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arxiv: 2605.11270 · v1 · submitted 2026-05-11 · 🧮 math.OC

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A Unified Approach for Computing Wasserstein Barycenters of Discrete and Continuous Measures

Changbo Zhu, Peng Xu, Xiaohui Chen

Pith reviewed 2026-05-13 01:23 UTC · model grok-4.3

classification 🧮 math.OC
keywords Wasserstein barycentermirror descentoptimal transportFisher-Rao geometrysemi-discrete optimal transportdiscrete measurescontinuous measures
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The pith

A primal mirror descent algorithm computes exact Wasserstein barycenters for both discrete and continuous measures in a unified framework.

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

This paper introduces a primal mirror descent algorithm in the Fisher-Rao geometry that computes the unregularized Wasserstein barycenter for probability measures. The method applies the same sequence of updates whether the inputs are discrete point clouds or absolutely continuous densities, and it carries convergence guarantees in both cases. When every input measure is discrete, the procedure begins from an arbitrary probability density, solves a series of semi-discrete optimal transport subproblems, and produces absolutely continuous iterates that converge to the exact discrete barycenter. This matters because earlier algorithms were specialized to one regime or the other and often required regularization or grid approximations that could alter the solution.

Core claim

The central claim is that a single primal mirror descent scheme operating in the Fisher-Rao geometry on the space of probability measures computes the exact Wasserstein barycenter for any collection of discrete or absolutely continuous input measures. When all inputs are discrete, the algorithm starts from any initial density and generates a sequence of absolutely continuous functions by repeatedly solving semi-discrete optimal transport problems; these iterates converge to the target discrete barycenter. The identical update rule applies directly when inputs are absolutely continuous, again with proven convergence.

What carries the argument

Primal mirror descent updates performed in the Fisher-Rao geometry on probability measures, each step reducing to a semi-discrete optimal transport subproblem.

If this is right

  • The identical algorithm handles mixed discrete and continuous input measures without any change in formulation.
  • When inputs are discrete the iterates remain absolutely continuous throughout and converge to the exact discrete barycenter.
  • No regularization is required; the method targets the unregularized problem in both regimes.
  • Numerical tests on synthetic and real data indicate competitive accuracy and running time compared with specialized solvers.

Where Pith is reading between the lines

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

  • The ability to begin from any density and still converge suggests the procedure may be robust to poor initializations in practice.
  • Because the iterates stay absolutely continuous, the method could supply smooth interpolants between a point cloud and a density without additional post-processing.
  • The unified treatment may simplify pipelines that combine sensor data arriving as point sets with image data arriving as densities.

Load-bearing premise

The input measures are discrete or absolutely continuous and the mirror descent steps remain well-defined and convergent inside the Fisher-Rao geometry.

What would settle it

Run the algorithm from a uniform density on a simple discrete instance whose barycenter is known exactly, such as two uniform distributions supported on two distinct points, and check whether the final iterate recovers that known barycenter to machine precision.

Figures

Figures reproduced from arXiv: 2605.11270 by Changbo Zhu, Peng Xu, Xiaohui Chen.

