGM2N: An Unsupervised and Generalizable Mesh Movement Network via M-Uniform Losscited by 2
Built on by
Not cited yet.