analysis / Optimal transport; quantitative stability

Letrouit's square-root stability conjecture for Brenier maps from a uniform convex source

Theorem 1.1: for KK compact convex with interior in Rd\mathbb R^d, d≥2d\ge2, and YY compact, ∥Tμ−Tν∥L2(ρ)≤C(K,Y)W2(μ,ν)1/3\|T_\mu-T_\nu\|_{L^2(\rho)}\le C(K,Y)W_2(\mu,\nu)^{1/3} for all probability measures μ,ν\mu,\nu on YY, atomic or not; the exponent 1/31/3 cannot be raised even for K=Y=[−1,1]dK=Y=[-1,1]^d and three-atom targets, so Letrouit's square-root conjecture is false and 1/31/3 is the sharp uniform exponent. Not shown: sharp exponents in W1W_1 (a sharp W11/4W_1^{1/4} bound is attributed to Merigot) or for nonuniform source densities.

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analysisSep 25, 2026Significance 12/100Registry: lean checked

Letrouit's square-root stability conjecture for Brenier maps from a uniform convex source

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Theorem 1.1: for KK compact convex with interior in Rd\mathbb R^d, d≥2d\ge2, and YY compact, ∥Tμ−Tν∥L2(ρ)≤C(K,Y)W2(μ,ν)1/3\|T_\mu-T_\nu\|_{L^2(\rho)}\le C(K,Y)W_2(\mu,\nu)^{1/3} for all probability measures μ,ν\mu,\nu on YY, atomic or not; the exponent 1/31/3 cannot be raised even for K=Y=[−1,1]dK=Y=[-1,1]^d and three-atom targets, so Letrouit's square-root conjecture is false and 1/31/3 is the sharp uniform exponent. Not shown: sharp exponents in…

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Theorem 1.1: for KK compact convex with interior in Rd\mathbb R^d, d≥2d\ge2, and YY compact, ∥Tμ−Tν∥L2(ρ)≤C(K,Y)W2(μ,ν)1/3\|T_\mu-T_\nu\|_{L^2(\rho)}\le C(K,Y)W_2(\mu,\nu)^{1/3} for all probability measures μ,ν\mu,\nu on YY, atomic or not; the exponent 1/31/3 cannot be raised even for K=Y=[−1,1]dK=Y=[-1,1]^d and three-atom targets, so Letrouit's square-root conjecture is false and 1/31/3 is the sharp uniform exponent. Not shown: sharp exponents in W1W_1 (a sharp W11/4W_1^{1/4} bound is attributed to Merigot) or for nonuniform source densities.

Theorem 1.1: for KK compact convex with interior in Rd\mathbb R^d, d≥2d\ge2, and YY compact, ∥Tμ−Tν∥L2(ρ)≤C(K,Y)W2(μ,ν)1/3\|T_\mu-T_\nu\|_{L^2(\rho)}\le C(K,Y)W_2(\mu,\nu)^{1/3} for all probability measures μ,ν\mu,\nu on YY, atomic or not; the exponent 1/31/3 cannot be raised even for K=Y=[−1,1]dK=Y=[-1,1]^d and three-atom targets, so Letrouit's square-root conjecture is false and 1/31/3 is the sharp uniform exponent. Not shown: sharp exponents in W1W_1 (a sharp W11/4W_1^{1/4} bound is attributed to Merigot) or for nonuniform source densities.

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