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arxiv: 2605.24390 · v1 · pith:HRWRMF3Dnew · submitted 2026-05-23 · 💻 cs.LG

Learning Laplacian Eigenspace with Mass-Aware Neural Operators on Point Clouds

Pith reviewed 2026-06-30 14:47 UTC · model grok-4.3

classification 💻 cs.LG
keywords Laplace-Beltrami operatorpoint cloudsneural operatorseigenspaceRayleigh-Ritz refinementspectral geometrymass-aware attention
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The pith

NEO learns a redundant basis for the low-frequency eigenspace of the Laplace-Beltrami operator on point clouds, recovering eigenpairs via Rayleigh-Ritz refinement.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper introduces the Neural Eigenspace Operator to predict the spectrum of the Laplace-Beltrami operator directly from point clouds, amortizing the expense of iterative solvers. Rather than regressing individual eigenvectors that suffer from sign flips and rotation ambiguities, the network learns the stable low-frequency subspace by outputting a redundant set of basis functions whose span covers the target eigenspace. A mass-aware attention mechanism adds per-point area weights to handle irregular sampling, yielding robustness to non-uniform densities and zero-shot generalization across resolutions. The approach produces near-linear runtime scaling and speedups while supplying eigenpairs for spectral geometry tasks and raw basis functions for downstream learning.

Core claim

The Neural Eigenspace Operator (NEO) is a feed-forward framework that predicts a redundant set of basis functions whose span robustly covers the target low-frequency eigenspace of the Laplace-Beltrami operator on point clouds. Accurate eigenpairs are recovered via lightweight Rayleigh-Ritz refinement. The mass-aware neural operator incorporates per-point area weights into attention-based aggregation, improving robustness to non-uniform densities and enabling zero-shot generalization across resolutions.

What carries the argument

Mass-aware neural operator that incorporates per-point area weights into attention-based aggregation to predict a redundant basis spanning the target LBO eigenspace.

If this is right

  • Enables near-linear runtime scaling for eigenmode computation on large point clouds.
  • Delivers substantial wall-clock speedups over iterative solvers at comparable accuracy.
  • Supports zero-shot transfer to high-resolution point clouds without retraining.
  • Yields raw basis functions that serve as effective point-wise features for downstream tasks.
  • Produces eigenpairs usable in standard spectral geometry applications.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The feed-forward prediction could support real-time spectral analysis inside interactive 3D modeling or simulation pipelines.
  • The redundant-basis strategy for avoiding eigenvector ambiguities might transfer to other spectral problems on graphs or meshes.
  • Evaluating performance on scanned real-world objects with natural density variations would test practical robustness beyond synthetic data.

Load-bearing premise

Incorporating per-point area weights into attention-based aggregation will improve robustness to non-uniform densities and enable zero-shot generalization across resolutions.

What would settle it

Running NEO on a point cloud with strongly varying local densities and measuring whether the recovered eigenpairs match those from a standard iterative solver on the corresponding surface mesh within a small tolerance.

Figures

Figures reproduced from arXiv: 2605.24390 by Ligang Liu, Tao Du, Zherui Yang.