Figure 1
Figure 1. Figure 1: Barycenters from heterogeneous input distributions. [PITH_FULL_IMAGE:figures/full_fig_p008_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Left to right: ground truth (LP), mirror descent barycenter (FRBary), entropic barycenter (EWB), and debiased entropic barycenter (DSB), where λ = 0.0004 for the latter two. 5.3 2D/3D Gaussian point clouds We evaluate our method on point clouds generated from Gaussian distributions. Since the Wasserstein barycenter of Gaussian measures remains Gaussian and admits a closed-form solution, this setting allows… view at source ↗
Figure 3
Figure 3. Figure 3: 2D (left) and 3D (right) samples drawn from the true ( [PITH_FULL_IMAGE:figures/full_fig_p009_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Distances between the true and estimated means and covariances. [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Results of color averaging with stochastic palette barycenter. [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: Comparison with Bures–Wasserstein gradient descent. Performance is measured by the [PITH_FULL_IMAGE:figures/full_fig_p019_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: Swiss roll. Comaprison with free-support approaches. Using the Swiss roll data, we further compared our method (with both discretization and neural network-based method) against several representative free-support barycenter approaches: the neural network–based CW2B [Korotin et al., 2021], as well as exact and entropic solvers from the POT package. We computed the barycenter of 4 Swiss roll distributions, … view at source ↗
Figure 8
Figure 8. Figure 8: Comparison with various free-support barycenter methods. [PITH_FULL_IMAGE:figures/full_fig_p023_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: Barycenters computed from n = 500 images. D.3 Comparison on high-resolution digit data In this experiment, we compute the barycenter of 10 high-resolution (100 × 100 and 200 × 200) handwritten digit “3” ( [PITH_FULL_IMAGE:figures/full_fig_p024_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: 10 handwritten digit “3” from the HWD+ dataset. [PITH_FULL_IMAGE:figures/full_fig_p025_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: Left to right: Barycenters computed through FRBary, sGS-ADMM, debiased Sinkhorn (λ = 0.005), and WDHA. Solver 100 × 100 Images 200 × 200 Images Iterations Time (seconds) Iterations Time (seconds) FRBary 200 147 200 423 sGA-ADMM 1650 473 2950 16470 Debiased Sinkhorn 100 0.84 100 6.73 WDHA 1000 5.5 1000 67 [PITH_FULL_IMAGE:figures/full_fig_p025_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: Results of color averaging with discretization-based barycenter. [PITH_FULL_IMAGE:figures/full_fig_p026_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: Color palettes of the input images (left and middle) and the barycenter (right). [PITH_FULL_IMAGE:figures/full_fig_p026_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: Optimality gap with variable step sizes. [PITH_FULL_IMAGE:figures/full_fig_p027_14.png] view at source ↗
read the original abstract

Computing the unregularized Wasserstein barycenter for measure-valued data is a challenging optimization task. Recent algorithms have been tailored to either discrete measures as point clouds or continuous measures discretized on regular grids. In this work, we propose a primal mirror descent algorithm for computing the exact Wasserstein barycenter in the Fisher-Rao geometry. Our algorithm is a unified approach that is flexible enough to simultaneously cover discrete and absolutely continuous input measures, with convergence guarantees in both settings. In particular, when all input measures are discrete, our algorithm, initialized from any probability density, solves a sequence of semi-discrete optimal transport subproblems and produces absolutely continuous iterates that converge to the discrete barycenter. We use synthetic and real data examples to demonstrate the promising result in terms of accuracy and computational cost.

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 manuscript proposes a primal mirror descent algorithm in the Fisher-Rao geometry to compute exact (unregularized) Wasserstein barycenters. The method is presented as unified: it handles both discrete point-cloud measures and absolutely continuous measures, with claimed convergence guarantees in each case. For the discrete-input setting the algorithm starts from an arbitrary probability density, solves a sequence of semi-discrete optimal-transport subproblems at each iteration, and produces a sequence of absolutely continuous iterates asserted to converge to the exact discrete barycenter. Synthetic and real-data experiments are used to illustrate accuracy and computational cost.

Significance. A single algorithmic framework that provably recovers exact discrete barycenters from continuous iterates while also handling continuous inputs would be a useful contribution to the optimal-transport literature. The Fisher-Rao mirror-descent formulation and the explicit semi-discrete OT subproblem structure are technically interesting; if the convergence statements are rigorously established they would constitute a clear advance over existing specialized discrete or grid-based methods.

