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Proof of The Support of an Optimal Coupling is Cyclically Monotone

lemmalem:optimal-coupling-cyclically-monotone-euclidean-2026a
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· 11,317 chars · 25 deps · depth 21 Reason: First publication: a cycle violating monotonicity is transported to small balls of positive mass, and re-pairing a common amount of mass across the cycle preserves both marginals and strictly lowers the cost.

A cycle violating monotonicity persists on small balls of positive mass; moving a common small amount of mass from each ball to the product of the marginals of consecutive balls preserves both marginals and strictly lowers the cost.

Proof

Each result cited below is universally quantified over the data in its own statement. Finite sums of real numbers are those of Finite Sum Notation in a Field, and for NNN\in\mathbb{N} we write ΣN\Sigma_{N} for the finite sum i=1N1\sum_{i=1}^{N}1 of NN copies of 11, a positive real number by claim 6 of Properties of Finite Sums and claim 6 of Elementary Order Arithmetic in an Ordered Field. We use twice that a finite nonempty set of real numbers has a least and a greatest member, which follows from claim 9 of Elementary Order Arithmetic in an Ordered Field together with the trichotomy of the order and induction on the number of members, the inductive set being the set of those pNp\in\mathbb{N} for which every family of pp real numbers has a least and a greatest member. Write cc for the Borel function on Rd+d\mathbb{R}^{d+d} with c(z)=pr1(z)pr2(z)2c(z)=\lVert\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)\rVert^{2} of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs, so that I(σ)=Rd+dcdσI(\sigma)=\int_{\mathbb{R}^{d+d}}c\,d\sigma for every σP(Rd+d)\sigma\in\mathcal{P}(\mathbb{R}^{d+d}) by Couplings of Two Probability Measures on Euclidean Space and Their Quadratic Cost §cost.

Suppose, for contradiction, that suppπ\operatorname{supp}\pi is not cyclically monotone. By Cyclically Monotone Subset of a Doubled Euclidean Space §monotone there are NNN\in\mathbb{N} and z1,,zNsuppπz_{1},\dots,z_{N}\in\operatorname{supp}\pi such that, writing xi=pr1(zi)x_{i}=\mathrm{pr}_{1}(z_{i}) and yi=pr2(zi)y_{i}=\mathrm{pr}_{2}(z_{i}) for i[N]i\in[N] and xN+1=x1x_{N+1}=x_{1},

0<i=1Nyi(xi+1xi).0<\sum_{i=1}^{N}y_{i}\cdot(x_{i+1}-x_{i}).

Let β\beta be a positive real with 4β=2i=1Nyi(xi+1xi)4\beta=2\sum_{i=1}^{N}y_{i}\cdot(x_{i+1}-x_{i}). For i[N]i\in[N] write i=i1i^{-}=i-1 if 2i2\le i and 1=N1^{-}=N; the map iii\mapsto i^{-} is a permutation of [N][N], its inverse being ii+1i\mapsto i+1 for i<Ni<N and N1N\mapsto1.

1. The algebraic identity. Expanding ab2=a22ab+b2\lVert a-b\rVert^{2}=\lVert a\rVert^{2}-2\,a\cdot b+\lVert b\rVert^{2}, which follows from claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n, and using additivity of finite sums (claim 2 of Properties of Finite Sums) together with the invariance of a finite sum under the reindexing iii\mapsto i^{-} (Invariance of Finite Sums and Products under Reindexing by a Permutation), which gives both i=1Nyi2=i=1Nyi2\sum_{i=1}^{N}\lVert y_{i^{-}}\rVert^{2}=\sum_{i=1}^{N}\lVert y_{i}\rVert^{2} and i=1Nxiyi=i=1Nxi+1yi\sum_{i=1}^{N}x_{i}\cdot y_{i^{-}}=\sum_{i=1}^{N}x_{i+1}\cdot y_{i}, one obtains

i=1Nxiyi2i=1Nxiyi2=2i=1Nyi(xixi+1)=4β.\sum_{i=1}^{N}\lVert x_{i}-y_{i^{-}}\rVert^{2}-\sum_{i=1}^{N}\lVert x_{i}-y_{i}\rVert^{2} =2\sum_{i=1}^{N}y_{i}\cdot(x_{i}-x_{i+1})=-4\beta .

