đ¤ AI Summary
This work addresses the challenges of slow convergence, training instability, and insufficient accuracy commonly encountered in Physics-Informed Neural Networks (PINNs), which stem from highly anisotropic and rapidly varying loss landscapes. To overcome these issues, the authors propose a lightweight, curvature-aware optimization framework that constructs an inexpensive surrogate for local geometric variations by leveraging secant curvature estimation and continuous gradient difference analysis. An adaptive correction mechanism with step-size normalization is introduced to enhance existing first-order optimizers, without requiring explicit computation of second-order matrices. The method is plug-and-play, computationally efficient, and broadly compatible with standard optimizers. Extensive experiments on high-dimensional and complex dynamical system benchmarksâincluding the heat equation, GrayâScott, BelousovâZhabotinsky, and KuramotoâSivashinsky systemsâdemonstrate significant improvements in convergence speed, training stability, and solution accuracy.
đ Abstract
Physics-Informed Neural Networks (PINNs) often suffer from slow convergence, training instability, and reduced accuracy on challenging partial differential equations due to the anisotropic and rapidly varying geometry of their loss landscapes. We propose a lightweight curvature-aware optimization framework that augments existing first-order optimizers with an adaptive predictive correction based on secant information. Consecutive gradient differences are used as a cheap proxy for local geometric change, together with a step-normalized secant curvature indicator to control the correction strength. The framework is plug-and-play, computationally efficient, and broadly compatible with existing optimizers, without explicitly forming second-order matrices. Experiments on diverse PDE benchmarks show consistent improvements in convergence speed, training stability, and solution accuracy over standard optimizers and strong baselines, including on the high-dimensional heat equation, Gray--Scott system, Belousov--Zhabotinsky system, and 2D Kuramoto--Sivashinsky system.