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Direct extension principle for tangent measure fields (small-time limit tangency)

Establish that, for any probability measure μ in the 2-Wasserstein space, the limit (in the narrow topology or the Wasserstein metric on the tangent bundle) of geodesic velocities issued from μ as the geodesic time parameter decreases to 0 remains in the geometric tangent cone Tan_μ. Concretely, prove that taking optimal transport plans that induce geodesics at time τ>0 and letting τ→0 yields a limiting measure field that is tangent to μ, thereby providing a direct extension result for tangent measure fields analogous to the extension principle available for optimal transport plans.

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Background

The paper proves restriction and decomposition results for centred tangent and solenoidal cones in Wasserstein spaces. A key technical tool is an extension lemma for optimal transport plans: given a decomposition μ=(1−λ)μ1+λμ2, an optimal plan between μ1 and a compactly supported target can be extended to an optimal plan for μ, enabling restriction and extension arguments for solenoidal fields.

By contrast, obtaining a comparable direct extension for tangent measure fields is obstructed by the behavior of geodesic velocities as the time parameter approaches zero: limits in the narrow or Wasserstein topology may fail to remain tangent. The authors therefore avoid a direct extension by first handling solenoidal fields via optimal plans and then mirroring the result to tangent fields through duality. A direct proof ensuring small-time limits remain tangent would close this gap.

References

Despite many attempts, the author could not find a direct proof of an extension result for tangent measure fields: when letting the optimal time decrease to 0, there is no guarantee that the narrow/Wasserstein limit stays tangent.

Local structure of centred tangent cones in the Wasserstein space (2508.10837 - Aussedat, 14 Aug 2025) in Subsection 'Stability with respect to restriction'