TheoremBase

The support bound integrates the embedding inequality over the full-measure set DaD_a; the swap and displacement claims follow from change of variables, since the swap preserves DaD_a and cac_a. For lower semicontinuity the truncated partial-sum costs min(SN(y−x)min(S_N(y-x), M) are bounded continuous minorants of cac_a on DaD_a, so weak convergence and two applications of monotone convergence give pi(Dapi(D_a)=1 and the liminf bound.

Proof

Each result cited is universally quantified over the data in its own statement.

Throughout, for z∈X×Xz\in X\times X we write x=π1(z)x=\pi_{1}(z), y=π2(z)y=\pi_{2}(z) and δ(z)=y−x\delta(z)=y-x, so that Da=δ−1(Xa)D_{a}=\delta^{-1}(X^{a}) and ca=na∘δc_{a}=n_{a}\circ\delta by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §pairs; in particular ca(z)=∣y−x∣a2c_{a}(z)=|y-x|_{a}^{2} for z∈Daz\in D_{a} and ca(z)=0c_{a}(z)=0 for z∉Daz\notin D_{a}, by the definition of nan_{a} in The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §borel. For N∈NN\in\mathbb{N}, SN:X→RS_{N}:X\to\mathbb{R} is the function SN(h)=∑k=1Nak−1hk2S_{N}(h)=\sum_{k=1}^{N}a_{k}^{-1}h_{k}^{2} of The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability. For a coupling π\pi, the complement (X×X)∖Da(X\times X)\setminus D_{a} is written DacD_{a}^{c}; it is Borel, and if π(Da)=1\pi(D_{a})=1 then π(Dac)=1−1=0\pi(D_{a}^{c})=1-1=0 by claim 3 of Basic Properties of a Measure, so that DacD_{a}^{c} is π\pi-null.

Claim (support-bound). Let π∈Πa(μ,ν)\pi\in\Pi^{a}(\mu,\nu), so π(Da)=1\pi(D_{a})=1 and Ia(π)=∫ca dπ<∞I^{a}(\pi)=\int c_{a}\,d\pi<\infty by Couplings of Finite Noise Cost and Their Noise Cost §finite and Couplings of Finite Noise Cost and Their Noise Cost §cost. For z∈Daz\in D_{a} the vector y−xy-x lies in XaX^{a}, so The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §embedding gives ∣π1(z)−π2(z)∣2=∣y−x∣2≤aˉ ∣y−x∣a2=aˉ ca(z)|\pi_{1}(z)-\pi_{2}(z)|^{2}=|y-x|^{2}\le\bar{a}\,|y-x|_{a}^{2}=\bar{a}\,c_{a}(z), where ∣x−y∣=∣y−x∣|x-y|=|y-x| by the symmetry of the metric (The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §metric). Both sides are nonnegative Borel functions of zz (Couplings of Two Borel Probability Measures on a Hilbert Space and Their Quadratic Cost §cost and The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §pairs, the multiple aˉ ca\bar{a}\,c_{a} of the Borel function cac_{a} being Borel by claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions), and the inequality holds outside the π\pi-null set DacD_{a}^{c}, so by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison and the scalar rule of Linearity and Monotonicity of the Lebesgue Integral §nonnegative,

I(π)=∫X×X∣π1(z)−π2(z)∣2 π(dz)≤∫X×Xaˉ ca dπ=aˉ Ia(π)<∞.I(\pi)=\int_{X\times X}|\pi_{1}(z)-\pi_{2}(z)|^{2}\,\pi(dz)\le\int_{X\times X}\bar{a}\,c_{a}\,d\pi=\bar{a}\,I^{a}(\pi)<\infty .

