TheoremBase

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 N∈NN\in\mathbb{N} we write Ξ£N\Sigma_{N} for the finite sum βˆ‘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 p∈Np\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)=βˆ₯pr1(z)βˆ’pr2(z)βˆ₯2c(z)=\lVert\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)\rVert^{2} of Probability Measures on Euclidean Space and Random Vectors: Standing Notation (v), so that I(Οƒ)=∫Rd+dc dΟƒI(\sigma)=\int_{\mathbb{R}^{d+d}}c\,d\sigma for every ΟƒβˆˆP(Rd+d)\sigma\in\mathcal{P}(\mathbb{R}^{d+d}) by Couplings of Two Probability Measures on Euclidean Space and Their Quadratic Cost (ii).

Suppose, for contradiction, that supp⁑π\operatorname{supp}\pi is not cyclically monotone. By Cyclically Monotone Subset of a Doubled Euclidean Space (i) there are N∈NN\in\mathbb{N} and z1,…,zN∈supp⁑πz_{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<βˆ‘i=1Nyiβ‹…(xi+1βˆ’xi).0<\sum_{i=1}^{N}y_{i}\cdot(x_{i+1}-x_{i}).

Let Ξ²\beta be a positive real with 4Ξ²=2βˆ‘i=1Nyiβ‹…(xi+1βˆ’xi)4\beta=2\sum_{i=1}^{N}y_{i}\cdot(x_{i+1}-x_{i}). For i∈[N]i\in[N] write iβˆ’=iβˆ’1i^{-}=i-1 if 2≀i2\le i and 1βˆ’=N1^{-}=N; the map i↦iβˆ’i\mapsto i^{-} is a permutation of [N][N], its inverse being i↦i+1i\mapsto i+1 for i<Ni<N and N↦1N\mapsto1.

1. The algebraic identity. Expanding βˆ₯aβˆ’bβˆ₯2=βˆ₯aβˆ₯2βˆ’2 aβ‹…b+βˆ₯bβˆ₯2\lVert a-b\rVert^{2}=\lVert a\rVert^{2}-2\,a\cdot b+\lVert b\rVert^{2}, which follows from claim 1 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square and The Dot Product on Rn\mathbb{R}^n Is Symmetric, Bilinear and Positive Definite, and using additivity of finite sums (claim 2 of Properties of Finite Sums) together with the invariance of a finite sum under the reindexing i↦iβˆ’i\mapsto i^{-} (Invariance of Finite Sums and Products under Reindexing by a Permutation), which gives both βˆ‘i=1Nβˆ₯yiβˆ’βˆ₯2=βˆ‘i=1Nβˆ₯yiβˆ₯2\sum_{i=1}^{N}\lVert y_{i^{-}}\rVert^{2}=\sum_{i=1}^{N}\lVert y_{i}\rVert^{2} and βˆ‘i=1Nxiβ‹…yiβˆ’=βˆ‘i=1Nxi+1β‹…yi\sum_{i=1}^{N}x_{i}\cdot y_{i^{-}}=\sum_{i=1}^{N}x_{i+1}\cdot y_{i}, one obtains

βˆ‘i=1Nβˆ₯xiβˆ’yiβˆ’βˆ₯2βˆ’βˆ‘i=1Nβˆ₯xiβˆ’yiβˆ₯2=2βˆ‘i=1Nyiβ‹…(xiβˆ’xi+1)=βˆ’4Ξ².\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 βˆ₯xiβˆ’yiβˆ₯\lVert x_{i}-y_{i}\rVert and βˆ₯xiβˆ’yiβˆ’βˆ₯\lVert x_{i}-y_{i^{-}}\rVert, i∈[N]i\in[N], and let Ξ΅\varepsilon be a positive real with Ρ≀1\varepsilon\le1 and Ξ£N Ρ (8L+8)<4Ξ²\Sigma_{N}\,\varepsilon\,(8L+8)<4\beta; such an Ξ΅\varepsilon exists by claim 3 of The Archimedean Property of the Real Numbers, applied to the positive number 4β (Ξ£N(8L+8))βˆ’14\beta\,(\Sigma_{N}(8L+8))^{-1}, together with claim 9 of Elementary Order Arithmetic in an Ordered Field to secure Ρ≀1\varepsilon\le1 as well. For i∈[N]i\in[N] put Ai=B(zi,Ξ΅)∈B(Rd+d)A_{i}=B(z_{i},\varepsilon)\in\mathcal{B}(\mathbb{R}^{d+d}) and mi=Ο€(Ai)m_{i}=\pi(A_{i}), a real number with 0<mi≀10<m_{i}\le1 by Support of a Borel Measure on a Metric Space (i) and claim 2 of Basic Properties of a Measure. Let mm be the least of m1,…,mNm_{1},\dots,m_{N} and put ΞΈ=m ΣNβˆ’1\theta=m\,\Sigma_{N}^{-1}, a positive real.