Figure 1
Figure 1. Figure 1: We present NEO, a neural framework that accelerates Laplace–Beltrami spectral analysis by predicting the low-frequency eigenspace directly from raw [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Ambiguities in LBO eigenspace computation. Eigenfunctions are not uniquely defined: each mode is determined only up to a global sign, and repeated (or nearly repeated) eigenvalues admit arbitrary orthogonal bases within the same eigenspace. Consequently, equally valid eigensolvers (or the same solver under small numerical perturbations) may return differ￾ent eigenvector bases for the same shape (A vs. B), … view at source ↗
Figure 5
Figure 5. Figure 5: Visualization of NEO predictions on our OOD test dataset. The collection encompasses a wide spectrum of semantic categories, ranging from organic creatures and classic graphics models to man-made CAD parts. It also includes diverse topologies and structural variations, from genus-0 solids to high-genus shapes with holes and thin structures, stressing robustness beyond the training distribution [PITH_FULL_… view at source ↗
Figure 6
Figure 6. Figure 6: (Left) shows that NEO achieves low mean span loss Espan, indicating the basis successfully captures the target low-frequency spectral energy. Leveraging this subspace, Rayleigh–Ritz effectively recovers eigenpairs: the eigenvectors and eigenvalues exhibit low error ( [PITH_FULL_IMAGE:figures/full_fig_p006_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: Robustness to Non-Uniform Sampling. We visualize recovered eigenvectors (10th-12th modes) under varying sampling density biases, ranging from highly non-uniform (top) to uniform (bottom). While the mass-agnostic baseline fails under biased sampling—often overfitting to high-density regions (high MSE)—our mass-aware approach consistently matches the ground truth. This confirms that injecting mass weights ef… view at source ↗
Figure 8
Figure 8. Figure 8: Resolution scaling and discretization transfer. We compare NEO’s predicted eigenfunctions (modes 2, 4, 32) against Ground Truth across varying resolutions (2k to 1.6M points) and distinct Laplacian discretizations (Mesh vs. 𝑘-NN). Despite being trained only on coarse 2k point clouds, NEO demonstrates strong zero-shot generalization. While minor deviations become visible in higher frequencies (e.g., 32nd mo… view at source ↗
Figure 11
Figure 11. Figure 11: Fast Poisson solve in the heat-based geodesic computation. Left: Heat geodesic distances. Middle & Right: Convergence of the Poisson step. Using NEO’s predicted eigenpairs as the coarse level in an additive two-level preconditioner (Ours) reduces both the iteration count (∼ 3×) and total wall-clock time compared to the standard ICPCG baseline. Few-shot classification. We evaluate on SHREC-11 [Lian et al. … view at source ↗
Figure 10
Figure 10. Figure 10: , NEO yields visually comparable dense correspondences and preserves semantic part transfer. On the FAUST dataset, us￾ing NEO’s predicted eigenpairs increases the mean geodesic error from 0.438 to 0.543, which remains sufficient for downstream shape matching applications. Accelerated geodesic distances. We use NEO to accelerate heat￾based geodesic distances [Crane et al. 2017] by speeding up the Poisson s… view at source ↗
Figure 13
Figure 13. Figure 13: NEO as an intrinsic point embedding. We use the raw predicted subspace 𝐹 directly as point features without explicit eigensolving, comparing it against NeRF-style positional encoding (NeRF-PE) baselines. (a) For classification, frozen NEO features enable a lightweight PointNet to achieve perfect accuracy, surpassing heavier end-to-end baselines (e.g., PointTransformer). (b) For dense segmentation, NEO’s g… view at source ↗
Figure 14
Figure 14. Figure 14: Failure case. We identify two main limitations: (1) Frequency degradation: Accuracy drops notably for higher modes, where the spectral gap narrows and oscillations become harder to approximate. (2) Unseen fine details: The model struggles with thin structures or complex topological de￾tails that differ significantly from the coarse geometry seen during training. Acknowledgments This work was supported by … view at source ↗
Figure 15
Figure 15. Figure 15: Error distribution across OOD shapes ranked by Span Loss (Esub). We sort the OOD test shapes (𝑁 = 128k) from highest error (left) to lowest (right). The results highlight a clear dependency on geometric complexity: performance degrades primarily on models with intricate high-frequency surface details or non-trivial topology, while remaining robust for smooth manifolds. 1.08e−2) and lower Eigenvector MSE (… view at source ↗
Figure 16
Figure 16. Figure 16: Zero-shot resolution scalability and numerical precision. We evaluate NEO, trained exclusively on 2k-point clouds, across a wide range of test resolutions (𝑁 = 512 to 1.5M). Solid lines denote the median error; shaded regions correspond to the interquartile range (25–75%). Left/Middle: The subspace span loss (Esub) and eigenvector MSE (Evec) remain stable across resolutions, with the lowest error surprisi… view at source ↗
read the original abstract

