mlsanityData to 14 Oct 2026

Rethinking Physics-Informed Regression Beyond Training Loops and Bespoke Architectures

arXiv 2512.13217 ↗First posted 15 Dec 2025math.OC cs.LGcited by 0

Not on the map. Why?

Abstract (arXiv)

We revisit the problem of physics-informed regression, and propose a method that directly computes the state at the prediction point, simultaneously with the derivative and curvature information of the existing samples. We frame each prediction as a constrained optimisation problem, leveraging multivariate Taylor series expansions and explicitly enforcing physical laws. Each individual query can be processed with low computational cost without any pre- or re-training, in contrast to global function approximator-based solutions such as neural networks. Our comparative benchmarks on a reaction-diffusion system show competitive predictive accuracy relative to a neural network-based solution, while completely eliminating the need for long training loops, and remaining robust to changes in the sampling layout.

Key facts. No citing papers in the map yet (data through 14 Oct 2026). Builds on 7 of its 15 references that are in the map. First posted on arXiv 15 Dec 2025.

Builds on

7 of 15 references.

References · 7

  1. 2019DeepONet: Learning nonlinear operators for identifying differential equations based on the universal approximation theorem of operatorscited by 2,018
  2. 2021Solving and Learning Nonlinear PDEs with Gaussian Processescited by 129
  3. 2022When Physics Meets Machine Learning: A Survey of Physics-Informed Machine Learningcited by 65
  4. 2022Physics-Informed Gaussian Process Regression Generalizes Linear PDE Solverscited by 41
  5. 2024Numerical analysis of physics-informed neural networks and related models in physics-informed machine learningcited by 39
  6. 2023A spectrum of physics-informed Gaussian processes for regression in engineeringcited by 14
  7. 2020Physics-informed Gaussian Process for Online Optimization of Particle Acceleratorscited by 7

Built on by

Not cited yet.