Neural Operators
Overview
Neural operators learn maps from input fields, parameters, or geometries to output fields, often approximating the solution map of a partial differential equation. DeepONet uses branch and trunk networks, Fourier Neural Operators learn interactions in spectral space, and graph and transformer operators handle irregular meshes and complex geometries; physics-informed losses and structure-preserving designs add physical constraints. These models can make repeated simulation, forecasting, and inverse design much faster than running a numerical solver for every case. A central challenge is making predictions reliable across new resolutions, geometries, and physical regimes while preserving stability over long rollouts and matching classical solvers when high accuracy is required.
Latest papers
313 papers52 papers in the last four weeks, up 24% on the four weeks before. 0.3% of all new papers.
Neural-Schwarz Tiling for Geometry-Universal PDE Solving at Scale
Approximation Theory of Laplacian-Based Neural Operators for Reaction-Diffusion System
NOFE - Neural Operator Function Embedding
Compositional Neural Operators for Multi-Dimensional Fluid Dynamics
Don't Fix the Basis -- Learn It: Spectral Representation with Adaptive Basis Learning for PDEs
jNO: A JAX Library for Neural Operator and Foundation Model Training
HS-FNO: History-Space Fourier Neural Operator for Non-Markovian Partial Differential Equations
Bridging Spectral Operator Learning and U-Net Hierarchies: SpectraNet for Stable Autoregressive PDE Surrogates
CATO: Charted Attention for Neural PDE Operators
Neural Operators as Efficient Function Interpolators
QuadNorm: Resolution-Robust Normalization for Neural Operators
One Operator for Many Densities: Amortized Approximation of Conditioning by Neural Operators
Do Neural Operators Forget Geometry? The Forgetting Hypothesis in Deep Operator Learning
A Robust Foundation Model for Conservation Laws: Injecting Context into Flux Neural Operators via Recurrent Vision Transformers
Hybrid Iterative Neural Low-Regularity Integrator for Nonlinear Dispersive Equations
Replay-Based Continual Learning for Physics-Informed Neural Operators
GRIFDIR: Graph Resolution-Invariant FEM Diffusion Models in Function Spaces over Irregular Domains
Isotropic Fourier Neural Operators
ZNO: Stable Rational Neural Operators in the Z-Domain for Discrete-Time Dynamics
An ALE-Consistent Graph Neural Operator-Transformer Framework for Fluid-Structure Interaction
RETO: A Rotary-Enhanced Transformer Operator for High-Fidelity Prediction of Automotive Aerodynamics
Learning Neural Operator Surrogates for the Black Hole Accretion Code
BHAC). First, a Physics Informed Fourier Neural Operator (PINO) is trained on the special-relativistic resistive MHD (SRRMHD) evolution of the Orszag-Tang vortex over a range of resistivities spanning the Sweet-Parker and fast reconnection regimes. By embedding the governing equations as an additional loss term evaluated at finer temporal resolution than the available data supervision, the model learns dynamics at time steps where no simulation data is provided, enabling recovery of plasmoid formation that a data-only baseline trained on the same sparse snapshots fails to reproduce. To our knowledge, the present work is the first application of a physics informed neural operator to special relativistic resistive MHD, and the first to investigate the capability of such models to resolve plasmoid formation in SRRMHD. In a second line of investigation, an OFormer-style Transformer Neural Operator is trained on the evolution of spine-sheath relativistic jets created with BHAC, in special-relativistic MHD (SRMHD). The model is directly applied on the adaptive mesh, highlighting the need for linear attention due to long sequences. The neural surrogate model is capable of capturing most of the major details, especially in early predictions. To our knowledge, this constitutes the first application of a neural operator directly on a high resolution adaptive mesh refinement grid in the context of MHD simulations.