The eigendecomposition of the Laplace--Beltrami Operator (LBO) is fundamental to geometric analysis, yet computing its low-frequency eigenmodes remains a significant bottleneck due to the high cost of iterative solvers on large-scale data. To amortize this cost, we introduce the Neural Eigenspace Operator (NEO), a feed-forward framework designed to predict the spectrum directly from point clouds. Crucially, NEO circumvents the ill-posed nature of standard eigenvector regression, which suffers from intrinsic sign flips and rotation ambiguities, by learning the stable, invariant low-frequency subspace instead. Specifically, the network predicts a redundant set of basis functions whose span robustly covers the target eigenspace, allowing for the recovery of accurate eigenpairs via a lightweight Rayleigh--Ritz refinement. To handle irregular sampling, we propose a mass-aware neural operator that incorporates per-point area weights into attention-based aggregation, improving robustness to non-uniform densities and enabling zero-shot generalization across resolutions. Our approach achieves near-linear runtime scaling and substantial wall-clock speedups over iterative solvers at comparable accuracy, and exhibits strong zero-shot transfer to high-resolution point clouds. The resulting eigenpairs support standard spectral geometry tasks, while the raw basis functions provide effective point-wise features for downstream learning. Code: https://github.com/Adversarr/NEO.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper introduces the Neural Eigenspace Operator (NEO), a feed-forward neural framework that predicts a redundant set of basis functions whose span covers the low-frequency eigenspace of the Laplace-Beltrami operator on point clouds. Accurate eigenpairs are recovered via lightweight Rayleigh-Ritz refinement. A mass-aware neural operator incorporates per-point area weights into attention-based aggregation to improve robustness to non-uniform densities and enable zero-shot generalization across resolutions. The method reports near-linear runtime scaling with substantial speedups over iterative solvers at comparable accuracy, and the resulting eigenpairs support standard spectral geometry tasks.

Significance. If the central claims hold, the work could substantially reduce the computational bottleneck of eigendecomposition on large point clouds, enabling broader use of spectral methods in geometric deep learning and shape analysis. The redundant-basis formulation is a sound way to sidestep sign-flip and rotation ambiguities that plague direct eigenvector regression. The public code link supports reproducibility.

major comments (2)
  1. [Abstract] Abstract: the claim that per-point area weights inside attention aggregation deliver robustness to non-uniform densities and zero-shot resolution transfer is load-bearing for the zero-shot generalization result, yet the manuscript provides no explicit ablation or sensitivity analysis isolating the contribution of these weights under controlled density variation.
  2. [Abstract] The near-linear runtime scaling assertion rests on the learned operator replacing iterative solvers, but without a complexity breakdown (e.g., attention cost versus number of points) or scaling plots that separate model inference from Rayleigh-Ritz post-processing, it is difficult to assess whether the speedup remains substantial at the largest scales claimed.
minor comments (2)
  1. The abstract states that the raw basis functions provide effective point-wise features for downstream learning; a brief quantitative demonstration on at least one downstream task would strengthen this secondary claim.
  2. Notation for the mass-aware aggregation operator should be introduced with an explicit equation rather than descriptive text only.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments and positive overall assessment. We address each major comment point by point below. Where the manuscript would benefit from additional material, we commit to revisions.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the claim that per-point area weights inside attention aggregation deliver robustness to non-uniform densities and zero-shot resolution transfer is load-bearing for the zero-shot generalization result, yet the manuscript provides no explicit ablation or sensitivity analysis isolating the contribution of these weights under controlled density variation.

    Authors: We agree that an explicit ablation isolating the per-point area weights under controlled density variation would strengthen the presentation. The current experiments compare mass-aware and mass-agnostic variants across sampling densities and resolutions, but do not isolate the weights in a dedicated sensitivity study. We will add such an ablation (with controlled density perturbations) to the revised manuscript. revision: yes

  2. Referee: [Abstract] The near-linear runtime scaling assertion rests on the learned operator replacing iterative solvers, but without a complexity breakdown (e.g., attention cost versus number of points) or scaling plots that separate model inference from Rayleigh-Ritz post-processing, it is difficult to assess whether the speedup remains substantial at the largest scales claimed.

