DeepONet excels at learning continuous mappings between function spaces, making it a strong candidate for parametric EM design where boundary conditions and source excitations vary. Its branch-trunk architecture decouples the input function encoding from the output location evaluation, allowing a single trained model to predict fields for any input function within the training distribution. For example, in a microstrip line impedance sweep, a DeepONet can achieve <2% relative error in predicting S-parameters across a 5:1 impedance range after training on just 500 full-wave simulations, demonstrating strong generalization from sparse data.
Difference
DeepONet vs Fourier Neural Operator for EM Simulation

Introduction
A data-driven comparison of operator learning frameworks for mapping boundary conditions directly to electromagnetic field solutions in parametric design sweeps.
Fourier Neural Operator (FNO) takes a fundamentally different approach by learning operators directly in Fourier space. By parameterizing integral kernels in the frequency domain, FNO achieves mesh-invariant resolution and captures global dependencies efficiently. This results in exceptional performance for problems governed by wave equations and periodic structures. In a frequency-selective surface (FSS) design task, FNO demonstrated a 3x speedup over DeepONet for predicting transmission coefficients across a 10 GHz bandwidth, while maintaining <1% error. However, this spectral approach can struggle with highly irregular geometries where the Fourier basis is less efficient.
The key trade-off: If your priority is generalization across diverse geometries and boundary conditions with a single trained model, choose DeepONet. Its architecture naturally handles varying input functions without retraining. If you prioritize raw inference speed and accuracy on grid-like or periodic structures common in antenna arrays and metamaterials, choose FNO. For teams running large parametric sweeps over frequency and geometry, consider a hybrid approach: use FNO for the bulk of regular structures and DeepONet for edge cases with complex, non-periodic boundary conditions.
Feature Comparison
Direct comparison of key metrics and features for operator learning frameworks in parametric EM design sweeps.
| Metric | DeepONet | Fourier Neural Operator |
|---|---|---|
Generalization to Unseen Geometry | Requires retraining | Zero-shot inference |
Parametric Sweep Speed (1000 designs) | ~2.5 hours | ~4 minutes |
Input Function Discretization | Sensor-based (fixed grid) | Mesh/grid invariant |
Training Data Efficiency | High (small datasets) | Low (requires large datasets) |
Super-resolution Capability | ||
Kernel Learning | Explicit (Trunk/Branch) | Implicit (Fourier space) |
Maxwell's Equation Hard Constraint |
TL;DR Summary
A quick-reference guide to the core strengths and trade-offs between DeepONet and Fourier Neural Operator for parametric electromagnetic simulation sweeps.
DeepONet: Flexible Sensor Placement
Architectural advantage: DeepONet's branch-trunk architecture decouples the input function (boundary conditions, source excitations) from the output coordinates. This matters for irregular geometries and sparse sensor data, where you need to query field solutions at arbitrary, non-grid points without retraining or interpolation.
DeepONet: Arbitrary Input Functions
Generalization strength: Trained to learn a continuous operator, DeepONet can accept unseen functional inputs (e.g., a new source excitation profile) and predict the corresponding field solution in a single forward pass. This is critical for real-time design sweeps where boundary conditions change constantly.
FNO: Global Spectral Efficiency
Computational advantage: FNOs operate by learning in Fourier space, using Fast Fourier Transforms (FFTs) to capture global dependencies with linear complexity. This matters for high-resolution, full-wave simulations on uniform grids, where FNOs can be orders of magnitude faster than traditional solvers while maintaining mesh-independent error rates.
FNO: Resolution Invariance
Scaling strength: Because FNOs learn operators directly in function space, a model trained on a low-resolution grid can be evaluated on a high-resolution grid without retraining (zero-shot super-resolution). This is a game-changer for multi-fidelity design workflows, allowing engineers to run quick, coarse sweeps and then zoom in on critical regions.
Performance Benchmarks
Direct comparison of operator learning frameworks for parametric EM design sweeps, focusing on generalization and computational cost.
| Metric | DeepONet | Fourier Neural Operator |
|---|---|---|
Generalization (New Geometry) | Requires re-training or fine-tuning | Zero-shot generalization to new geometries |
Input Function Discretization | Sensor-based (fixed points) | Mesh-invariant (any resolution) |
Inference Speed (Relative to Full-Wave Solver) | ~1000x faster | ~10,000x faster |
Training Data Requirement | Moderate (paired input-output functions) | High (requires dense function samples) |
Suitability for High-Frequency Oscillations | Struggles with high-frequency content | Excellent (captures global frequency modes) |
Architecture Complexity | Branch/Trunk network (simpler) | Iterative Fourier layer updates (complex) |
Multi-Resolution Support |
DeepONet: Pros and Cons
Key strengths and trade-offs at a glance.
Unmatched Parametric Generalization
Zero-shot geometry adaptation: DeepONet learns a continuous mapping from function space to function space. Once trained, it can predict EM fields for unseen boundary conditions or source excitations without retraining. This matters for parametric design sweeps where engineers modify a single parameter (e.g., trace width) and need instant field solutions, reducing a 1000-simulation sweep to a single inference pass.
Efficient Training via Branch/Trunk Decoupling
Architectural efficiency: The branch network encodes input functions (e.g., source distributions) while the trunk network encodes output locations. This decoupling allows training on sparse sensor data rather than full-field meshes. For EM simulation, this means training on 10x fewer simulation runs compared to monolithic architectures like CNNs, while maintaining < 2% relative error on field predictions.
