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Spectral Diffusion Models on the Sphere

Pierpaolo Brutti, Claudio Durastanti, Francesco Mari

TL;DR

This work extends score-based diffusion modeling to spherical data by formulating forward and reverse SDEs directly in the spherical harmonic spectral domain. It shows that the spherical DFT maps spatial Brownian motion to a constrained, non-isotropic Gaussian, necessitating a spherical mirrored Brownian noise model and a covariance $\Sigma$ in the spectral diffusion dynamics. The authors derive a matrix-based spherical DFT framework with $U = Y^{\mathsf H}Q$, establish the forward/reverse SDEs for spectral coefficients, and analyze the relationship between spatial and spectral score-matching losses, proving they are not equivalent due to geometry-induced bias. Numerical illustrations on band-limited spheres, including MNIST-Sphere, demonstrate numerical viability and reveal the geometry-driven differences in diffusion behavior while yielding comparable sample quality to spatial-domain models. This framework enables principled generative modeling of spherical data with potential applications in cosmology, earth science, and computer graphics.

Abstract

Diffusion models provide a principled framework for generative modeling via stochastic differential equations and time-reversed dynamics. Extending spectral diffusion approaches to spherical data, however, raises nontrivial geometric and stochastic issues that are absent in the Euclidean setting. In this work, we develop a diffusion modeling framework defined directly on finite-dimensional spherical harmonic representations of real-valued functions on the sphere. We show that the spherical discrete Fourier transform maps spatial Brownian motion to a constrained Gaussian process in the frequency domain with deterministic, generally non-isotropic covariance. This induces modified forward and reverse-time stochastic differential equations in the spectral domain. As a consequence, spatial and spectral score matching objectives are no longer equivalent, even in the band-limited setting, and the frequency-domain formulation introduces a geometry-dependent inductive bias. We derive the corresponding diffusion equations and characterize the induced noise covariance.

Spectral Diffusion Models on the Sphere

TL;DR

This work extends score-based diffusion modeling to spherical data by formulating forward and reverse SDEs directly in the spherical harmonic spectral domain. It shows that the spherical DFT maps spatial Brownian motion to a constrained, non-isotropic Gaussian, necessitating a spherical mirrored Brownian noise model and a covariance in the spectral diffusion dynamics. The authors derive a matrix-based spherical DFT framework with , establish the forward/reverse SDEs for spectral coefficients, and analyze the relationship between spatial and spectral score-matching losses, proving they are not equivalent due to geometry-induced bias. Numerical illustrations on band-limited spheres, including MNIST-Sphere, demonstrate numerical viability and reveal the geometry-driven differences in diffusion behavior while yielding comparable sample quality to spatial-domain models. This framework enables principled generative modeling of spherical data with potential applications in cosmology, earth science, and computer graphics.

Abstract

Diffusion models provide a principled framework for generative modeling via stochastic differential equations and time-reversed dynamics. Extending spectral diffusion approaches to spherical data, however, raises nontrivial geometric and stochastic issues that are absent in the Euclidean setting. In this work, we develop a diffusion modeling framework defined directly on finite-dimensional spherical harmonic representations of real-valued functions on the sphere. We show that the spherical discrete Fourier transform maps spatial Brownian motion to a constrained Gaussian process in the frequency domain with deterministic, generally non-isotropic covariance. This induces modified forward and reverse-time stochastic differential equations in the spectral domain. As a consequence, spatial and spectral score matching objectives are no longer equivalent, even in the band-limited setting, and the frequency-domain formulation introduces a geometry-dependent inductive bias. We derive the corresponding diffusion equations and characterize the induced noise covariance.
Paper Structure (20 sections, 6 theorems, 85 equations, 1 figure, 1 table)

This paper contains 20 sections, 6 theorems, 85 equations, 1 figure, 1 table.

Key Result

Lemma 3.3

Let $f \in L^2(\mathbb{S}^2)$ be $L$-band-limited, and let be its samples on the equiangular grid. Define the vector of spatial samples and let $\hat{\mathbf{a}} \in \mathbb{C}^{L^2}$ be the vector of spherical Fourier coefficients ordered as Then the discrete spherical Fourier transform can be expressed as the matrix--vector product where $Y$ is the spherical harmonics matrix and $Q$ the samp

Figures (1)

  • Figure 1: Comparison between the empirical covariance matrix of $\varphi[{\mathbf{\tilde{v}}}(t)]$, for $t=0$, estimated from $5\times10^{4}$ i.i.d samples (left), and the theoretical covariance matrix $\Sigma$ (right), with maximum bandlimit $L=4$.

Theorems & Definitions (20)

  • Remark 2.1
  • Definition 3.1: Spherical harmonics matrix
  • Definition 3.2: Sample weights matrix
  • Lemma 3.3: DFT of a real-valued spherical map
  • Lemma 3.4: Pseudoinverse of the spherical DFT operator $U$
  • Remark 3.5
  • Proposition 3.6: Isometry between the $L$-band limited spherical signal space and the Fourier coefficients space
  • Definition 3.7: Spherical mirrored Brownian motion
  • Lemma 3.8: Image of Brownian motion under the spherical DFT
  • Remark 3.9: Densities and scores for constrained spherical Fourier coefficients
  • ...and 10 more