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Finsler-Laplace-Beltrami Operators with Application to Shape Analysis
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Derives a Finsler heat kernel from Randers-metric Finsler heat diffusion and a Finsler-Laplace-Beltrami operator (FLBO), then plugs it into ACSCNN-style spectral anisotropic convolutions for shape correspondence.
Problem
Anisotropic Laplace-Beltrami operators used in geometric deep learning for shape correspondence are heuristically designed and lack theoretical justification; the paper asks whether Finsler geometry offers a principled generalization.
Approach
Starting from the Finsler heat equation with a Randers metric and a short-time simplification with small asymmetry omega, the homogeneous part yields an anisotropic diffusion operator (FLBO) whose diffusivity is the dual Randers metric's Finsler diffusivity; this is discretized on triangle meshes and used as the basis of spectral anisotropic convolutions.
Key results
- On FAUST Remeshed, the FLBO variant with tau=0.3 reaches 62.67% accuracy at r=0 versus 61.95% for ACSCNN.
- On SCAPE Remeshed, tau=0.1 reaches 46.94% at r=0 versus 46.13% for ACSCNN.
- On SHREC'16 Partial Cuts the method is on par with or better than ACSCNN for default tau=0.1 (mixed per-category results, e.g. Michael 16.04 vs 12.82).
Measured effects reported in the paper
| What was changed | Where | Measured | Effect |
|---|---|---|---|
| Use FLBO (τ = 0.1) instead of ACSCNN | Shape correspondence · FAUST Remeshed | Accuracy (r = 0): 61.95 -> 62.61 | Helped |
| Use FLBO (τ = 0.1) instead of ACSCNN | Shape correspondence · SCAPE Remeshed | Accuracy (r = 0): 46.13 -> 46.94 | Helped |
| Vary τ from 0.1 to 0.2 (ablation) | FLBO shape correspondence · FAUST Remeshed | Accuracy (r = 0): 62.61 -> 62.58 | No clear effect |
| Vary τ from 0.1 to 0.3 (ablation) | FLBO shape correspondence · FAUST Remeshed | Accuracy (r = 0): 62.61 -> 62.67 | No clear effect |
| Vary τ from 0.1 to 0.4 (ablation) | FLBO shape correspondence · SCAPE Remeshed | Accuracy (r = 0): 46.94 -> 45.82 | Hurt |
| Vary τ from 0.1 to 0.5 (ablation) | FLBO shape correspondence · SCAPE Remeshed | Accuracy (r = 0): 46.94 -> 45.26 | Hurt |
| Vary τ from 0.1 to 0.2 (ablation) | FLBO shape correspondence · SHREC’16 Partial Cuts | Accuracy (r = 0): Cat: 40.13 -> 37.72; Dog: 59.31 -> 60.02 | Mixed |
| Vary τ from 0.1 to 0.3 (ablation) | FLBO shape correspondence · SHREC’16 Partial Cuts | Accuracy (r = 0): Cat: 40.13 -> 40.26; Michael: 16.04 -> 13.15 | Mixed |
| Vary τ from 0.1 to 0.4 (ablation) | FLBO shape correspondence · SHREC’16 Partial Cuts | Accuracy (r = 0): Cat: 40.13 -> 39.63; Horse: 42.72 -> 44.83 | Mixed |
| Vary τ from 0.1 to 0.5 (ablation) | FLBO shape correspondence · SHREC’16 Partial Cuts | Accuracy (r = 0): Cat: 40.13 -> 40.94; Victoria: 27.95 -> 28.46 | Mixed |
| Vary τ from 0.1 to 0.2 (ablation) | FLBO shape correspondence · SHREC’16 Partial Holes | Accuracy (r = 0): Cat: 19.95 -> 17.99; Horse: 47.87 -> 49.77 | Mixed |
| Vary τ from 0.1 to 0.3 (ablation) | FLBO shape correspondence · SHREC’16 Partial Holes | Accuracy (r = 0): Cat: 19.95 -> 21.27; Michael: 12.00 -> 11.31 | Mixed |
Surprising findings
- Performance is largely insensitive to the Finsler asymmetry hyperparameter tau, with results remaining consistent across tau from 0.1 to 0.5.
Limitations
- Derivation relies on strong assumptions, including small asymmetry omega and a short-time simplification with a specific initialization.
- Discretization is straightforward and only one choice of metric (M, omega) is explored.
- Gains over ACSCNN are often small and within noise across settings.
Experimental setup
Datasets: FAUST Remeshed SCAPE Remeshed SHREC'16 Partial Cuts SHREC'16 Partial Holes
Benchmarks: FAUST Remeshed SCAPE Remeshed SHREC'16 Partial Cuts SHREC'16 Partial Holes
Metrics: accuracy within r geodesic radius (Princeton benchmark proto
Baselines: FieldConv ACSCNN
Builds on: ACSCNN anisotropic Laplace-Beltrami operator FieldConv Finsler heat equation
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