3. The normalised pieces and their marginals. For i∈[N]i\in[N] let hi=miβˆ’11Aih_{i}=m_{i}^{-1}\mathbf{1}_{A_{i}}, a measurable function from Rd+d\mathbb{R}^{d+d} to [0,∞)[0,\infty), and let Ο€i\pi_{i} be the measure with density hih_{i} with respect to Ο€\pi, as in claim 3 of that lemma. For B∈B(Rd+d)B\in\mathcal{B}(\mathbb{R}^{d+d}) the product 1Bhi\mathbf{1}_{B}h_{i} is miβˆ’11Ai∩Bm_{i}^{-1}\mathbf{1}_{A_{i}\cap B}, so claim 1 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion and The Integral of an Indicator Function is the Measure of the Set give

Ο€i(B)=miβˆ’1 π(Ai∩B).\pi_{i}(B)=m_{i}^{-1}\,\pi(A_{i}\cap B).

In particular Ο€i∈P(Rd+d)\pi_{i}\in\mathcal{P}(\mathbb{R}^{d+d}) and Ο€i(Rd+dβˆ–Ai)=0\pi_{i}(\mathbb{R}^{d+d}\setminus A_{i})=0. Put Ξ±i=(pr1)#Ο€i\alpha_{i}=(\mathrm{pr}_{1})_{\#}\pi_{i} and Ξ²i=(pr2)#Ο€i\beta_{i}=(\mathrm{pr}_{2})_{\#}\pi_{i}, probability measures on Rd\mathbb{R}^{d} by claim 1 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables.

If z∈Aiz\in A_{i} then pr1(z)βˆ’xi=pr1(zβˆ’zi)\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 (i) and Concatenation Identifies a Product of Euclidean Spaces with a Euclidean Space, so βˆ₯pr1(z)βˆ’xiβˆ₯≀βˆ₯zβˆ’ziβˆ₯≀Ρ\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 (i) and claim 2 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square; likewise βˆ₯pr2(z)βˆ’yiβˆ₯≀Ρ\lVert\mathrm{pr}_{2}(z)-y_{i}\rVert\le\varepsilon. Hence Ξ±i(Rdβˆ–BΛ‰(xi,Ξ΅))=0\alpha_{i}(\mathbb{R}^{d}\setminus\bar{B}(x_{i},\varepsilon))=0 and Ξ²i(Rdβˆ–BΛ‰(yi,Ξ΅))=0\beta_{i}(\mathbb{R}^{d}\setminus\bar{B}(y_{i},\varepsilon))=0.

4. The competitor. Let g=1βˆ’ΞΈβˆ‘i=1Nhig=1-\theta\sum_{i=1}^{N}h_{i}. For every zz one has miβˆ’1≀mβˆ’1m_{i}^{-1}\le m^{-1}, since 0<m≀mi0<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)≀mβˆ’1h_{i}(z)\le m^{-1} by claim 5 of Elementary Arithmetic in an Ordered Field; summing the resulting nonnegative differences mβˆ’1βˆ’hi(z)m^{-1}-h_{i}(z) with claims 2, 3 and 5 of Properties of Finite Sums gives ΞΈβˆ‘i=1Nhi(z)≀θ ΣN mβˆ’1=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 Ξ½g\nu_{g} with density gg with respect to Ο€\pi satisfies, by the computation of step 3,

Ξ½g(B)=Ο€(B)βˆ’ΞΈβˆ‘i=1NΟ€i(B)(B∈B(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 Οƒi\sigma_{i} be the measure with constant density ΞΈ\theta with respect to the product measure Ξ±i⊠βiβˆ’\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 (iii), so that Οƒi(B)=θ (Ξ±i⊠βiβˆ’)(B)\sigma_{i}(B)=\theta\,(\alpha_{i}\boxtimes\beta_{i^{-}})(B) by the same computation, and put ΟƒN+1=Ξ½g\sigma_{N+1}=\nu_{g}.