Now suppose π∈Πa(μ,ν)\pi\in\Pi^{a}(\mu,\nu) exists. If μ∈P2(X)\mu\in\mathcal{P}_{2}(X), then I(π)<∞I(\pi)<\infty and the converse part of Couplings on a Hilbert Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, the Lipschitz Bound and the Moment Bound §cost-finite give ν∈P2(X)\nu\in\mathcal{P}_{2}(X). If ν∈P2(X)\nu\in\mathcal{P}_{2}(X), then by Couplings on a Hilbert Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, the Lipschitz Bound and the Moment Bound §swap the swapped measure σ#π\sigma_{\#}\pi lies in Π(ν,μ)\Pi(\nu,\mu) with I(σ#π)=I(π)<∞I(\sigma_{\#}\pi)=I(\pi)<\infty, and the converse part of Couplings on a Hilbert Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, the Lipschitz Bound and the Moment Bound §cost-finite, applied to the pair (ν,μ)(\nu,\mu) and the coupling σ#π\sigma_{\#}\pi, gives μ∈P2(X)\mu\in\mathcal{P}_{2}(X).

Claim (swap). Let π∈Πa(μ,ν)\pi\in\Pi^{a}(\mu,\nu). By Couplings on a Hilbert Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, the Lipschitz Bound and the Moment Bound §swap, σ\sigma is Borel and σ#π∈Π(ν,μ)\sigma_{\#}\pi\in\Pi(\nu,\mu). For z∈X×Xz\in X\times X one has δ(σ(z))=x−y=−δ(z)\delta(\sigma(z))=x-y=-\delta(z). Since XaX^{a} is a linear subspace of XX (The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §hilbert), δ(z)∈Xa\delta(z)\in X^{a} if and only if −δ(z)∈Xa-\delta(z)\in X^{a}; hence σ−1(Da)=Da\sigma^{-1}(D_{a})=D_{a}. Moreover ca∘σ=cac_{a}\circ\sigma=c_{a}: off DaD_{a} both sides vanish, and for z∈Daz\in D_{a}, homogeneity and symmetry of ⟨⋅,⋅⟩a\langle\cdot,\cdot\rangle_{a} give ∣−δ(z)∣a2=(−1)2∣δ(z)∣a2=∣δ(z)∣a2|-\delta(z)|_{a}^{2}=(-1)^{2}|\delta(z)|_{a}^{2}=|\delta(z)|_{a}^{2}. By Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pushforward, that is by claims 1 and 2 of Image Measures, Measures with Densities, and Change of Variables,

σ#π(Da)=π(σ−1(Da))=π(Da)=1,∫X×Xca d(σ#π)=∫X×Xca∘σ dπ=∫X×Xca dπ=Ia(π)<∞.\sigma_{\#}\pi(D_{a})=\pi\bigl(\sigma^{-1}(D_{a})\bigr)=\pi(D_{a})=1,\qquad\int_{X\times X}c_{a}\,d(\sigma_{\#}\pi)=\int_{X\times X}c_{a}\circ\sigma\,d\pi=\int_{X\times X}c_{a}\,d\pi=I^{a}(\pi)<\infty .

So σ#π\sigma_{\#}\pi has finite noise cost by Couplings of Finite Noise Cost and Their Noise Cost §finite, whence σ#π∈Πa(ν,μ)\sigma_{\#}\pi\in\Pi^{a}(\nu,\mu) by Couplings of Finite Noise Cost and Their Noise Cost §couplings, with Ia(σ#π)=Ia(π)I^{a}(\sigma_{\#}\pi)=I^{a}(\pi) by Couplings of Finite Noise Cost and Their Noise Cost §cost. In particular, if (μ,ν)(\mu,\nu) is noise-connected then so is (ν,μ)(\nu,\mu), and applying this to the pair (ν,μ)(\nu,\mu) gives the converse (Couplings of Finite Noise Cost and Their Noise Cost §connected).

