FLOW MATCHING AND OPTIMAL TRANSPORT: AN ILLUSTRATED INTRODUCTION TO WASSERSTEIN–OTTO GEOMETRY

We recall and derive the equations underlying Flow Match- ing, making explicit the probability density function of the linearly in- terpolated random variable and relating it to the transporting veloc- ity field through the continuity equation. We visualise how the initial density is transported and compare the resulting path with a geodesic in Wasserstein–Otto geometry. We demonstrate that, for an isotropic Gaussian initial law, the Flow Matching velocity field is the minimum- energy representative of the density variation at each time, among fields satisfying the continuity equation, even though the path is generally not a geodesic under the Wasserstein–Otto metric. We explain the dis- tinction between this local minimisation and the minimisation of the action over paths with fixed endpoints using explicit calculations and illustrations.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-09
DOI
https://doi.org/10.5281/zenodo.24084197
Primary Topic
Geometric Analysis and Curvature Flows
Type
preprint
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preprint

FLOW MATCHING AND OPTIMAL TRANSPORT: AN ILLUSTRATED INTRODUCTION TO WASSERSTEIN–OTTO GEOMETRY

Pierre Guilbert
Zenodo (CERN European Organization for Nuclear Research)
Geometric Analysis and Curvature Flows
preprint

FLOW MATCHING AND OPTIMAL TRANSPORT: AN ILLUSTRATED INTRODUCTION TO WASSERSTEIN–OTTO GEOMETRY

Pierre Guilbert
preprint en

Abstract

We recall and derive the equations underlying Flow Match- ing, making explicit the probability density function of the linearly in- terpolated random variable and relating it to the transporting veloc- ity field through the continuity equation. We visualise how the initial density is transported and compare the resulting path with a geodesic in Wasserstein–Otto geometry. We demonstrate that, for an isotropic Gaussian initial law, the Flow Matching velocity field is the minimum- energy representative of the density variation at each time, among fields satisfying the continuity equation, even though the path is generally not a geodesic under the Wasserstein–Otto metric. We explain the dis- tinction between this local minimisation and the minimisation of the action over paths with fixed endpoints using explicit calculations and illustrations.

Zenodo (CERN European Organization for Nuclear Research)
Geometric Analysis and Curvature Flows
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