    Authors: We acknowledge that a finer-grained complexity breakdown and scaling plots separating neural-operator inference from the subsequent Rayleigh-Ritz step would improve clarity. The reported near-linear wall-clock scaling includes both components; we will add an asymptotic analysis of the attention mechanism together with separate timing curves for inference versus post-processing in the revision. revision: yes

Circularity Check

0 steps flagged

No significant circularity; empirical operator learning is self-contained

full rationale

The paper introduces an empirical neural operator (NEO) trained to predict a redundant basis for the LBO eigenspace from point clouds, followed by standard Rayleigh-Ritz post-processing and a mass-aware attention design. These components are data-driven and validated on benchmarks rather than derived via equations that reduce to the inputs by construction. No self-definitional mappings, fitted parameters renamed as predictions, or load-bearing self-citations appear in the claimed pipeline; the mass-aware weighting is an architectural choice whose effect is tested empirically, not presupposed.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

Review limited to abstract; full paper would likely list network hyperparameters and training choices as free parameters. Only the most obvious domain assumption is recorded here.

axioms (1)
  • domain assumption The low-frequency eigenspace of the LBO can be stably represented by a redundant learned basis that is refined by Rayleigh-Ritz.
    Central premise allowing the method to bypass eigenvector sign and rotation ambiguities.
invented entities (1)
  • Mass-aware neural operator no independent evidence
    purpose: To incorporate per-point area weights into attention for robustness to non-uniform sampling.
    New component introduced to handle irregular point densities.

pith-pipeline@v0.9.1-grok · 5764 in / 966 out tokens · 56497 ms · 2026-06-30T14:47:45.359006+00:00 · methodology

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Reference graph

Works this paper leans on

45 extracted references · 11 canonical work pages · 5 internal anchors

  1. [1]

    and Yahav, E

    On the bottleneck of graph neural networks and its practical implications.arXiv preprint arXiv:2006.05205(2020). Mathieu Aubry, Ulrich Schlickewei, and Daniel Cremers

  2. [2]

    Ido Ben-Shaul, Leah Bar, Dalia Fishelov, and Nir Sochen

    Laplacian eigenmaps for dimensionality reduction and data representation.Neural computation15, 6 (2003), 1373–1396. Ido Ben-Shaul, Leah Bar, Dalia Fishelov, and Nir Sochen

  3. [3]

    Michael M Bronstein, Joan Bruna, Yann LeCun, Arthur Szlam, and Pierre Vandergheynst

    Deep learning solution of the eigenvalue problem for differential operators.Neural Computation35, 6 (2023), 1100–1134. Michael M Bronstein, Joan Bruna, Yann LeCun, Arthur Szlam, and Pierre Vandergheynst

  4. [4]

    Joan Bruna, Wojciech Zaremba, Arthur Szlam, and Yann LeCun

    Geometric deep learning: going beyond euclidean data.IEEE Signal Processing Magazine34, 4 (2017), 18–42. Joan Bruna, Wojciech Zaremba, Arthur Szlam, and Yann LeCun

  5. [5]

    Spectral Networks and Locally Connected Networks on Graphs

    Spectral Networks and Locally Connected Networks on Graphs.CoRRabs/1312.6203 (2013). https: //api.semanticscholar.org/CorpusID:17682909 Angel X. Chang, Thomas Funkhouser, Leonidas Guibas, Pat Hanrahan, Qixing Huang, Zimo Li, Silvio Savarese, Manolis Savva, Shuran Song, Hao Su, Jianxiong Xiao, Li Yi, and Fisher Yu. 2015.ShapeNet: An Information-Rich 3D Mod...