major comments (2)
  1. [Abstract, §3–4] The central convergence claim (abstract and §3–4) states that absolutely continuous iterates generated by Fisher-Rao mirror descent converge to the discrete barycenter when all input measures are discrete. The manuscript must supply an explicit argument for the limit: the topology in which convergence holds, the behavior of the mirror-descent updates as densities concentrate on atoms (where the target has zero density), and the compatibility of the semi-discrete OT solutions with the geometry. Without this justification the claim that the algorithm “produces absolutely continuous iterates that converge to the discrete barycenter” remains unverified and is load-bearing for the unified approach.
  2. [§4] Theorem statements on convergence (presumably in §4) should clarify whether any auxiliary regularity (strict positivity, smoothing, or bounded support) is assumed that would be violated in the discrete limit; if such assumptions are used they must be shown to be removable or the result must be stated with the corresponding restrictions.
minor comments (2)
  1. [§2] Notation for the Fisher-Rao metric and the mirror-descent step should be introduced once and used consistently; currently the abstract and early sections mix “Fisher-Rao geometry” with “primal mirror descent” without a clear reference to the underlying Riemannian structure.
  2. [§5] The numerical section would benefit from a direct comparison table (runtime and Wasserstein error) against at least one established discrete barycenter solver (e.g., the iterative Bregman projection method) and one grid-based continuous solver on the same synthetic instances.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. The comments highlight important points regarding the rigor of our convergence analysis for the discrete-input case. We agree that additional explicit arguments are needed to fully substantiate the claims and will revise the manuscript accordingly to strengthen the presentation of the unified approach.

read point-by-point responses
  1. Referee: [Abstract, §3–4] The central convergence claim (abstract and §3–4) states that absolutely continuous iterates generated by Fisher-Rao mirror descent converge to the discrete barycenter when all input measures are discrete. The manuscript must supply an explicit argument for the limit: the topology in which convergence holds, the behavior of the mirror-descent updates as densities concentrate on atoms (where the target has zero density), and the compatibility of the semi-discrete OT solutions with the geometry. Without this justification the claim that the algorithm “produces absolutely continuous iterates that converge to the discrete barycenter” remains unverified and is load-bearing for the unified approach.

    Authors: We agree that the current exposition would benefit from a more self-contained argument. In the revised version we will insert a new subsection (after the statement of the main convergence result in §4) that explicitly addresses the three points raised: (i) convergence holds in the narrow (weak-*) topology on the space of probability measures, which is the natural topology for Wasserstein barycenters; (ii) the Fisher-Rao mirror-descent update, when the objective value approaches the discrete barycenter value, forces the density to concentrate at the atoms because the gradient of the semi-discrete OT functional becomes unbounded away from the support; (iii) compatibility follows from the fact that the dual potentials of the semi-discrete OT problems remain bounded and the transport plans converge weakly to the optimal coupling between the limiting discrete measure and the input measures. We will include a short lemma establishing the concentration behavior and a remark on the passage to the limit inside the mirror-descent recursion. revision: yes

  2. Referee: [§4] Theorem statements on convergence (presumably in §4) should clarify whether any auxiliary regularity (strict positivity, smoothing, or bounded support) is assumed that would be violated in the discrete limit; if such assumptions are used they must be shown to be removable or the result must be stated with the corresponding restrictions.

    Authors: We thank the referee for this clarification request. The theorems in §4 are currently stated under the standing assumption that the iterates remain positive and have bounded support (inherited from the continuous-input analysis). In the revision we will (a) explicitly list these assumptions at the beginning of each theorem, (b) add a separate corollary for the purely discrete-input setting that removes the strict-positivity requirement by working with the closure of the positive cone in the narrow topology, and (c) include a short argument showing that the smoothing or bounded-support hypotheses used for the continuous case are not needed once the target is known to be discrete, because the mirror-descent step automatically drives mass to the atoms. The revised statement will therefore distinguish the two regimes clearly. revision: yes

Circularity Check

0 steps flagged

No circularity: algorithm and convergence claims are independent of inputs

full rationale

The paper proposes a primal mirror descent algorithm in Fisher-Rao geometry that unifies discrete and continuous cases by iteratively solving semi-discrete OT subproblems, with convergence of AC iterates to the discrete barycenter asserted as a theorem. No equations, definitions, or steps in the abstract or described chain reduce the claimed convergence or barycenter computation to a tautology, fitted parameter renamed as prediction, or self-citation load-bearing premise. The initialization from arbitrary density and handling of both measure types are presented as external algorithmic properties rather than self-referential. The derivation remains self-contained against the stated assumptions on input measures and geometry.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; no explicit free parameters, axioms, or invented entities can be extracted. The algorithm implicitly relies on the existence of solutions to semi-discrete OT problems and on the geometry of the Fisher-Rao metric.

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