2. Choice of the radius. Let LL be the greatest of the 2N2N real numbers xiyi\lVert x_{i}-y_{i}\rVert and xiyi\lVert x_{i}-y_{i^{-}}\rVert, i[N]i\in[N], and let ε\varepsilon be a positive real with ε1\varepsilon\le1 and ΣNε(8L+8)<4β\Sigma_{N}\,\varepsilon\,(8L+8)<4\beta; such an ε\varepsilon exists by claim 3 of The Archimedean Property of the Real Numbers, applied to the positive number 4β(ΣN(8L+8))14\beta\,(\Sigma_{N}(8L+8))^{-1}, together with claim 9 of Elementary Order Arithmetic in an Ordered Field to secure ε1\varepsilon\le1 as well. For i[N]i\in[N] put Ai=B(zi,ε)B(Rd+d)A_{i}=B(z_{i},\varepsilon)\in\mathcal{B}(\mathbb{R}^{d+d}) and mi=π(Ai)m_{i}=\pi(A_{i}), a real number with 0<mi10<m_{i}\le1 by Support of a Borel Measure on a Metric Space §support and claim 2 of Basic Properties of a Measure. Let mm be the least of m1,,mNm_{1},\dots,m_{N} and put θ=mΣN1\theta=m\,\Sigma_{N}^{-1}, a positive real.

3. The normalised pieces and their marginals. For i[N]i\in[N] let hi=mi11Aih_{i}=m_{i}^{-1}\mathbf{1}_{A_{i}}, a measurable function from Rd+d\mathbb{R}^{d+d} to [0,)[0,\infty), and let πi\pi_{i} be the measure with density hih_{i} with respect to π\pi, as in claim 3 of that lemma. For BB(Rd+d)B\in\mathcal{B}(\mathbb{R}^{d+d}) the product 1Bhi\mathbf{1}_{B}h_{i} is mi11AiBm_{i}^{-1}\mathbf{1}_{A_{i}\cap B}, so claim 1 of Linearity and Monotonicity of the Lebesgue Integral and The Integral of an Indicator Function is the Measure of the Set give

πi(B)=mi1π(AiB).\pi_{i}(B)=m_{i}^{-1}\,\pi(A_{i}\cap B).

In particular πiP(Rd+d)\pi_{i}\in\mathcal{P}(\mathbb{R}^{d+d}) and πi(Rd+dAi)=0\pi_{i}(\mathbb{R}^{d+d}\setminus A_{i})=0. Put αi=(pr1)#πi\alpha_{i}=(\mathrm{pr}_{1})_{\#}\pi_{i} and βi=(pr2)#πi\beta_{i}=(\mathrm{pr}_{2})_{\#}\pi_{i}, probability measures on Rd\mathbb{R}^{d} by claim 1 of Image Measures, Measures with Densities, and Change of Variables.

If zAiz\in A_{i} then pr1(z)xi=pr1(zzi)\mathrm{pr}_{1}(z)-x_{i}=\mathrm{pr}_{1}(z-z_{i}), because the coordinate projections are compatible with differences by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections and Concatenation Identifies a Product of Euclidean Spaces with a Euclidean Space, so pr1(z)xizziε\lVert\mathrm{pr}_{1}(z)-x_{i}\rVert\le\lVert z-z_{i}\rVert\le\varepsilon by the norm bound of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections and claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n; likewise pr2(z)yiε\lVert\mathrm{pr}_{2}(z)-y_{i}\rVert\le\varepsilon. Hence αi(RdBˉ(xi,ε))=0\alpha_{i}(\mathbb{R}^{d}\setminus\bar{B}(x_{i},\varepsilon))=0 and βi(RdBˉ(yi,ε))=0\beta_{i}(\mathbb{R}^{d}\setminus\bar{B}(y_{i},\varepsilon))=0.

4. The competitor. Let g=1θi=1Nhig=1-\theta\sum_{i=1}^{N}h_{i}. For every zz one has mi1m1m_{i}^{-1}\le m^{-1}, since 0<mmi0<m\le m_{i} and inversion reverses the order on the positive reals by claims 7 and 10 of Elementary Order Arithmetic in an Ordered Field, so hi(z)m1h_{i}(z)\le m^{-1} by claim 5 of Elementary Arithmetic in an Ordered Field; summing the resulting nonnegative differences m1hi(z)m^{-1}-h_{i}(z) with claims 2, 3 and 5 of Properties of Finite Sums gives θi=1Nhi(z)θΣNm1=1\theta\sum_{i=1}^{N}h_{i}(z)\le\theta\,\Sigma_{N}\,m^{-1}=1; thus gg is a measurable function from Rd+d\mathbb{R}^{d+d} to [0,)[0,\infty), and the measure νg\nu_{g} with density gg with respect to π\pi satisfies, by the computation of step 3,

νg(B)=π(B)θi=1Nπi(B)(BB(Rd+d)).\nu_{g}(B)=\pi(B)-\theta\sum_{i=1}^{N}\pi_{i}(B)\qquad(B\in\mathcal{B}(\mathbb{R}^{d+d})).

