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AMR-Transformer: Enabling Efficient Long-range Interaction for Complex Neural Fluid Simulation
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Proposes AMR-Transformer, which tokenizes fluid fields with a physics-constrained adaptive mesh refinement (quadtree) and feeds the tokens to an encoder-only Transformer solver to model long-range interactions efficiently.
Problem
Neural CFD surrogates struggle to capture long-range dependencies (e.g., shockwaves, turbulence) with CNN/GNN receptive-field limits, while Transformers' O(N^2) attention over all grid cells is too costly at high resolution.
Approach
Use a hierarchical multi-way-tree adaptive mesh refinement as a tokenizer, with a Navier-Stokes-aware pruning module (velocity gradient, vorticity, momentum, Kelvin-Helmholtz shear) deciding which regions are subdivided, so a Transformer attends over a small set of multi-scale patches.
Key results
- On the Dam problem, MSE drops to 1.63E-4 versus 1.64E-3 for DeepONet (about 91% relative improvement).
- On the Shock problem, NMSE of 9.32E-4 beats FNO's 5.53E-3 (about 83% improvement).
- AMR tokenizer reduces token count by roughly 60-70% and FLOPs by 70-75% on CFDBench, reaching up to about 60x FLOPs reduction versus ViT.
Measured effects reported in the paper
| What was changed | Where | Measured | Effect |
|---|---|---|---|
| Use AMR-Transformer instead of DeepONet | Dam simulation · Dam | MSE: 1.64E-3 -> 1.63E-4 | Helped |
| Use AMR-Transformer instead of FNO | Cylinder simulation · Cylinder | MSE: 2.74E-5 -> 2.09E-5 | Helped |
| Use AMR-Transformer instead of U-Net | Cavity simulation · Cavity | MSE: 1.58E-2 -> 4.71E-3 | Helped |
| Use AMR-Transformer instead of U-Net | Tube simulation · Tube | MSE: 1.29E-3 -> 1.33E-3 | Hurt |
| Use AMR-Transformer instead of FNO | Shockwave simulation · Shockwave | MSE: 4.83E-3 -> 9.66E-4 | Helped |
| Use AMR-Transformer instead of FNO | Diffusion-Reaction · Diffusion-Reaction | MSE: 1.76E-2 -> 1.75E-2 | Helped |
| Use AMR-Transformer instead of DeepONet | NS-Incom-Inhom simulation · NS-Incom-Inhom | MSE: 5.88E-6 -> 3.76E-6 | Helped |
| Use AMR tokenizer instead of a regular tokenizer | Shockwave Transformer · Shockwave | GFLOPs: 71.37 -> 7.51 | Helped |
| Use only velocity-gradient pruning instead of all physical criteria (ablation) | AMR-Transformer on Dam · Dam | MSE: 1.63E-4 -> 2.80E-4 | Hurt |
| Use only vorticity pruning instead of all physical criteria (ablation) | AMR-Transformer on Dam · Dam | MSE: 1.63E-4 -> 1.93E-3 | Hurt |
| Use only momentum pruning instead of all physical criteria (ablation) | AMR-Transformer on Dam · Dam | MSE: 1.63E-4 -> 1.12E-3 | Hurt |
| Use only Kelvin-Helmholtz instability pruning instead of all physical criteria (ablation) | AMR-Transformer on Dam · Dam | MSE: 1.63E-4 -> 5.40E-4 | Hurt |
Surprising findings
- The Identity baseline outperforms FNO on the Dam problem in MAE, and DeepONet is close to Identity on Cylinder and Dam.
- Individual physical pruning criteria alone give worse accuracy than the combined criteria, and FNO (1.00 NMSE) fails on NS-Incom-Inhom.
Limitations
- Shockwave dataset is small (10 cases) and at 128x128 resolution.
- Pruning thresholds are sampled randomly and tuned post-training; the paper provides limited theoretical justification for the criteria.
- Several reported comparisons rely on baseline configurations taken from CFDBench with no mention of ablating the tokenizer on the other baselines.
Experimental setup
Datasets: CFDBench PDEBench Shockwave (new)
Benchmarks: CFDBench PDEBench Shockwave
Metrics: NMSE MAE MSE GFLOPs token count
Baselines: U-Net FNO DeepONet MeshGraphNet ViT Identity
Builds on: Vision Transformer MeshGraphNet Fourier Neural Operator DeepONet
Closest papers by meaning
- Transolver++: An Accurate Neural Solver for PDEs on Million-Scale Geometries (ICML 2025 · similarity 0.80)
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