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Proof of Every Square-Integrable Noncommutative Law is the Law of a Square-Integrable Tuple; Realisation of Couplings and of Almost Optimal Pairs

theoremthm:l2-law-realisation-2026a
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· 13,731 chars · 37 deps · depth 31 Reason: V-A2: chain gluing of optimal couplings, law algebras, inductive limit and an L^2 Cauchy argument.

Approximate the L2 law by bounded laws at geometric distances, glue optimal couplings of consecutive ones into consistent joint laws, realise them in an inductive limit of tracial W*-probability spaces, and take the L2 limit of the resulting Cauchy sequence of bounded tuples; couplings and almost optimal pairs follow by splitting a realised 2d-tuple.

Proof

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

Notation. MM and MkM_{k} name sets of operators, the algebras of tracial W*-probability spaces; the second moment M(λ)M(\lambda) of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation §laws is not used. As in Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation §dimensions, I(γ)I(\gamma) is the cost of a coupling γ\gamma. For k∈Nk\in\mathbb{N} let θk=(12)k\theta_{k}=(\tfrac{1}{2})^{k}, the natural power of The Real Numbers: Standing Notation and Background §numbers; thus θk>0\theta_{k}>0 and θk+1=12θk\theta_{k+1}=\tfrac{1}{2}\theta_{k}, and (θk)k∈N(\theta_{k})_{k\in\mathbb{N}} converges to 00 by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §geometric with r=12r=\tfrac{1}{2}. For a tracial W*-probability space, HsaH_{\mathrm{sa}} is the set of fixed vectors of its conjugation, as in Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws. Every variable xix_{i} is self-adjoint: its support is the one-letter word (i)(i), which is its own reversal, so xi∗=xix_{i}^{*}=x_{i} by The Algebra of Noncommutative Polynomials in Finitely Many Self-Adjoint Variables §adjoint.

Proof of clause 1 (Laws). Let μ∈Σd2\mu\in\Sigma^{2}_{d}. Choices are made in this order: first a representing Cauchy sequence yy (Step 1, a single instance), then the sequence (λk)(\lambda_{k}) by countable choice (Step 1), then the sequence (γk)(\gamma_{k}) by countable choice, given (λk)(\lambda_{k}) (Step 2). Every later object is either a single instance of an existence statement (Steps 3 and 5) or determined by the preceding data.

Step 1. Approximating bounded laws. By Square-Integrable Noncommutative Laws: the Wasserstein Completion of the Laws, Affine Push-Forwards, Moments, Couplings and Cost §laws and The Metric Completion of a Metric Space §completion, μ=[y]\mu=[y] for some Cauchy sequence y=(yn)n∈Ny=(y_{n})_{n\in\mathbb{N}} in (Σd,W2)(\Sigma_{d},W_{2}), and by The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §density the sequence (κd(yn))n∈N(\kappa_{d}(y_{n}))_{n\in\mathbb{N}} converges to μ\mu in (Σd2,W^2)(\Sigma^{2}_{d},\widehat{W}_{2}). For k∈Nk\in\mathbb{N} let

Ak={λ∈Σd: W^2(κd(λ),μ)<θk}.A_{k}=\bigl\{\lambda\in\Sigma_{d}:\ \widehat{W}_{2}(\kappa_{d}(\lambda),\mu)<\theta_{k}\bigr\}.

Each AkA_{k} is nonempty: Convergent Sequence in a Metric Space with the real number θk>0\theta_{k}>0 gives K∈NK\in\mathbb{N} with yK∈Aky_{K}\in A_{k}. By Axiom of Countable Choice (with S=ΣdS=\Sigma_{d}) there is a sequence (λk)k∈N(\lambda_{k})_{k\in\mathbb{N}} with λk∈Ak\lambda_{k}\in A_{k} for every kk. Since W^2\widehat{W}_{2} is a metric by The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §metric, conditions 3 and 4 of Metric Space and The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §isometry give

W2(λk,λk+1)=W^2(κd(λk),κd(λk+1))≤W^2(κd(λk),μ)+W^2(μ,κd(λk+1))<θk+θk+1<2θk.(1)W_{2}(\lambda_{k},\lambda_{k+1})=\widehat{W}_{2}(\kappa_{d}(\lambda_{k}),\kappa_{d}(\lambda_{k+1}))\le\widehat{W}_{2}(\kappa_{d}(\lambda_{k}),\mu)+\widehat{W}_{2}(\mu,\kappa_{d}(\lambda_{k+1}))<\theta_{k}+\theta_{k+1}<2\theta_{k}.\qquad\text{(1)}