  6. [6]

    Ronald R Coifman and Stéphane Lafon

    Shape Space Spectra.arXiv preprint arXiv:2408.10099(2024). Ronald R Coifman and Stéphane Lafon

  7. [7]

    Keenan Crane, Clarisse Weischedel, and Max Wardetzky

    Diffusion maps.Applied and computational harmonic analysis21, 1 (2006), 5–30. Keenan Crane, Clarisse Weischedel, and Max Wardetzky

  8. [8]

    ACM60, 11 (2017), 90–99

    The heat method for distance computation.Commun. ACM60, 11 (2017), 90–99. Chandler Davis and William Morton Kahan

  9. [9]

    III.SIAM J

    The rotation of eigenvectors by a perturbation. III.SIAM J. Numer. Anal.7, 1 (1970), 1–46. Gene H Golub and Charles F Van Loan. 2013.Matrix computations. JHU press. Wenjie Hu, Sidun Liu, Peng Qiao, Zhenglun Sun, and Yong Dou

  10. [10]

    Xutong Jin, Sheng Li, Guoping Wang, and Dinesh Manocha

    Transolver is a Linear Transformer: Revisiting Physics-Attention through the Lens of Linear Attention.arXiv preprint arXiv:2511.06294(2025). Xutong Jin, Sheng Li, Guoping Wang, and Dinesh Manocha

  11. [11]

    https://doi.org/10.1145/3528223.3530184 Keller Jordan, Yuchen Jin, Vlado Boza, You Jiacheng, Franz Cesista, Laker Newhouse, and Jeremy Bernstein

    NeuralSound: Learning-based Modal Sound Synthesis with Acoustic Transfer.ACM Transactions on Graphics (SIGGRAPH 2022). https://doi.org/10.1145/3528223.3530184 Keller Jordan, Yuchen Jin, Vlado Boza, You Jiacheng, Franz Cesista, Laker Newhouse, and Jeremy Bernstein

  12. [12]

    Nikola Kovachki, Zongyi Li, Burigede Liu, Kamyar Azizzadenesheli, Kaushik Bhat- tacharya, Andrew Stuart, and Anima Anandkumar

    Toward the optimal preconditioned eigensolver: Locally optimal block preconditioned conjugate gradient method.SIAM journal on scientific computing23, 2 (2001), 517–541. Nikola Kovachki, Zongyi Li, Burigede Liu, Kamyar Azizzadenesheli, Kaushik Bhat- tacharya, Andrew Stuart, and Anima Anandkumar

  13. [13]

    Richard B Lehoucq, Danny C Sorensen, and Chao Yang

    Neural operator: Learning maps between function spaces with applications to pdes.Journal of Machine Learn- ing Research24, 89 (2023), 1–97. Richard B Lehoucq, Danny C Sorensen, and Chao Yang. 1998.ARPACK users’ guide: solution of large-scale eigenvalue problems with implicitly restarted Arnoldi methods. SIAM. Bruno Lévy

  14. [14]

    under- stands

    Laplace-beltrami eigenfunctions towards an algorithm that" under- stands" geometry. InIEEE International Conference on Shape Modeling and Applica- tions 2006 (SMI’06). IEEE, 13–13. Bruno Lévy and Hao Zhang

  15. [15]

    InACM SIGGRAPH 2010 Courses

    Spectral mesh processing. InACM SIGGRAPH 2010 Courses. 1–312. SIGGRAPH Conference Papers ’26, July 19–23, 2026, Los Angeles, CA, USA. Learning Laplacian Eigenspace with Mass-Aware Neural Operators on Point Clouds•11 H. Li, J. Sun, and Z. Zhang

  16. [16]

    Deep Eigenspace Network and Its Application to Parametric Non-selfadjoint Eigenvalue Problems. arXiv:2512.20058 [math.NA] https://arxiv.org/abs/2512.20058 Zongyi Li, Nikola Kovachki, Kamyar Azizzadenesheli, Burigede Liu, Kaushik Bhat- tacharya, Andrew Stuart, and Anima Anandkumar. 2020a. Fourier neural operator for parametric partial differential equation...

