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Space-Time Continuous PDE Forecasting using Equivariant Neural Fields

NeurIPS 2024 · Probabilistic and scientific modeling › Differential equations and PDEs · approach: Neural PDE solvers · 0 citations (OpenAlex)

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Proposes a space-time continuous PDE solver that models solutions as equivariant latent-space flows of an SE(n)-style equivariant neural field, with meta-learned initial latents, and evaluates on heat, Navier-Stokes, shallow-water and convection PDEs.

Problem

Neural-field-based PDE forecasting ignores known PDE symmetries and boundary conditions, so it generalizes poorly to unseen geometric transformations of initial conditions and to complex geometries such as the sphere, torus and ball.

Approach

Extends equivariant neural fields (ENFs) to PDE-specific symmetry groups (torus translations, S^2 rotations about an axis, SO(3), ball) via custom bi-invariant attributes, models PDE solutions as neural-ODE flows of pose-context latents using log/exp-map message passing, and uses meta-learned initial latents for fast inference.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Add periodic-translation equivariance (ablation)Ours on Navier-Stokes on 𝕋² · Navier-Stokes on 𝕋², 100% observed, t_in testMSE: 2.60{ ±3.16}E-02 -> 1.57{ ±0.09}E-03Helped
Add meta-learning instead of autodecoding (ablation)Ours with 𝕋²/π equivariance on Navier-Stokes · Navier-Stokes on 𝕋², 100% observed, t_in testMSE: 6.75{ ±0.62}E-02 -> 1.57{ ±0.09}E-03Helped
Add periodic-translation equivariance (ablation)Ours on Navier-Stokes on 𝕋² · Navier-Stokes on 𝕋², 50% observed, t_in testMSE: 2.60{ ±3.16}E-02 -> 5.75{ ±2.58}E-03Helped
Add periodic-translation equivariance (ablation)Ours on Navier-Stokes on 𝕋² · Navier-Stokes on 𝕋², 5% observed, t_in testMSE: 7.96{ ±1.65}E-02 -> 3.44{ ±1.43}E-02Helped
Add meta-learning instead of autodecoding (ablation)Ours with 𝕋²/π equivariance on Navier-Stokes · Navier-Stokes on 𝕋², 50% observed, t_in testMSE: 7.01{ ±3.56}E-02 -> 5.75{ ±2.58}E-03Helped
Add meta-learning instead of autodecoding (ablation)Ours with 𝕋²/π equivariance on Navier-Stokes · Navier-Stokes on 𝕋², 5% observed, t_in testMSE: 7.01{ ±3.56}E-02 -> 3.44{ ±1.43}E-02Helped
Use the proposed continuous equivariant solver rather than DINoShallow-water on S² · Shallow-water on S², zero-shot 2× super-resolution, t_in testMSE: 3.37E-04 -> 1.61 { ±0.01}E-04Helped
Use the proposed continuous equivariant solver rather than DINoInternally-heated convection in 𝔹³ · Internally-heated convection in 𝔹³, t_in testMSE: 3.06E-03 -> 5.99{ ±0.15}E-04Helped
Use the proposed continuous equivariant solver rather than DINoShallow-water on S² · Shallow-water on S², train resolution, t_out testMSE: 1.37E-03 -> 1.87{ ±0.04}E-03Hurt

Surprising findings

Limitations

Experimental setup

Datasets: Planar heat diffusion (py-pde) Navier-Stokes on flat 2-torus (py-pde, Gaussian random field ICs) Heat diffusion on S^2 (Dedalus) Global shallow-water equations on S^2 (Dedalus) Internally-heated convection in 3D ball (Dedalus)

Benchmarks: Planar heat diffusion equivariance test Navier-Stokes on T2 Heat diffusion on sphere (data efficiency) Shallow-water on sphere (super-resolution) Internally-heated convection in ball

Metrics: MSE

Baselines: CNODE FNO G-FNO DINo

Builds on: Conditional neural fields for PDE modelling (CNF-ODE / DINo) Equivariant Neural Fields PONITA Meta-SGD Neural ODE

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