For i∈[N+1]i\in[N+1] let (Xi,Fi,ΞΌi)(X_{i},\mathcal{F}_{i},\mu_{i}) be the transport of (Rd+d,B(Rd+d),Οƒi)(\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+dΓ—{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 (XβŠ”,FβŠ”,ΞΌβŠ”)(X_{\sqcup},\mathcal{F}_{\sqcup},\mu_{\sqcup}), and the map W:XβŠ”β†’Rd+dW:X_{\sqcup}\to\mathbb{R}^{d+d} with W((z,i))=zW((z,i))=z is measurable by claim 4(b) there. Let Ο€~=W#ΞΌβŠ”\tilde\pi=W_{\#}\mu_{\sqcup} be its image measure; since Wβˆ’1(B)W^{-1}(B) meets XiX_{i} in the transport of BB, whose ΞΌi\mu_{i}-measure is Οƒi(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

Ο€~(B)=βˆ‘i=1N+1Οƒi(B)=Ο€(B)βˆ’ΞΈβˆ‘i=1NΟ€i(B)+ΞΈβˆ‘i=1N(Ξ±i⊠βiβˆ’)(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 Ο€~(Rd+d)=1βˆ’ΞΈβ€‰Ξ£N+θ ΣN=1\tilde\pi(\mathbb{R}^{d+d})=1-\theta\,\Sigma_{N}+\theta\,\Sigma_{N}=1. For A∈B(Rd)A\in\mathcal{B}(\mathbb{R}^{d}), using Ο€i(pr1βˆ’1(A))=Ξ±i(A)\pi_{i}(\mathrm{pr}_{1}^{-1}(A))=\alpha_{i}(A) and (Ξ±i⊠βiβˆ’)(pr1βˆ’1(A))=Ξ±i(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 (iii),

Ο€~(pr1βˆ’1(A))=Ο€(pr1βˆ’1(A))=ΞΌ(A),\tilde\pi\bigl(\mathrm{pr}_{1}^{-1}(A)\bigr)=\pi\bigl(\mathrm{pr}_{1}^{-1}(A)\bigr)=\mu(A),

and for B∈B(Rd)B\in\mathcal{B}(\mathbb{R}^{d}), using βˆ‘i=1NΞ²iβˆ’(B)=βˆ‘i=1NΞ²i(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,

Ο€~(pr2βˆ’1(B))=Ο€(pr2βˆ’1(B))=Ξ½(B).\tilde\pi\bigl(\mathrm{pr}_{2}^{-1}(B)\bigr)=\pi\bigl(\mathrm{pr}_{2}^{-1}(B)\bigr)=\nu(B).

Hence Ο€~∈Π(ΞΌ,Ξ½)\tilde\pi\in\Pi(\mu,\nu) by Couplings of Two Probability Measures on Euclidean Space and Their Quadratic Cost (i).

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 (iii). By claim 2 of Image Measures and Measures with a Density: Measures, Integrals 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 Οƒi\sigma_{i}) and claim 3 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables,