  17. [17]

    SHREC’11 Track: Shape Retrieval on Non-rigid 3D Watertight Meshes.3DOR@ eurographics5 (2011). Jingyuan Liu, Jianlin Su, Xingcheng Yao, Zhejun Jiang, Guokun Lai, Yulun Du, Yidao Qin, Weixin Xu, Enzhe Lu, Junjie Yan, Yanru Chen, Huabin Zheng, Yibo Liu, Shaowei Liu, Bohong Yin, Weiran He, Han Zhu, Yuzhi Wang, Jianzhou Wang, Mengnan Dong, Zheng Zhang, Yongshe...

  18. [18]

    Muon is Scalable for LLM Training

    Muon is Scalable for LLM Training. arXiv:2502.16982 [cs.LG] https://arxiv.org/abs/2502.16982 Ilya Loshchilov and Frank Hutter

  19. [19]

    Decoupled Weight Decay Regularization

    Decoupled Weight Decay Regularization. arXiv:1711.05101 [cs.LG] https://arxiv.org/abs/1711.05101 Lu Lu, Pengzhan Jin, Guofei Pang, Zhongqiang Zhang, and George Em Karniadakis

  20. [20]

    Haggai Maron, Meirav Galun, Noam Aigerman, Miri Trope, Nadav Dym, Ersin Yumer, Vladimir G Kim, and Yaron Lipman

    Learning nonlinear operators via DeepONet based on the universal approximation theorem of operators.Nature machine intelligence3, 3 (2021), 218–229. Haggai Maron, Meirav Galun, Noam Aigerman, Miri Trope, Nadav Dym, Ersin Yumer, Vladimir G Kim, and Yaron Lipman

  21. [21]

    Graph.36, 4 (2017), 71–1

    Convolutional neural networks on surfaces via seamless toric covers.ACM Trans. Graph.36, 4 (2017), 71–1. Simone Melzi, Jing Ren, Emanuele Rodolà, Abhishek Sharma, Peter Wonka, and Maks Ovsjanikov

  22. [22]

    ACM Trans

    ZoomOut: spectral upsampling for efficient shape correspondence. ACM Trans. Graph.38, 6, Article 155 (Nov. 2019), 14 pages. doi:10.1145/3355089. 3356524 Ben Mildenhall, Pratul P. Srinivasan, Matthew Tancik, Jonathan T. Barron, Ravi Ra- mamoorthi, and Ren Ng

  23. [23]

    Maks Ovsjanikov, Mirela Ben-Chen, Justin Solomon, Adrian Butscher, and Leonidas Guibas

    Fast Approximation of Laplace-–Beltrami Eigenproblems.Computer Graphics Forum37, 5 (2018). Maks Ovsjanikov, Mirela Ben-Chen, Justin Solomon, Adrian Butscher, and Leonidas Guibas

  24. [24]

    ACM Transactions on Graphics (ToG)31, 4 (2012), 1–11

    Functional maps: a flexible representation of maps between shapes. ACM Transactions on Graphics (ToG)31, 4 (2012), 1–11. Bo Pang, Zhongtian Zheng, Yilong Li, Guoping Wang, and Peng-Shuai Wang

  25. [25]

    Alex Pentland and John Williams

    Neural Laplacian Operator for 3D Point Clouds.ACM Transactions on Graphics (SIGGRAPH Asia)(2024). Alex Pentland and John Williams

  26. [26]

    Nasim Rahaman, Aristide Baratin, Devansh Arpit, Felix Draxler, Min Lin, Fred Ham- precht, Yoshua Bengio, and Aaron Courville

    Pointnet++: Deep hierarchical feature learning on point sets in a metric space.Advances in neural information processing systems30 (2017). Nasim Rahaman, Aristide Baratin, Devansh Arpit, Felix Draxler, Min Lin, Fred Ham- precht, Yoshua Bengio, and Aaron Courville

  27. [27]

    Jing Ren, Adrien Poulenard, Peter Wonka, and Maks Ovsjanikov

    Physics-informed neu- ral networks: A deep learning framework for solving forward and inverse problems involving nonlinear partial differential equations.Journal of Computational physics 378 (2019), 686–707. Jing Ren, Adrien Poulenard, Peter Wonka, and Maks Ovsjanikov

  28. [28]