For i[N]i\in[N] let σi\sigma_{i} be the measure with constant density θ\theta with respect to the product measure αiβi\alpha_{i}\boxtimes\beta_{i^{-}} of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product, so that σi(B)=θ(αiβi)(B)\sigma_{i}(B)=\theta\,(\alpha_{i}\boxtimes\beta_{i^{-}})(B) by the same computation, and put σN+1=νg\sigma_{N+1}=\nu_{g}.

For i[N+1]i\in[N+1] let (Xi,Fi,μi)(X_{i},\mathcal{F}_{i},\mu_{i}) be the transport of (Rd+d,B(Rd+d),σi)(\mathbb{R}^{d+d},\mathcal{B}(\mathbb{R}^{d+d}),\sigma_{i}) along the bijection z(z,i)z\mapsto(z,i) onto Xi=Rd+d×{i}X_{i}=\mathbb{R}^{d+d}\times\{i\}, as in claim 2 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions. The sets XiX_{i} are pairwise disjoint, so claim 4 of that lemma provides their countable disjoint union (X,F,μ)(X_{\sqcup},\mathcal{F}_{\sqcup},\mu_{\sqcup}), and the map W:XRd+dW:X_{\sqcup}\to\mathbb{R}^{d+d} with W((z,i))=zW((z,i))=z is measurable by claim 4(b) there. Let π~=W#μ\tilde\pi=W_{\#}\mu_{\sqcup} be its image measure; since W1(B)W^{-1}(B) meets XiX_{i} in the transport of BB, whose μi\mu_{i}-measure is σi(B)\sigma_{i}(B) by claim 2 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, claim 4(a) there gives

π~(B)=i=1N+1σi(B)=π(B)θi=1Nπi(B)+θi=1N(αiβi)(B).\tilde\pi(B)=\sum_{i=1}^{N+1}\sigma_{i}(B)=\pi(B)-\theta\sum_{i=1}^{N}\pi_{i}(B)+\theta\sum_{i=1}^{N}(\alpha_{i}\boxtimes\beta_{i^{-}})(B).

5. The competitor is a coupling. Taking B=Rd+dB=\mathbb{R}^{d+d} gives π~(Rd+d)=1θΣN+θΣN=1\tilde\pi(\mathbb{R}^{d+d})=1-\theta\,\Sigma_{N}+\theta\,\Sigma_{N}=1. For AB(Rd)A\in\mathcal{B}(\mathbb{R}^{d}), using πi(pr11(A))=αi(A)\pi_{i}(\mathrm{pr}_{1}^{-1}(A))=\alpha_{i}(A) and (αiβi)(pr11(A))=αi(A)(\alpha_{i}\boxtimes\beta_{i^{-}})(\mathrm{pr}_{1}^{-1}(A))=\alpha_{i}(A) from Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product,

π~(pr11(A))=π(pr11(A))=μ(A),\tilde\pi\bigl(\mathrm{pr}_{1}^{-1}(A)\bigr)=\pi\bigl(\mathrm{pr}_{1}^{-1}(A)\bigr)=\mu(A),

and for BB(Rd)B\in\mathcal{B}(\mathbb{R}^{d}), using i=1Nβi(B)=i=1Nβi(B)\sum_{i=1}^{N}\beta_{i^{-}}(B)=\sum_{i=1}^{N}\beta_{i}(B) by Invariance of Finite Sums and Products under Reindexing by a Permutation,

π~(pr21(B))=π(pr21(B))=ν(B).\tilde\pi\bigl(\mathrm{pr}_{2}^{-1}(B)\bigr)=\pi\bigl(\mathrm{pr}_{2}^{-1}(B)\bigr)=\nu(B).

Hence π~Π(μ,ν)\tilde\pi\in\Pi(\mu,\nu) by Couplings of Two Probability Measures on Euclidean Space and Their Quadratic Cost §coupling.

