Learning the Helmholtz equation operator with DeepONet for non-parametric 2D geometries

arXiv cs.LG / 5/4/2026

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Key Points

  • The paper proposes a physics-informed DeepONet-based neural operator to solve the 2D Helmholtz equation on non-parameterized, non-uniform geometries.
  • It models an inner scatterer in the center of a square domain, using a signed distance function to encode arbitrary boundary shapes for the DeepONet branch network.
  • The trunk network uses local information, enabling the model to learn the mapping from scatterer geometry to the resulting scattered wavefield.
  • The authors test generalization on unseen geometries by comparing outputs with finite element method (FEM) results, showing that adequate coverage of the training space is key.
  • The method aims to provide a computationally lighter, geometry-flexible surrogate that can be refined to new regions without full retraining and avoids remeshing and reliance on FEM-generated training data.

Abstract

This paper deals with solving the 2D Helmholtz equation on non-parametric domains, leveraging a physics-informed neural operator network based on the DeepONet framework. We consider a 2D square domain with an inclusion of arbitrary boundary geometry at its center. This inclusion acts as a scatterer for an incoming harmonic wave. The aim is to learn the operator linking the geometry of the scatterer to the resulting scattered field. A signed distance function to the boundary of the inner inclusion, evaluated at several points in the domain, is used to encode its geometry. It serves as input for the branch part of the DeepONet architecture, while local information is used as input for the trunk part. This approach enables the encoding of arbitrary geometries, whether they are parameterized or not. The evaluation of the model on unseen geometries is compared with its finite element method (FEM) equivalent to test its generalization capabilities. The trained network weights implicitly embed the local physics and their interaction with the domain geometry. If the training space sufficiently covers the target evaluation space, the model can generalize accordingly. Furthermore, it can be refined to extend to another region of interest without retraining from scratch. This framework also avoids the need to remesh the domain for each geometry. The proposed approach delivers a computationally lighter surrogate model than FEM alternatives and avoids relying on FEM-generated training data.

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