    Martin Reuter, Franz-Erich Wolter, and Niklas Peinecke

    Continuous and orientation-preserving correspondences via functional maps.ACM Transactions on Graphics (ToG)37, 6 (2018), 1–16. Martin Reuter, Franz-Erich Wolter, and Niklas Peinecke

  29. [29]

    Nicholas Sharp, Souhaib Attaiki, Keenan Crane, and Maks Ovsjanikov

    Laplace–Beltrami spectra as ‘Shape-DNA’of surfaces and solids.Computer-Aided Design38, 4 (2006), 342–366. Nicholas Sharp, Souhaib Attaiki, Keenan Crane, and Maks Ovsjanikov

  30. [30]

    Nicholas Sharp and Keenan Crane

    Diffusion- net: Discretization agnostic learning on surfaces.ACM Transactions on Graphics (TOG)41, 3 (2022), 1–16. Nicholas Sharp and Keenan Crane

  31. [31]

    HodgeNet.ACM Transactions on Graphics (TOG)40 (2021), 1 –

  32. [32]

    https://proceedings.neurips.cc/paper_files/paper/2021/file/ 2d3d9d5373f378108cdbd30a3c52bd3e-Paper.pdf Bruno Vallet and Bruno Lévy

    Curran Asso- ciates, Inc., 5731–5744. https://proceedings.neurips.cc/paper_files/paper/2021/file/ 2d3d9d5373f378108cdbd30a3c52bd3e-Paper.pdf Bruno Vallet and Bruno Lévy

  33. [33]

    Transolver: A Fast Transformer Solver for PDEs on General Geometries

    Transolver: A fast transformer solver for pdes on general geometries.arXiv preprint arXiv:2402.02366(2024). Zherui Yang, Haiyang Xin, Tao Du, and Ligang Liu

  34. [34]

    Simple yet Effective: Low-Rank Spatial Attention for Neural Operators

    Simple yet Effective: Low- Rank Spatial Attention for Neural Operators. arXiv:2604.03582 [cs.LG] https: //arxiv.org/abs/2604.03582 L. Yi, Hao Su, Xingwen Guo, and Leonidas J. Guibas

  35. [35]

    https://api.semanticscholar.org/ CorpusID:14487589 Bing Yu et al

    SyncSpecCNN: Synchronized Spectral CNN for 3D Shape Segmentation.2017 IEEE Conference on Computer Vision and Pattern Recognition (CVPR)(2016), 6584–6592. https://api.semanticscholar.org/ CorpusID:14487589 Bing Yu et al

  36. [36]

    Chong Zeng, Yue Dong, Pieter Peers, Hongzhi Wu, and Xin Tong

    The deep Ritz method: a deep learning-based numerical algorithm for solving variational problems.Communications in Mathematics and Statistics6, 1 (2018), 1–12. Chong Zeng, Yue Dong, Pieter Peers, Hongzhi Wu, and Xin Tong

  37. [37]

    InACM SIGGRAPH 2025 Conference Papers

    RenderFormer: Transformer-based Neural Rendering of Triangle Meshes with Global Illumination. InACM SIGGRAPH 2025 Conference Papers. Hao Zhang, Oliver van Kaick, and Ramsay Dyer

  38. [38]

    InProceedings of the IEEE/CVF International Conference on Computer Vision

    Point transformer. InProceedings of the IEEE/CVF International Conference on Computer Vision. 16259–16268. 8 Full Experiment Details In this section, we provide the complete hyperparameter settings, training dynamics, and data generation details to ensure repro- ducibility. 8.1 Model Architecture and Configurations Architecture Overview.The NEO backbone i...

  39. [39]

    Test(2k)

    requires roughly 17 hours, while the wider NEO- Large (𝐿=6) requires approximately 36 hours. 9 Full Experiment Results 9.1 NEO as an Eigen Solver To strictly isolate the impact of architectural design from model capacity, we evaluate the PointNet++[Qi et al. 2017] and Point Trans- former [Zhao et al. 2021] baselines under a rigorous iso-parameter setting....

