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$φ-$DeepONet: A Discontinuity Capturing Neural Operator

Published 9 Apr 2026 in cs.CE and math.AP | (2604.08076v1)

Abstract: We present $φ-$DeepONet, a physics-informed neural operator designed to learn mappings between function spaces that may contain discontinuities or exhibit non-smooth behavior. Classical neural operators are based on the universal approximation theorem which assumes that both the operator and the functions it acts on are continuous. However, many scientific and engineering problems involve naturally discontinuous input fields as well as strong and weak discontinuities in the output fields caused by material interfaces. In $φ$-DeepONet, discontinuities in the input are handled using multiple branch networks, while discontinuities in the output are learned through a nonlinear latent embedding of the interface. This embedding is constructed from a {\it one-hot} representation of the domain decomposition that is combined with the spatial coordinates in a modified trunk network. The outputs of the branch and trunk networks are then combined through a dot product to produce the final solution, which is trained using a physics- and interface-informed loss function. We evaluate $φ$-DeepONet on several one- and two-dimensional benchmark problems and demonstrate that it delivers accurate and stable predictions even in the presence of strong interface-driven discontinuities.

Summary

  • The paper introduces $φ$-DeepONet, a framework that embeds interface information via latent codes to robustly approximate discontinuous PDE solutions.
  • It employs multiple branch networks and an augmented trunk network to directly capture abrupt changes without explicit domain decomposition, achieving error reductions from 10⁻¹ to 10⁻³.
  • Numerical evaluations in 1D and 2D settings demonstrate its scalability and computational efficiency in modeling multiphysics problems with heterogeneous interfaces.

Formal Analysis of "φφ-DeepONet: A Discontinuity Capturing Neural Operator" (2604.08076)

Introduction and Motivation

The presented work introduces the φφ-DeepONet architecture, a neural operator framework optimized for PDEs with discontinuities arising from interfaces in heterogeneous media. Traditional neural operators, including DeepONet and its physics-informed variants, are limited by assumptions of continuity in both input and output function spaces. This restriction hinders applicability to interface problems where input fields and solution gradients often contain abrupt changes due to material heterogeneity or coupled physical regimes.

The φφ-DeepONet architecture directly addresses these challenges through a physics-informed and interface-aware neural operator embedding, designed for robust and accurate approximation of solution manifolds with strong and weak discontinuities. The method avoids explicit domain decomposition, leveraging latent embeddings to capture interface structure within the operator’s trunk network. Figure 1

Figure 1: Schematic of the problem domain with two regions Ω1\Omega_1 and Ω2\Omega_2 separated by an interface $\Gamma_{\text{12}$.

Methodological Framework

φφ-DeepONet extends the DeepONet formulation by integrating multiple branch networks to handle discontinuous inputs and a modified trunk network enriched with latent embeddings to encode output discontinuities caused by material interfaces. The architecture can be abstracted as follows:

  • Branch Networks: Each subdomain possesses its own dedicated branch net, encoding sampled input fields (possibly discontinuous) localized to that region.
  • Trunk Network Augmentation: The trunk is augmented to receive, alongside spatial coordinates, a latent variable ϕϕ that contains interface-specific information. The latent embedding is constructed via:
    • Scalar embedding (prescribed per subdomain)
    • Categorical (one-hot) embedding
    • Non-linear categorical embedding (learned projection matrix, optionally with a non-linear activation such as tanh\tanh)

The interface information is provided to the trunk network as an additional input, facilitating expressive modeling of discontinuous solution spaces. The final network output is produced by a dot product between the augmented trunk output and the concatenated branch outputs. Figure 2

Figure 2: Schematic of the architecture of φφ-DeepONet for approximating the operator φφ0.

Training is performed with a loss comprising soft enforcement of PDE, boundary, and interface jump constraints, enabling simultaneous satisfaction of physical laws and discontinuity conditions.

Numerical Evaluation and Results

The φφ1-DeepONet is systematically benchmarked against classical DeepONet and domain-decomposition operator networks (such as IONet) across a range of 1D and 2D problems with both continuous and discontinuous inputs.

