Table of Contents
Fetching ...

Neural Parameter Regression for Explicit Representations of PDE Solution Operators

Konrad Mundinger, Max Zimmer, Sebastian Pokutta

TL;DR

Neural Parameter Regression (NPR) addresses learning PDE solution operators across varying initial conditions by combining Hypernetworks with Physics-Informed learning. It parameterizes the output network with a low-rank hidden-weight representation and enforces the initial condition through a reparameterization, enabling efficient, self-supervised operator learning. On 1D heat and Burgers IBVPs, NPR achieves competitive accuracy with Physics-Informed DeepONets and demonstrates strong adaptability to out-of-distribution initial conditions via rapid fine-tuning. This approach offers a scalable path for rapid inference and adaptation in operator learning, with potential for real-time design and control applications, while highlighting limitations in high-dimensional domains and more challenging solution features.

Abstract

We introduce Neural Parameter Regression (NPR), a novel framework specifically developed for learning solution operators in Partial Differential Equations (PDEs). Tailored for operator learning, this approach surpasses traditional DeepONets (Lu et al., 2021) by employing Physics-Informed Neural Network (PINN, Raissi et al., 2019) techniques to regress Neural Network (NN) parameters. By parametrizing each solution based on specific initial conditions, it effectively approximates a mapping between function spaces. Our method enhances parameter efficiency by incorporating low-rank matrices, thereby boosting computational efficiency and scalability. The framework shows remarkable adaptability to new initial and boundary conditions, allowing for rapid fine-tuning and inference, even in cases of out-of-distribution examples.

Neural Parameter Regression for Explicit Representations of PDE Solution Operators

TL;DR

Neural Parameter Regression (NPR) addresses learning PDE solution operators across varying initial conditions by combining Hypernetworks with Physics-Informed learning. It parameterizes the output network with a low-rank hidden-weight representation and enforces the initial condition through a reparameterization, enabling efficient, self-supervised operator learning. On 1D heat and Burgers IBVPs, NPR achieves competitive accuracy with Physics-Informed DeepONets and demonstrates strong adaptability to out-of-distribution initial conditions via rapid fine-tuning. This approach offers a scalable path for rapid inference and adaptation in operator learning, with potential for real-time design and control applications, while highlighting limitations in high-dimensional domains and more challenging solution features.

Abstract

We introduce Neural Parameter Regression (NPR), a novel framework specifically developed for learning solution operators in Partial Differential Equations (PDEs). Tailored for operator learning, this approach surpasses traditional DeepONets (Lu et al., 2021) by employing Physics-Informed Neural Network (PINN, Raissi et al., 2019) techniques to regress Neural Network (NN) parameters. By parametrizing each solution based on specific initial conditions, it effectively approximates a mapping between function spaces. Our method enhances parameter efficiency by incorporating low-rank matrices, thereby boosting computational efficiency and scalability. The framework shows remarkable adaptability to new initial and boundary conditions, allowing for rapid fine-tuning and inference, even in cases of out-of-distribution examples.
Paper Structure (20 sections, 15 equations, 4 figures, 2 tables, 1 algorithm)

This paper contains 20 sections, 15 equations, 4 figures, 2 tables, 1 algorithm.

Figures (4)

  • Figure 1: The proposed architecture: The Hypernetwork $H_\Phi$ maps an initial condition to another function parametrized by $T_{H_\Phi}$, hence approximating a mapping between function spaces.
  • Figure 2: The heat equation: The first and second row correspond to $u_0(x) = 0.5 \sin(4 \pi x) + \cos(2 \pi x)+ 0.3 \cos(6 \pi x) + 0.8$ and the $u_0(x) = \sum_{n=1}^3 (\sin(n \pi x) + \cos(n \pi x)) + 1$, respectively. The columns shows the reference solutions, the results of and the absolute differences, respectively.
  • Figure 3: The heat equation with the out-of-distribution condition $u_0(x) = 5x + 3 \sin(4 \pi x)$. We plot the reference solution (left), the absolute difference to the reference solution before fine-tuning (middle) and after fine-tuning (right).
  • Figure 4: The Burgers equation: The first row shows the results for the initial condition $u_0(x) = -0.9x + 1.1$ and the second row for $u_0(x) = -0.2x + 1.8$.