Claim (displacement). Let T=(idX,S)T=(\mathrm{id}_{X},S), Borel as stated. By Couplings on a Hilbert Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, the Lipschitz Bound and the Moment Bound §pushforward, applied with its maps SS and TT taken to be idX\mathrm{id}_{X} and our SS, the measure T#μT_{\#}\mu lies in Π((idX)#μ,S#μ)\Pi((\mathrm{id}_{X})_{\#}\mu,S_{\#}\mu), and (idX)#μ=μ(\mathrm{id}_{X})_{\#}\mu=\mu because idX−1(B)=B\mathrm{id}_{X}^{-1}(B)=B for every Borel BB. Since δ(T(x))=S(x)−x∈Xa\delta(T(x))=S(x)-x\in X^{a} for every xx, one has T−1(Da)=XT^{-1}(D_{a})=X and ca∘T(x)=na(S(x)−x)c_{a}\circ T(x)=n_{a}(S(x)-x). By claims 1 and 2 of Image Measures, Measures with Densities, and Change of Variables,

T#μ(Da)=μ(X)=1,∫X×Xca d(T#μ)=∫Xna(S(x)−x) μ(dx),T_{\#}\mu(D_{a})=\mu(X)=1,\qquad\int_{X\times X}c_{a}\,d(T_{\#}\mu)=\int_{X}n_{a}(S(x)-x)\,\mu(dx),

and the right-hand side is finite by hypothesis. Hence T#μT_{\#}\mu has finite noise cost by Couplings of Finite Noise Cost and Their Noise Cost §finite, so T#μ∈Πa(μ,S#μ)T_{\#}\mu\in\Pi^{a}(\mu,S_{\#}\mu) by Couplings of Finite Noise Cost and Their Noise Cost §couplings, with the displayed noise cost by Couplings of Finite Noise Cost and Their Noise Cost §cost. For S=idXS=\mathrm{id}_{X}, which is Borel and satisfies S(x)−x=0X∈XaS(x)-x=0_{X}\in X^{a}, the integrand is na(0X)=⟨0X,0X⟩a=0n_{a}(0_{X})=\langle0_{X},0_{X}\rangle_{a}=0 (homogeneity of ⟨⋅,⋅⟩a\langle\cdot,\cdot\rangle_{a} with the factor 00), so its integral is 00 by the scalar rule of Linearity and Monotonicity of the Lebesgue Integral §nonnegative with c=0c=0; thus, by the case just proved (that is, by Couplings of Finite Noise Cost and Their Noise Cost §finite and Couplings of Finite Noise Cost and Their Noise Cost §couplings, with the value from Couplings of Finite Noise Cost and Their Noise Cost §cost), (idX,idX)#μ∈Πa(μ,μ)(\mathrm{id}_{X},\mathrm{id}_{X})_{\#}\mu\in\Pi^{a}(\mu,\mu) has noise cost 00, and (μ,μ)(\mu,\mu) is noise-connected.

Claim (lsc). Since Πa(μj,νj)⊆Π(μj,νj)\Pi^{a}(\mu_{j},\nu_{j})\subseteq\Pi(\mu_{j},\nu_{j}), Couplings on a Hilbert Space: Tightness, Closedness under Weak Convergence, and Lower Semicontinuity of the Quadratic Cost §closed gives π∈Π(μ,ν)\pi\in\Pi(\mu,\nu). Let L=lim inf⁡jIa(πj)L=\liminf_{j}I^{a}(\pi_{j}), a real number by Limit Inferior of a Bounded Sequence of Real Numbers.