1D Single Interface

For problems with a single sharp interface and continuous input functions, φφ2-DeepONet achieves mean relative φφ3 errors on the order of φφ4 to φφ5, substantially outperforming standard DeepONet (error φφ6). Non-linear categorical embedding variants yield the best accuracy. Computational cost remains comparable or lower than IONet, which incurs higher parameterization and training cost as the interface complexity increases.

1D Multiple Interfaces

When scaling to four interfaces and five subdomains, the accuracy trend persists: non-linear CE variants with moderate latent dimension (φφ7) produce mean test errors φφ8, outscoring baseline methods. Empirically, increasing latent dimension saturates gains and, for high-dimensional embeddings, can degrade performance through overparameterization, as evidenced in bimodal error distribution studies. Figure 3

Figure 3: Variation of the test φφ9 errors with increasing size of the input dataset (φφ0).

2D Discontinuous Domains

In two-dimensional interface problems (e.g., square domain with diagonal interface), φφ1-DeepONet achieves φφ2 errors down to φφ3 for non-linear CE trunk designs, reducing errors by up to two orders of magnitude over DeepONet. For complex, non-trivial interfaces (e.g., petal-shaped), compact latent embedding (φφ4 or φφ5) suffices for optimal performance, while higher-dimensional latent spaces are detrimental. Figure 4

Figure 4

Figure 4

Figure 4: Ablation study for 2D petal-shaped interface: error as function of trunk depth, number of training samples, and sensor resolution for different embedding dimensions.

Discontinuous Inputs and Outputs

For cases where both input and output functions are discontinuous, multiple branch networks per subdomain encode distinct input fields. The method sustains accuracy (φφ6 error φφ7 for moderate embedding dimension), while baselines deteriorate further.

Implications and Theoretical Insights

φφ8-DeepONet demonstrates that latent embedding of interface structure within trunk networks can supplant explicit domain decomposition for operator learning in heterogeneous domains. This approach reduces parameter proliferation as interface count increases, attaining both computational efficiency and improved fidelity near sharp transitions. The use of categorical or non-linear embeddings delivers flexibility and adaptability, important for problems with complex or evolving interfaces.

The tendency for diminishing returns and possible overfitting with high-dimensional latent spaces highlights the importance of embedding dimension selection—a critical hyperparameter warranting further theoretical investigation.

Practically, φφ9-DeepONet enables mesh-free surrogate modeling for multiphysics, materials science, and engineering problems that previously required laborious mesh generation or retraining for each new PDE parameterization. The approach supports broad generalization within the scope of training distributions and provides some, albeit limited, out-of-distribution generalization.

Future Directions

Potential extensions include:

  • Implicit interface learning: Removing reliance on fixed domain decomposition and learning interface structure entirely from data.
  • Continuous latent fields: Replacing piecewise constant embeddings with continuous, possibly learned, fields for finer interface modeling.
  • Strict constraint satisfaction: Transitioning from soft penalty enforcement to hard constraint satisfaction in trunk/branch parameterizations.
  • Multiphysics and uncertainty: Application to stochastic, multiphase, or coupled multiphysics systems where interface positions, properties, or dynamics are uncertain or time-varying.
  • Automated embedding selection: Theoretical and empirical analysis to determine optimal embedding dimension as function of interface and domain complexity.

Conclusion

Ω1\Omega_10-DeepONet constitutes an authoritative advance in operator learning for PDEs with discontinuous solutions, particularly interface-driven phenomena. By embedding interface information directly within the operator architecture rather than relying on explicit domain partitioning, the framework achieves substantial improvements in solution accuracy, computational efficiency, and scalability relative to conventional neural operators and domain-decomposed surrogates.

The architecture is robust across diverse problem settings as long as the interface partition and embedding are adequately specified. The framework’s limitations with unknown interfaces and dependence on embedding dimensionality underscore ongoing research directions for adaptive and fully data-driven interface representation. Ω1\Omega_11-DeepONet extends the neural operator paradigm toward practical modeling of discontinuous systems in applied mathematics, computational physics, and engineering.

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