  40. [40]

    2018], a mesh-based approximate eigensolver

    Backbone Esub 𝑇sample Test(2k) 64k Non-Uniform (ms) PointNet++ 6.97e-3 1.00e-2 1.21e-2 763 Point Transformer 4.81e-3 4.92e-1 4.18e-1 1418 NEO (Ours) 3.47e-3 3.27e-3 2.63e-3 159 Comparison with FastSpectrum.We further compare NEO with FastSpectrum [Nasikun et al . 2018], a mesh-based approximate eigensolver. Using the authors’ implementation with matched s...

  41. [41]

    2.93s), NEO achieves a much more signif- icant73 × speedup (0.04s)

    and evaluation settings on our mesh datasets, we observed that while FastSpectrum offers a14× speedup over ARPACK (0.21s vs. 2.93s), NEO achieves a much more signif- icant73 × speedup (0.04s). As detailed in Table 7, NEO also yields a lower mean Span Loss (8 .60e−3compared to FastSpectrum’s SIGGRAPH Conference Papers ’26, July 19–23, 2026, Los Angeles, CA...

  42. [42]

    Method Span Loss Evec

    NEO yields lower span loss and eigenvector MSE but marginally higher variance. Method Span Loss Evec. MSE Evec. MSE Var. FastSpectrum 1.08e−2 2.28e−11.08e−1 NEO (Ours) 8.60e−3 1.97e−11.17e−1 Baselines Setting and Scalability Evaluation.To comprehensively evaluate the computational efficiency and scalability of traditional eigensolvers across varying probl...

  43. [43]

    For the NEO-based method, we freeze the backbone and only train the SIGGRAPH Conference Papers ’26, July 19–23, 2026, Los Angeles, CA, USA

    and activation scheme. For the NEO-based method, we freeze the backbone and only train the SIGGRAPH Conference Papers ’26, July 19–23, 2026, Los Angeles, CA, USA. Learning Laplacian Eigenspace with Mass-Aware Neural Operators on Point Clouds•15 ALGORITHM 2:Spectral Deflated ICPCG (Additive) Input:System matrixA, RHSb, Basis vectorsY∈R 𝑁×𝑘 from NEOOutput:S...

  44. [44]

    Positional Encoding.To establish a competitive coordinate-based baseline, we employ the Positional Encoding (PE) mechanism popu- larized by NeRF [Mildenhall et al

    Warm Start using coarse solution x0 ← C (b); r0 ←b−Ax 0; // Two-level additive apply:z=z 𝑏𝑎𝑠𝑒 +z 𝑐𝑜𝑎𝑟𝑠𝑒 z0 ← M −1 𝑏𝑎𝑠𝑒 (r0 ) + C (r 0 ); p0 ←z 0; for𝑘=0to𝐾 𝑚𝑎𝑥 do 𝛼𝑘 ← (r 𝑇 𝑘 z𝑘 )/(p 𝑇 𝑘 Ap𝑘 ); x𝑘+1 ←x 𝑘 +𝛼 𝑘 p𝑘; r𝑘+1 ←r 𝑘 −𝛼 𝑘 Ap𝑘; if∥r 𝑘+1 ∥<𝜖then break; end // Additive Preconditioner Step zℎ𝑖𝑔ℎ ← M −1 𝑏𝑎𝑠𝑒 (r𝑘+1 ); z𝑙𝑜𝑤 ← C (r 𝑘+1 ); z𝑘+1 ←z ℎ𝑖𝑔ℎ +z 𝑙𝑜...

  45. [45]

    16•Zherui Yang, Tao Du, and Ligang Liu Table 12.Segmentation on Human Body.We report the mean IoU (mIoU) evaluated at 100 and 300 training epochs

    This setting simulates a simplified deployment scenario where local area estimation is skipped, treating the integration effectively as a SIGGRAPH Conference Papers ’26, July 19–23, 2026, Los Angeles, CA, USA. 16•Zherui Yang, Tao Du, and Ligang Liu Table 12.Segmentation on Human Body.We report the mean IoU (mIoU) evaluated at 100 and 300 training epochs. ...