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Physics-Informed Error Field Learning: A Post-Training Optimization Framework for Physics-Informed Neural Networks

Jiuyun Sun, Yong Zhang

arXiv:2608.24970v1cs.LG

TL;DR

PINNs often yield diminishing accuracy gains at late training stages despite rising computational costs. PIEFL learns a physically constrained error field with an auxiliary network, and experiments show improved accuracy with lower computational costs.

  • Problem

    Late-stage PINN optimization often produces diminishing accuracy improvements while computational costs continue to increase.

  • Method

    PIEFL fixes an accurate primary network, derives physics-based error equations, and trains an auxiliary network to learn and correct its prediction errors.

  • Results

    Across representative PDE problems, PIEFL further reduces prediction errors and improves final-solution accuracy compared with continuous conventional PINN training.

  • Takeaways & Limitations

    PIEFL offers a computationally efficient, architecture-compatible late-stage optimization strategy that can integrate with existing PINN techniques.

Abstract

from arXiv · show

Physics-Informed Neural Networks (PINNs) have emerged as an important class of numerical methods for solving partial differential equations (PDEs). However, during the late-stage optimization process, further parameter updates often yield diminishing accuracy improvements while increasing computational costs. To address this issue, this paper proposes a Physics-Informed Error Field Learning (PIEFL) framework for PINNs. Unlike conventional approaches that continuously approximate the solution field using a single network, PIEFL introduces an auxiliary error network after the primary network achieves satisfactory accuracy and shifts the learning objective from the solution field to the error field. By deriving error control equations under physical constraints, the error network learns the discrepancy between the current approximation and the exact solution, and the learned error correction is combined with the primary prediction to improve solution accuracy. The proposed framework avoids continuous optimization of the entire solution space and focuses computational resources on correcting existing prediction errors. Moreover, PIEFL requires no modification to the primary network architecture, making it compatible with existing PINN models and applicable as a general post-training optimization strategy. Numerical experiments on representative PDEs demonstrate that PIEFL achieves higher solution accuracy under the same computational budget, validating its effectiveness in improving the performance of PINNs.

1. Introduction

PINNs face efficiency, stability, and precision challenges, especially when late-stage training produces diminishing accuracy gains at rising computational cost. PIEFL addresses this bottleneck by learning physics-constrained error fields after primary-network training, improving accuracy without changing the PINN architecture.

  • PINNs face challenges in computational efficiency, training stability, and achieving high-precision PDE solutions.
  • Late-stage parameter optimization often yields diminishing solution-accuracy improvements while computational costs continue increasing.The primary network has typically captured the target solution’s overall structure by this stage.
  • PIEFL shifts post-training optimization from continuously learning the solution field to independently learning the existing prediction’s error field.The framework first trains a primary network, then introduces an auxiliary error network once satisfactory accuracy is reached.
  • PIEFL provides an efficient late-stage correction strategy that reduces prediction errors with lower computational costs and marginal additional overhead.It focuses resources on correcting existing errors rather than continuously optimizing a nearly converged solution network.
  • PIEFL requires no modification to existing PINN architectures and is compatible with architecture improvements, adaptive sampling, and loss weighting strategies.Representative PDE experiments report higher solution accuracy with lower computational costs than continuous training strategies.
  • Physics-based error control equations impose the original system’s physical constraints on the error-learning process.These equations are derived from the physical constraints satisfied by the error field.

2. Methodology

PIEFL extends standard PINNs with a cascaded two-stage architecture: a primary network first approximates the PDE solution, then a fixed-primary error network learns a physically constrained correction. The final prediction combines the primary approximation with the learned error field, whose output may be amplified by a scaling coefficient.

  • Standard PINNs: Standard PINNs combine initial/boundary-condition data loss MSEu with physical loss MSEf enforcing PDE constraints at collocation points.MSEu measures initial and boundary conditions, while MSEf enforces the physical residual on collocation points.
  • Primary network: PIEFL uses a cascaded architecture in which a primary network first produces an approximate PDE solution satisfying physical laws and IC/BC constraints.The primary network shares the input configuration and loss function of standard PINNs and outputs the initial prediction up and residual fp.
  • Error network: After the primary parameters are fixed, an error network learns a physically constrained error field ue from the preliminary solution information.The predicted solution up and residual fp provide information and physical residual constraints for subsequent error correction.
  • Error-field formulation: The error-field formulation rewrites the solution as u = up + ue and derives a governing equation, physical residual, and loss for the error network.The error initial and boundary conditions are obtained by subtracting the primary prediction up from the original IC/BC.
  • Final prediction: PIEFL forms its final prediction by combining the primary output with the error-network output, using scaling coefficient α to amplify typically small errors.The coefficient α reduces the difficulty of learning the error field.

3. Numerical Experiments

Numerical experiments on the KdV and nonlinear Schrödinger equations show that PIEFL improves PINN accuracy by learning and correcting the primary network’s error field. The framework achieves substantial error reductions while retaining compatibility with standard PINN comparisons.

  • Experimental design: Experiments compare standard PINNs and PIEFL on three representative PDEs using relative 𝕃2 error as the evaluation metric.The PDEs are the KdV, nonlinear Schrödinger, and (2+1)-dimensional KP equations.
  • KdV equation: For the KdV equation, PIEFL reduces the primary network’s relative error from 3.846063e−3 to 1.469116e−4, versus 9.480554e−4 for the baseline PINN.The error network’s relative error is 1.659345e−2, while its learned correction substantially improves the final prediction.
  • Results visualization: Visual results for the KdV and nonlinear Schrödinger cases show that PIEFL learns the primary PINN’s error field and supplies accurate corrections while both models solve the PDEs accurately.The figures present predicted solutions, error distributions, and correction fields.
  • KdV equation: During KdV training, PIEFL initially has slightly higher error but begins decreasing more rapidly at approximately 6500 iterations as the error network learns the remaining discrepancy.The reported trends indicate that improved error-field learning is linked to improved final-solution accuracy.
  • Nonlinear Schrödinger equation: For one-soliton and two-soliton nonlinear Schrödinger solutions, PIEFL reduces relative 𝕃2 errors to 8.745380e−5 and 3.573394e−4, achieving ERRs of 95.22% and 91.49%.The corresponding primary-network errors are 2.773287e−3 and 1.086328e−2.

4. Conclusion

PIEFL improves late-stage PINN efficiency by shifting learning from the solution field to an independently learned error field after the primary network reaches high accuracy. Validation on representative PDEs shows additional error correction can reduce prediction errors, while the framework remains compatible with existing PINN architectures and optimization strategies.

  • Framework contribution: PIEFL introduces an independent error network after the primary network achieves high accuracy, shifting the learning objective from the complete solution field to the error field.This changes the optimization target rather than continuously training a single network to approximate the full solution.
  • Numerical validation: PIEFL further reduces prediction errors through additional error correction compared with continuous training strategies on the KdV, nonlinear Schrödinger, and KP equations.The framework was validated on several representative PDE problems.
  • Compatibility and efficiency: PIEFL requires no modifications to existing PINN architectures and can integrate with architecture enhancement, adaptive sampling, and loss balancing strategies.The method improves efficiency by modifying the learning objective instead of continuously increasing the original solution network’s optimization cost.
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