π€ AI Summary
To address the reliance of operator learning on costly high-fidelity simulation data for dissipative partial differential equations (PDEs), this paper proposes DOOLβan unsupervised operator learning framework grounded in the Onsager variational principle, with Rayleighian functional minimization as its optimization objective and no requirement for labeled data. DOOL introduces a spatiotemporal decoupled architecture: a trunk network encodes only spatial coordinates, while an explicit time integrator enforcing physical conservation laws enables efficient training and long-term extrapolation. Notably, it is the first work to extend the Onsager framework to non-standard second-order dissipative wave systems. Experiments demonstrate that DOOL significantly outperforms supervised DeepONet and MIONet on canonical dissipative PDEs, achieving superior accuracy, strong generalization across domains and parameters, and high computational efficiency.
π Abstract
Existing operator learning methods rely on supervised training with high-fidelity simulation data, introducing significant computational cost. In this work, we propose the deep Onsager operator learning (DOOL) method, a novel unsupervised framework for solving dissipative equations. Rooted in the Onsager variational principle (OVP), DOOL trains a deep operator network by directly minimizing the OVP-defined Rayleighian functional, requiring no labeled data, and then proceeds in time explicitly through conservation/change laws for the solution. Another key innovation here lies in the spatiotemporal decoupling strategy: the operator's trunk network processes spatial coordinates exclusively, thereby enhancing training efficiency, while integrated external time stepping enables temporal extrapolation. Numerical experiments on typical dissipative equations validate the effectiveness of the DOOL method, and systematic comparisons with supervised DeepONet and MIONet demonstrate its enhanced performance. Extensions are made to cover the second-order wave models with dissipation that do not directly follow OVP.