🤖 AI Summary
Operator learning on multi-resolution irregular meshes faces challenges of scarce high-quality labeled data and inconsistent sample resolutions.
Method: This paper proposes a physics-informed, data-free neural operator framework. It extends the RINO architecture to a fully unsupervised setting: pre-trained basis functions encode arbitrarily discretized inputs into a latent space; an MLP models the operator mapping; and PDE constraints—formulated via finite differences—are embedded directly into the loss function as hard physical priors.
Contribution/Results: The framework requires no input-output paired data. It significantly improves generalization and robustness across mixed coarse–fine meshes. In multiple multi-resolution numerical experiments—including Poisson, Darcy flow, and Navier–Stokes problems—the model stably predicts physical fields with accuracy comparable to traditional PDE solvers, while drastically reducing dependence on high-fidelity labeled datasets.
📝 Abstract
The predictive accuracy of operator learning frameworks depends on the quality and quantity of available training data (input-output function pairs), often requiring substantial amounts of high-fidelity data, which can be challenging to obtain in some real-world engineering applications. These datasets may be unevenly discretized from one realization to another, with the grid resolution varying across samples. In this study, we introduce a physics-informed operator learning approach by extending the Resolution Independent Neural Operator (RINO) framework to a fully data-free setup, addressing both challenges simultaneously. Here, the arbitrarily (but sufficiently finely) discretized input functions are projected onto a latent embedding space (i.e., a vector space of finite dimensions), using pre-trained basis functions. The operator associated with the underlying partial differential equations (PDEs) is then approximated by a simple multi-layer perceptron (MLP), which takes as input a latent code along with spatiotemporal coordinates to produce the solution in the physical space. The PDEs are enforced via a finite difference solver in the physical space. The validation and performance of the proposed method are benchmarked on several numerical examples with multi-resolution data, where input functions are sampled at varying resolutions, including both coarse and fine discretizations.