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Finsler-Laplace-Beltrami Operators with Application to Shape Analysis

CVPR 2024 · Probabilistic and scientific modeling › Molecules and proteins · approach: Sparse graphical and tensor models · 9 citations (OpenAlex)

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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

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Use FLBO (τ = 0.1) instead of ACSCNNShape correspondence · FAUST RemeshedAccuracy (r = 0): 61.95 -> 62.61Helped
Use FLBO (τ = 0.1) instead of ACSCNNShape correspondence · SCAPE RemeshedAccuracy (r = 0): 46.13 -> 46.94Helped
Vary τ from 0.1 to 0.2 (ablation)FLBO shape correspondence · FAUST RemeshedAccuracy (r = 0): 62.61 -> 62.58No clear effect
Vary τ from 0.1 to 0.3 (ablation)FLBO shape correspondence · FAUST RemeshedAccuracy (r = 0): 62.61 -> 62.67No clear effect
Vary τ from 0.1 to 0.4 (ablation)FLBO shape correspondence · SCAPE RemeshedAccuracy (r = 0): 46.94 -> 45.82Hurt
Vary τ from 0.1 to 0.5 (ablation)FLBO shape correspondence · SCAPE RemeshedAccuracy (r = 0): 46.94 -> 45.26Hurt
Vary τ from 0.1 to 0.2 (ablation)FLBO shape correspondence · SHREC’16 Partial CutsAccuracy (r = 0): Cat: 40.13 -> 37.72; Dog: 59.31 -> 60.02Mixed
Vary τ from 0.1 to 0.3 (ablation)FLBO shape correspondence · SHREC’16 Partial CutsAccuracy (r = 0): Cat: 40.13 -> 40.26; Michael: 16.04 -> 13.15Mixed
Vary τ from 0.1 to 0.4 (ablation)FLBO shape correspondence · SHREC’16 Partial CutsAccuracy (r = 0): Cat: 40.13 -> 39.63; Horse: 42.72 -> 44.83Mixed
Vary τ from 0.1 to 0.5 (ablation)FLBO shape correspondence · SHREC’16 Partial CutsAccuracy (r = 0): Cat: 40.13 -> 40.94; Victoria: 27.95 -> 28.46Mixed
Vary τ from 0.1 to 0.2 (ablation)FLBO shape correspondence · SHREC’16 Partial HolesAccuracy (r = 0): Cat: 19.95 -> 17.99; Horse: 47.87 -> 49.77Mixed
Vary τ from 0.1 to 0.3 (ablation)FLBO shape correspondence · SHREC’16 Partial HolesAccuracy (r = 0): Cat: 19.95 -> 21.27; Michael: 12.00 -> 11.31Mixed

Surprising findings

Limitations

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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