I(Ο€~)=I(Ο€)βˆ’ΞΈβˆ‘i=1N∫c dΟ€i+ΞΈβˆ‘i=1N∫c d(Ξ±i⊠βiβˆ’).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,q∈Rdp,q\in\mathbb{R}^{d} and let z∈Rd+dz\in\mathbb{R}^{d+d} satisfy βˆ₯pr1(z)βˆ’pβˆ₯≀Ρ\lVert\mathrm{pr}_{1}(z)-p\rVert\le\varepsilon and βˆ₯pr2(z)βˆ’qβˆ₯≀Ρ\lVert\mathrm{pr}_{2}(z)-q\rVert\le\varepsilon. Writing a=pr1(z)βˆ’pr2(z)a=\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z) and b=pβˆ’qb=p-q, claims 5 and 6 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square give βˆ₯aβˆ’bβˆ₯≀2Ξ΅\lVert a-b\rVert\le2\varepsilon, and the same two claims give both βˆ₯aβˆ₯βˆ’βˆ₯bβˆ₯≀βˆ₯aβˆ’bβˆ₯\lVert a\rVert-\lVert b\rVert\le\lVert a-b\rVert and βˆ₯bβˆ₯βˆ’βˆ₯aβˆ₯≀βˆ₯aβˆ’bβˆ₯\lVert b\rVert-\lVert a\rVert\le\lVert a-b\rVert, hence ∣βˆ₯aβˆ₯βˆ’βˆ₯bβˆ₯βˆ£β‰€2Ξ΅\bigl|\lVert a\rVert-\lVert b\rVert\bigr|\le2\varepsilon by claim 6 of Properties of the Absolute Value in an Ordered Field. Since βˆ₯bβˆ₯≀L\lVert b\rVert\le L and therefore βˆ₯aβˆ₯≀L+2Ξ΅\lVert a\rVert\le L+2\varepsilon, claim 4 of Properties of the Absolute Value in an Ordered Field gives

∣c(z)βˆ’βˆ₯bβˆ₯2∣=∣βˆ₯aβˆ₯βˆ’βˆ₯bβˆ₯βˆ£β‹…(βˆ₯aβˆ₯+βˆ₯bβˆ₯)≀2Ρ (2L+2Ξ΅)≀Ρ (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 Ρ≀1\varepsilon\le1. By step 3 this applies Ο€i\pi_{i}-almost everywhere with (p,q)=(xi,yi)(p,q)=(x_{i},y_{i}) and (Ξ±i⊠βiβˆ’)(\alpha_{i}\boxtimes\beta_{i^{-}})-almost everywhere with (p,q)=(xi,yiβˆ’)(p,q)=(x_{i},y_{i^{-}}), the second because the marginals of the product measure are Ξ±i\alpha_{i} and Ξ²iβˆ’\beta_{i^{-}} by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets (iii). Integrating these bounds with claims 1 and 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion and The Lebesgue Integral and Null Sets (iii), and summing,

I(Ο€~)βˆ’I(Ο€)≀θ(βˆ‘i=1Nβˆ₯xiβˆ’yiβˆ’βˆ₯2βˆ’βˆ‘i=1Nβˆ₯xiβˆ’yiβˆ₯2)+θ ΣN Ρ (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 Ξ΅(4L+4)\varepsilon(4L+4).

7. The contradiction. By step 1 the bracket equals βˆ’4Ξ²-4\beta, and by the choice of Ξ΅\varepsilon in step 2 we have Ξ£N Ρ (8L+8)<4Ξ²\Sigma_{N}\,\varepsilon\,(8L+8)<4\beta; multiplying that inequality by the positive number ΞΈ\theta (claim 10 of Elementary Order Arithmetic in an Ordered Field) and adding βˆ’4ΞΈΞ²-4\theta\beta to both sides (claim 1 there) gives

I(Ο€~)βˆ’I(Ο€)<βˆ’4ΞΈΞ²+4ΞΈΞ²=0.I(\tilde\pi)-I(\pi)<-4\theta\beta+4\theta\beta=0 .

Thus I(Ο€~)<I(Ο€)I(\tilde\pi)<I(\pi), and I(Ο€)=W2(ΞΌ,Ξ½)2I(\pi)=W_{2}(\mu,\nu)^{2} because Ο€\pi is optimal. This contradicts W2(ΞΌ,Ξ½)2≀I(Ο€~)W_{2}(\mu,\nu)^{2}\le I(\tilde\pi), which holds for every member of Ξ (ΞΌ,Ξ½)\Pi(\mu,\nu) by The Quadratic Wasserstein Distance on Euclidean Space (i) and applies to Ο€~\tilde\pi by step 5.

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

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