6. The cost of the competitor. All the costs below are finite by Couplings on Euclidean Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, and the Lipschitz Bound §cost-finite. By claim 2 of Image Measures, Measures with Densities, and Change of Variables applied to WW, claims 4(c) and 2 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions (the latter transporting each Xi\int_{X_{i}} back to an integral against σi\sigma_{i}) and claim 3 of Image Measures, Measures with Densities, and Change of Variables,

I(π~)=I(π)θi=1Ncdπi+θi=1Ncd(αiβi).I(\tilde\pi)=I(\pi)-\theta\sum_{i=1}^{N}\int c\,d\pi_{i}+\theta\sum_{i=1}^{N}\int c\,d(\alpha_{i}\boxtimes\beta_{i^{-}}).

We estimate the two families of integrals. Let p,qRdp,q\in\mathbb{R}^{d} and let zRd+dz\in\mathbb{R}^{d+d} satisfy pr1(z)pε\lVert\mathrm{pr}_{1}(z)-p\rVert\le\varepsilon and pr2(z)qε\lVert\mathrm{pr}_{2}(z)-q\rVert\le\varepsilon. Writing a=pr1(z)pr2(z)a=\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z) and b=pqb=p-q, claims 5 and 6 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n give ab2ε\lVert a-b\rVert\le2\varepsilon, and the same two claims give both abab\lVert a\rVert-\lVert b\rVert\le\lVert a-b\rVert and baab\lVert b\rVert-\lVert a\rVert\le\lVert a-b\rVert, hence ab2ε\bigl|\lVert a\rVert-\lVert b\rVert\bigr|\le2\varepsilon by claim 6 of Properties of the Absolute Value in an Ordered Field. Since bL\lVert b\rVert\le L and therefore aL+2ε\lVert a\rVert\le L+2\varepsilon, claim 4 of Properties of the Absolute Value in an Ordered Field gives

c(z)b2=ab(a+b)2ε(2L+2ε)ε(4L+4),\bigl|c(z)-\lVert b\rVert^{2}\bigr|=\bigl|\lVert a\rVert-\lVert b\rVert\bigr|\cdot\bigl(\lVert a\rVert+\lVert b\rVert\bigr)\le2\varepsilon\,(2L+2\varepsilon)\le\varepsilon\,(4L+4),

the first equality by the factorisation of a difference of squares (claim 4 of Zero Products and Elementary Identities in a Field) and claim 4 of Properties of the Absolute Value in an Ordered Field, and the last step using ε1\varepsilon\le1. By step 3 this applies πi\pi_{i}-almost everywhere with (p,q)=(xi,yi)(p,q)=(x_{i},y_{i}) and (αiβi)(\alpha_{i}\boxtimes\beta_{i^{-}})-almost everywhere with (p,q)=(xi,yi)(p,q)=(x_{i},y_{i^{-}}), the second because the marginals of the product measure are αi\alpha_{i} and βi\beta_{i^{-}} by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product. Integrating these bounds with claims 1 and 2 of Linearity and Monotonicity of the Lebesgue Integral and The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison, and summing,

I(π~)I(π)θ(i=1Nxiyi2i=1Nxiyi2)+θΣNε(8L+8),I(\tilde\pi)-I(\pi)\le\theta\Bigl(\sum_{i=1}^{N}\lVert x_{i}-y_{i^{-}}\rVert^{2}-\sum_{i=1}^{N}\lVert x_{i}-y_{i}\rVert^{2}\Bigr)+\theta\,\Sigma_{N}\,\varepsilon\,(8L+8),

the second term accounting for the 2N2N integrals, each of which deviates from the corresponding squared distance by at most ε(4L+4)\varepsilon(4L+4).

7. The contradiction. By step 1 the bracket equals 4β-4\beta, and by the choice of ε\varepsilon in step 2 we have ΣNε(8L+8)<4β\Sigma_{N}\,\varepsilon\,(8L+8)<4\beta; multiplying that inequality by the positive number θ\theta (claim 10 of Elementary Order Arithmetic in an Ordered Field) and adding 4θβ-4\theta\beta to both sides (claim 1 there) gives

I(π~)I(π)<4θβ+4θβ=0.I(\tilde\pi)-I(\pi)<-4\theta\beta+4\theta\beta=0 .

Thus I(π~)<I(π)I(\tilde\pi)<I(\pi), and I(π)=W2(μ,ν)2I(\pi)=W_{2}(\mu,\nu)^{2} because π\pi is optimal. This contradicts W2(μ,ν)2I(π~)W_{2}(\mu,\nu)^{2}\le I(\tilde\pi), which holds for every member of Π(μ,ν)\Pi(\mu,\nu) by The Quadratic Wasserstein Distance on Euclidean Space §distance and applies to π~\tilde\pi by step 5.

Therefore suppπ\operatorname{supp}\pi is cyclically monotone, which is claim 1 of the statement.

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