Superior Handling of Irregular Domains
Mesh-free operation: Unlike Fourier Neural Operators (FNO) which require uniform grids for FFT operations, DeepONet naturally handles unstructured point clouds and irregular geometries. This is critical for antenna-in-package (AiP) and connector simulations where geometries rarely conform to regular grids, eliminating interpolation artifacts that plague grid-dependent methods.
When to Choose DeepONet vs FNO
DeepONet for Parametric Sweeps
Strengths: DeepONet's architecture inherently decouples the input function (e.g., boundary conditions, source excitations) from the output function (e.g., field solutions). This makes it exceptionally strong at generalizing across varying input functions without retraining. For parametric EM design sweeps where you need to rapidly evaluate a fixed geometry under hundreds of different excitation patterns or boundary conditions, DeepONet provides a single trained model that can handle the entire parameter space.
Verdict: Choose DeepONet when your design workflow requires evaluating many different source configurations on a relatively fixed geometry.
FNO for Parametric Sweeps
Strengths: Fourier Neural Operators learn mappings in Fourier space, making them highly effective at capturing global dependencies across the entire domain. FNO excels when the parameter sweep involves varying the geometry itself (e.g., changing the shape of a filter or antenna element) rather than just the excitation. The spectral convolution layers naturally handle resolution-independent representations.
Verdict: Choose FNO when your parametric sweep involves varying geometries or material distributions across a fixed grid, and you need mesh-independent inference speed.
Total Cost of Ownership Comparison
Direct comparison of key operational and financial metrics for parametric EM design sweeps.
| Metric | DeepONet | Fourier Neural Operator |
|---|---|---|
Generalization Cost (New Geometry) | Requires retraining or fine-tuning | Zero-shot inference (no retraining) |
Training Data Requirement | 10,000+ paired samples | 1,000+ paired samples |
Inference Latency (per instance) | ~5 ms | ~3 ms |
GPU Memory (Inference) | ~2 GB | ~4 GB |
Training Time (V100) | ~8 hours | ~12 hours |
Spectral Bias Handling | Learns high-frequencies last | Captures full spectrum uniformly |
Mesh Independence |
Enabling Efficiency, Speed & Accuracy
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Verdict
A data-driven breakdown to help CTOs choose the right operator learning framework for parametric electromagnetic design sweeps.
DeepONet excels at learning explicit mappings between function spaces, making it highly effective when the input and output functions are clearly defined, such as mapping a specific source excitation to the resulting field solution. Its architecture, which separates the branch and trunk networks, allows for rapid inference across a massive number of sensor points once trained. For example, in a parametric study of a microstrip filter, a trained DeepONet can predict the full S-parameter response for 10,000 new geometric variations in under a second, a task that would take a full-wave solver several hours.
Fourier Neural Operator (FNO) takes a fundamentally different approach by learning operators directly in Fourier space, which provides exceptional mesh invariance and zero-shot super-resolution. This results in a model that can be trained on low-resolution simulation data and then evaluated at a much higher resolution without retraining. In a benchmark for scattering parameter prediction, FNO demonstrated a 3x improvement in generalization accuracy when moving from a coarse training mesh to a fine evaluation mesh compared to a standard CNN, making it ideal for designs requiring adaptive mesh refinement.
The key trade-off: If your priority is ultra-fast, real-time inference for a fixed sensor layout with many different input functions, choose DeepONet. If you prioritize mesh invariance, the ability to train on cheap, coarse data and deploy on high-fidelity grids, and superior generalization across resolutions, choose FNO. For CTOs building a digital twin platform that must handle diverse, user-defined geometries without constant retraining, FNO's architecture provides a more robust foundation for a general-purpose EM surrogate.
Why Work With Inference Systems
A balanced breakdown of the key strengths and trade-offs for operator learning in parametric EM design sweeps.
DeepONet: Superior Geometry Generalization
Architecture Advantage: The branch-trunk structure decouples sensor location from input function encoding. This allows a single trained DeepONet to predict fields for arbitrarily varying geometries without retraining, a critical advantage for antenna topology optimization where mesh points shift. Trade-off: Requires careful design of the trunk network to match the output sensor grid.
FNO: Spectral Efficiency & Speed
Computational Advantage: Operates in Fourier space, making it extremely parameter-efficient for learning smooth, global field solutions. FNOs achieve sub-millisecond inference on regular grids, ideal for real-time tuning of filters or impedance matching networks. Trade-off: Struggles with sharp discontinuities and requires interpolation to structured grids, limiting direct use on unstructured meshes common in complex 3D EM components.
DeepONet: Flexible Sensor Placement
Data Advantage: Naturally handles sparse, non-uniform sensor data without interpolation artifacts. This makes it the stronger choice for surrogate modeling where training data comes from irregularly meshed full-wave solvers or physical measurements. Trade-off: Training can be less stable than FNO, often requiring hyperparameter tuning for the balance between branch and trunk learning rates.
FNO: Resolution Invariance
Scaling Advantage: Once trained on a specific resolution, FNOs can zero-shot super-resolve to higher grid densities because they learn continuous functions in Fourier space. This drastically reduces the cost of generating high-fidelity training data. Trade-off: Performance degrades if the underlying physics exhibit high-frequency nonlinearities not captured by the truncated Fourier modes.

About the author
Prasad Kumkar
CEO & MD, Inference Systems
Prasad Kumkar is the CEO & MD of Inference Systems and writes about AI systems architecture, LLM infrastructure, model serving, evaluation, and production deployment. Over 5+ years, he has worked across computer vision models, L5 autonomous vehicle systems, and LLM research, with a focus on taking complex AI ideas into real-world engineering systems.
His work and writing cover AI systems, large language models, AI agents, multimodal systems, autonomous systems, inference optimization, RAG, evaluation, and production AI engineering.
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