Step 1 (bounded continuous minorants). For N,M∈NN,M\in\mathbb{N} let gN,M(z)=min⁡{SN(δ(z)),M}g_{N,M}(z)=\min\{S_{N}(\delta(z)),M\}. Then 0≤gN,M≤M0\le g_{N,M}\le M, as SN≥0S_{N}\ge0. It is continuous on X×XX\times X: if zm→zz_{m}\to z, then πi(zm)→πi(z)\pi_{i}(z_{m})\to\pi_{i}(z) for i=1,2i=1,2 by Properties of the Product of Two Real Inner Product Spaces §componentwise, so δ(zm)→δ(z)\delta(z_{m})\to\delta(z) by The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §linear-limits, so SN(δ(zm))→SN(δ(z))S_{N}(\delta(z_{m}))\to S_{N}(\delta(z)) by the continuity of SNS_{N} (The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §partial-sums) and Continuity Between Metric Spaces is Equivalent to Sequential Continuity §sequential; and ∣min⁡{s,M}−min⁡{t,M}∣≤∣s−t∣|\min\{s,M\}-\min\{t,M\}|\le|s-t| for real s,ts,t (check the cases s,t≤Ms,t\le M; s,t≥Ms,t\ge M; s≤M≤ts\le M\le t and its mirror), so gN,M(zm)→gN,M(z)g_{N,M}(z_{m})\to g_{N,M}(z), and Continuity Between Metric Spaces is Equivalent to Sequential Continuity §on-subset applies. Hence gN,Mg_{N,M} is Borel by claims 2 and 3 of Borel Measurability and Bounded Integration on a Metric Space, and its integral as a bounded integrable function equals its integral as a nonnegative function by claim 6 of that lemma. For z∈Daz\in D_{a}, The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §partial-sums gives gN,M(z)≤SN(δ(z))≤sup⁡N′SN′(δ(z))=∣δ(z)∣a2=ca(z)g_{N,M}(z)\le S_{N}(\delta(z))\le\sup_{N'}S_{N'}(\delta(z))=|\delta(z)|_{a}^{2}=c_{a}(z).

Step 2 (passage to the limit in jj). Fix N,MN,M. Since πj(Da)=1\pi_{j}(D_{a})=1, the inequality gN,M≤cag_{N,M}\le c_{a} holds outside the πj\pi_{j}-null set DacD_{a}^{c}, so The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison gives αj:=∫gN,M dπj≤∫ca dπj=Ia(πj)\alpha_{j}:=\int g_{N,M}\,d\pi_{j}\le\int c_{a}\,d\pi_{j}=I^{a}(\pi_{j}). By Weak Convergence of Finite Borel Measures on a Metric Space, αj→α:=∫gN,M dπ\alpha_{j}\to\alpha:=\int g_{N,M}\,d\pi. We show α≤L\alpha\le L. Let ε>0\varepsilon>0 and choose KK with αm>α−ε\alpha_{m}>\alpha-\varepsilon for all m≥Km\ge K. Then Ia(πm)≥αm>α−εI^{a}(\pi_{m})\ge\alpha_{m}>\alpha-\varepsilon for m≥Km\ge K, so α−ε\alpha-\varepsilon is a lower bound of AK={Ia(πm):m≥K}A_{K}=\{I^{a}(\pi_{m}):m\ge K\}, whence α−ε≤inf⁡AK≤L\alpha-\varepsilon\le\inf A_{K}\le L by Limit Inferior of a Bounded Sequence of Real Numbers. As ε\varepsilon was arbitrary, α≤L\alpha\le L. Thus ∫gN,M dπ≤L\int g_{N,M}\,d\pi\le L for all N,M∈NN,M\in\mathbb{N}.

