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CoPINN: Cognitive Physics-Informed Neural Networks

ICML 2025 · Probabilistic and scientific modeling › Differential equations and PDEs · approach: Physics-informed neural network training

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Proposes CoPINN, a separable-subnetwork PINN that weights collocation points by PDE-residual-gradient difficulty and schedules training from easy to hard via a cognitive (self-paced) scheduler, outperforming seven PINN baselines on PDE benchmarks.

Problem

Standard PINNs treat easy and hard collocation points equally, so errors concentrate near physical boundaries, causing unstable learning, poor local minima and an "Unbalanced Prediction Problem" (UPP).

Approach

Combines SPINN-style separable per-axis subnetworks with a self-paced learning scheme that measures each collocation point's difficulty by the gradient of the PDE residual and linearly shifts sample weights from easy to hard over training epochs.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Use CoPINN instead of SPINN (m)Helmholtz · Helmholtz, Nc=323RL2: 0.0595 -> 0.0050Helped
Use CoPINN instead of SPINN (m)(2+1)-d Klein-Gordon · (2+1)-d Klein-Gordon, Nc=323RL2: 0.0020 -> 0.0006Helped
Use CoPINN instead of SPINN (m)(3+1)-d Klein-Gordon · (3+1)-d Klein-Gordon, Nc=323RL2: 0.0065 -> 0.0027Helped
Use CoPINN instead of FPINNDiffusion · Diffusion, Nc=323RL2: 0.0048 -> 0.0038Helped
Use CoPINN instead of SPINN (m)Flow-mixing 3D · Flow-mixing 3D, Nc=323RL2: 0.0263 -> 0.0230Helped
Apply CoPINN difficulty evaluation and cognitive training scheduler to PINNPINN · Convection, ξ=30 and ξ=50RL2: ξ=30: 0.0160 -> 0.0055; ξ=50: 0.5471 -> 0.5811Mixed
Add cognitive training scheduler instead of using the original loss function (ablation)CoPINN · (2+1)-d Klein-Gordon, Nc=323RL2: 0.0020 -> 0.0006Helped
Add the epoch change component to the scheduler (ablation)CoPINN without epoch change component · (2+1)-d Klein-Gordon, Nc=323RL2: 0.0027 -> 0.0006Helped
Add the sample change component to the scheduler (ablation)CoPINN without sample change component · (2+1)-d Klein-Gordon, Nc=323RL2: 0.0010 -> 0.0006Helped

Surprising findings

Limitations

Experimental setup

Datasets: Helmholtz equation (manufactured solution) Diffusion equation (FEniCS reference, 101^3) (2+1)-d Klein-Gordon (3+1)-d Klein-Gordon (2+1)-d Flow Mixing 1D Convection equation

Benchmarks: Helmholtz Diffusion (2+1)-d Klein-Gordon (3+1)-d Klein-Gordon Flow-mixing 3D 1D Convection

Metrics: Relative L2 error RMSE improvement percentage

Baselines: PINN gPINN SPINN SPINN(m) AHD-PINN RoPINN FPINN

Builds on: PINN SPINN self-paced learning gPINN RoPINN

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