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Numerical Solution of the $L^1$-Optimal Transport Problem on Surfaces

Luca Berti, Enrico Facca, Mario Putti

TL;DR

This work tackles the numerical solution of the $L^{1}$-optimal transport problem on 2D surfaces by extending the Dynamic Monge-Kantorovich (DMK) formulation to Riemannian manifolds and solving it with Surface Finite Element Methods. By discretizing in space with SFEM and in time via forward Euler, the authors obtain time-converged approximations to the Monge-Kantorovich equations and Beckmann problem, and they demonstrate superior accuracy and convergence compared to the Earth Mover's Distance ADMM approach on a sphere. The key contributions include a geometry-aware DMK discretization on surfaces, a stable MOL scheme with inf-sup stabilization, and rigorous numerical validation against closed-form MK solutions, including explicit computation of the Wasserstein-1 distance $W_{1}$. The results indicate that the proposed DMK-based method is efficient, robust, and capable of achieving higher accuracy, providing a promising tool for OT on curved manifolds with potential extensions to multilevel and implicit-time schemes.

Abstract

In this article we study the numerical solution of the $L^1$-Optimal Transport Problem on 2D surfaces embedded in $R^3$, via the DMK formulation introduced in [FaccaCardinPutti:2018]. We extend from the Euclidean into the Riemannian setting the DMK model and conjecture the equivalence with the solution Monge-Kantorovich equations, a PDE-based formulation of the $L^1$-Optimal Transport Problem. We generalize the numerical method proposed in [FaccaCardinPutti:2018,FaccaDaneriCardinPutti:2020] to 2D surfaces embedded in $\REAL^3$ using the Surface Finite Element Model approach to approximate the Laplace-Beltrami equation arising from the model. We test the accuracy and efficiency of the proposed numerical scheme, comparing our approximate solution with respect to an exact solution on a 2D sphere. The results show that the numerical scheme is efficient, robust, and more accurate with respect to other numerical schemes presented in the literature for the solution of ls$L^1$-Optimal Transport Problem on 2D surfaces.

Numerical Solution of the $L^1$-Optimal Transport Problem on Surfaces

TL;DR

This work tackles the numerical solution of the -optimal transport problem on 2D surfaces by extending the Dynamic Monge-Kantorovich (DMK) formulation to Riemannian manifolds and solving it with Surface Finite Element Methods. By discretizing in space with SFEM and in time via forward Euler, the authors obtain time-converged approximations to the Monge-Kantorovich equations and Beckmann problem, and they demonstrate superior accuracy and convergence compared to the Earth Mover's Distance ADMM approach on a sphere. The key contributions include a geometry-aware DMK discretization on surfaces, a stable MOL scheme with inf-sup stabilization, and rigorous numerical validation against closed-form MK solutions, including explicit computation of the Wasserstein-1 distance . The results indicate that the proposed DMK-based method is efficient, robust, and capable of achieving higher accuracy, providing a promising tool for OT on curved manifolds with potential extensions to multilevel and implicit-time schemes.

Abstract

In this article we study the numerical solution of the -Optimal Transport Problem on 2D surfaces embedded in , via the DMK formulation introduced in [FaccaCardinPutti:2018]. We extend from the Euclidean into the Riemannian setting the DMK model and conjecture the equivalence with the solution Monge-Kantorovich equations, a PDE-based formulation of the -Optimal Transport Problem. We generalize the numerical method proposed in [FaccaCardinPutti:2018,FaccaDaneriCardinPutti:2020] to 2D surfaces embedded in using the Surface Finite Element Model approach to approximate the Laplace-Beltrami equation arising from the model. We test the accuracy and efficiency of the proposed numerical scheme, comparing our approximate solution with respect to an exact solution on a 2D sphere. The results show that the numerical scheme is efficient, robust, and more accurate with respect to other numerical schemes presented in the literature for the solution of ls-Optimal Transport Problem on 2D surfaces.

Paper Structure

This paper contains 17 sections, 1 theorem, 39 equations, 3 figures.

Key Result

Proposition 1

The OT density $\mu^*$ is the unique minimizer of $\mathcal{L}$ and the corresponding infimum value is exactly the Wasserstein-1 distance between $f^{+}$ and $f^{-}$: $\mathcal{L}(\mu^*)=W_{1}(f^{+},f^{-})$. Moreover, for any $T>0$ for which a solution pair $(\mu(t,\cdot), u(t,\cdot)$ of prob:dmk e

Figures (3)

  • Figure 1: Spatial distribution of the $L^{2}$-projection of $f^{+} -f^{-}$ on the mesh $\mathcal{T}$ with $554$ nodes and $1104$ triangles (left). Spatial distribution of the density $\mu^*$ together with the contour lines of the supports of $f^{+}$ and $f^{-}$ (right).
  • Figure 2: Experimental convergence towards the MK solution. Left column: time ($t$) evolution of $\operatorname{var}(\mu_{ h }(t))$, which measures convergence towards equilibrium, and of $\operatorname{err}(v_{ h }(t))$ and $\operatorname{err}_{W_{1}}(\mu_{ h }(t))$, which measure the accuracy of the spatial approximation. The results are obtained on successive uniform refinements of a an initial mesh with 554 nodes and 1124 triangles. Right column: values of the four simulation metrics as a function of computational time ($t_{CPU}$, seconds). The simulations were conducted on a first-generation 2.2GHz Intel-I5 (1-core) laptop computer.
  • Figure 3: Spatial convergence of DMK and EMDADMM on the relative Beckmann error $\operatorname{err}_{BP}(v_{ h }^*)$ (left) and on the Wasserstein-1 distance $\operatorname{err}_{W_{1}}(\mu_{ h }^*)$ (right). The errors are calculated on four mesh refinements and the corresponding experimental spatial convergence rate with respect to mesh parameter $h$, evaluated by linear approximation, is reported in the plot legend.

Theorems & Definitions (3)

  • Proposition 1
  • Remark 1
  • Definition 1: Tangential Gradient