Step 3 (limit in NN). Fix MM. By The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §partial-sums, SN≤SN+1S_{N}\le S_{N+1}, so gN,M≤gN+1,Mg_{N,M}\le g_{N+1,M} on X×XX\times X. Let GM(z)=sup⁡NgN,M(z)G_{M}(z)=\sup_{N}g_{N,M}(z). By Monotone Convergence Theorem, GMG_{M} is measurable and ∫GM dπ=sup⁡N∫gN,M dπ≤L\int G_{M}\,d\pi=\sup_{N}\int g_{N,M}\,d\pi\le L. If z∈Dacz\in D_{a}^{c}, then δ(z)∉Xa\delta(z)\notin X^{a}, so by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §partial-sums the sequence (SN(δ(z)))N(S_{N}(\delta(z)))_{N} is not bounded above, and some NN has SN(δ(z))≥MS_{N}(\delta(z))\ge M, i.e. gN,M(z)=Mg_{N,M}(z)=M; hence GM(z)=MG_{M}(z)=M. If z∈Daz\in D_{a} and ca(z)≤Mc_{a}(z)\le M, then gN,M(z)=SN(δ(z))g_{N,M}(z)=S_{N}(\delta(z)) for all NN by Step 1, so GM(z)=sup⁡NSN(δ(z))=ca(z)G_{M}(z)=\sup_{N}S_{N}(\delta(z))=c_{a}(z); if z∈Daz\in D_{a} and ca(z)>Mc_{a}(z)>M, then some NN has SN(δ(z))>MS_{N}(\delta(z))>M (approximation of the supremum ca(z)c_{a}(z)), so GM(z)=MG_{M}(z)=M. In all cases M 1Dac≤GMM\,\mathbf{1}_{D_{a}^{c}}\le G_{M}, and min⁡{ca(z),M}≤GM(z)\min\{c_{a}(z),M\}\le G_{M}(z) for z∈Daz\in D_{a}.

Step 4 (π(Da)=1\pi(D_{a})=1). By The Integral of an Indicator Function is the Measure of the Set and Linearity and Monotonicity of the Lebesgue Integral §nonnegative, M π(Dac)=∫M 1Dac dπ≤∫GM dπ≤LM\,\pi(D_{a}^{c})=\int M\,\mathbf{1}_{D_{a}^{c}}\,d\pi\le\int G_{M}\,d\pi\le L for every M∈NM\in\mathbb{N}. If p=π(Dac)p=\pi(D_{a}^{c}) were positive, the Archimedean property would give M∈NM\in\mathbb{N} with Mp>LMp>L, a contradiction. So p=0p=0 and π(Da)=1−p=1\pi(D_{a})=1-p=1 by claim 3 of Basic Properties of a Measure.

Step 5 (limit in MM). Since gN,M≤gN,M+1g_{N,M}\le g_{N,M+1}, also GM≤GM+1G_{M}\le G_{M+1}. Let H(z)=sup⁡MGM(z)∈[0,∞]H(z)=\sup_{M}G_{M}(z)\in[0,\infty]. By Monotone Convergence Theorem, HH is measurable and ∫H dπ=sup⁡M∫GM dπ≤L\int H\,d\pi=\sup_{M}\int G_{M}\,d\pi\le L. Moreover ca≤Hc_{a}\le H on X×XX\times X: off DaD_{a}, ca=0≤Hc_{a}=0\le H; on DaD_{a}, choosing M≥ca(z)M\ge c_{a}(z) (Archimedean property) gives ca(z)=min⁡{ca(z),M}≤GM(z)≤H(z)c_{a}(z)=\min\{c_{a}(z),M\}\le G_{M}(z)\le H(z) by Step 3. Hence, by the monotonicity part of Linearity and Monotonicity of the Lebesgue Integral §nonnegative,

∫X×Xca dπ≤∫X×XH dπ≤L<∞.\int_{X\times X}c_{a}\,d\pi\le\int_{X\times X}H\,d\pi\le L<\infty .

Together with Step 4 and π∈Π(μ,ν)\pi\in\Pi(\mu,\nu), this shows that π\pi has finite noise cost (Couplings of Finite Noise Cost and Their Noise Cost §finite), so π∈Πa(μ,ν)\pi\in\Pi^{a}(\mu,\nu) (Couplings of Finite Noise Cost and Their Noise Cost §couplings), and, by Couplings of Finite Noise Cost and Their Noise Cost §cost, Ia(π)=∫ca dπ≤lim inf⁡jIa(πj)I^{a}(\pi)=\int c_{a}\,d\pi\le\liminf_{j}I^{a}(\pi_{j}).

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