Moreover (κd(λk))k∈N(\kappa_{d}(\lambda_{k}))_{k\in\mathbb{N}} converges to μ\mu: for real η>0\eta>0 there is KK with θk<η\theta_{k}<\eta for all k≥Kk\ge K, and then W^2(κd(λk),μ)<θk<η\widehat{W}_{2}(\kappa_{d}(\lambda_{k}),\mu)<\theta_{k}<\eta. (2)\qquad\text{(2)}

Step 2. Optimal couplings. For k∈Nk\in\mathbb{N} let BkB_{k} be the set of γ∈Π(λk,λk+1)\gamma\in\Pi(\lambda_{k},\lambda_{k+1}) with I(γ)=W2(λk,λk+1)2I(\gamma)=W_{2}(\lambda_{k},\lambda_{k+1})^{2}. Each BkB_{k} is nonempty: by Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §law there are reals r,r′>0r,r'>0 with λk∈Σd,r\lambda_{k}\in\Sigma_{d,r} and λk+1∈Σd,r′\lambda_{k+1}\in\Sigma_{d,r'}; both lie in Σd,R\Sigma_{d,R} for R=max⁡(r,r′)R=\max(r,r') by Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §monotone; so The Noncommutative Wasserstein Distance: Existence of Optimal Couplings, Symmetry, Separation, a Moment Bound, Weak-Star Lower Semicontinuity, and Displacement Interpolation §attained gives an optimal coupling, which lies in BkB_{k} by The Noncommutative Quadratic Wasserstein Distance and Optimal Couplings §optimal. By Axiom of Countable Choice (with SS the set of maps P2d→C\mathcal{P}_{2d}\to\mathbb{C}) there is a sequence (γk)k∈N(\gamma_{k})_{k\in\mathbb{N}} with γk∈Bk\gamma_{k}\in B_{k} for every kk. Squaring the nonnegative numbers in (1),

γk∈Π(λk,λk+1),I(γk)=W2(λk,λk+1)2<4θk2.(3)\gamma_{k}\in\Pi(\lambda_{k},\lambda_{k+1}),\qquad I(\gamma_{k})=W_{2}(\lambda_{k},\lambda_{k+1})^{2}<4\theta_{k}^{2}.\qquad\text{(3)}

Step 3. Consistent joint laws. Apply Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws to (λk)(\lambda_{k}) and (γk)(\gamma_{k}), and fix a sequence (Γk)k∈N(\Gamma_{k})_{k\in\mathbb{N}} with Γk∈Σkd\Gamma_{k}\in\Sigma_{kd} and the properties Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §consistent, Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §links and Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §blocks, with the substitutions βk\beta_{k}, δk\delta_{k} and εk\varepsilon_{k} of that lemma.

Step 4. The spaces and the embeddings. For k∈Nk\in\mathbb{N} let Hk=HΓkH_{k}=\mathcal{H}_{\Gamma_{k}}, Mk=MΓkM_{k}=\mathcal{M}_{\Gamma_{k}} and Ωk=ΩΓk\Omega_{k}=\Omega_{\Gamma_{k}}, and write Lp(k)L^{(k)}_{p} for the left multiplication by p∈Pkdp\in\mathcal{P}_{kd} on HkH_{k} (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §multiplication). By The Tracial Algebra of a Noncommutative Law is a Tracial W*-Probability Space: the W*-Closure of the Left Multiplications §w-star, (Hk,Mk,Ωk)(H_{k},M_{k},\Omega_{k}) is a tracial W*-probability space with trace τΓk\tau_{\Gamma_{k}}. Apply Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation with γ=Γk+1∈Σ(k+1)d\gamma=\Gamma_{k+1}\in\Sigma_{(k+1)d}, m=(k+1)dm=(k+1)d, n=kdn=kd and the kdkd-tuple (x1,…,xkd)(x_{1},\dots,x_{kd}) of self-adjoint polynomials; its substitution is βk\beta_{k}, so the marginal law of that lemma is Γk+1∘βk=Γk\Gamma_{k+1}\circ\beta_{k}=\Gamma_{k} by Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §consistent. Let πk:Mk→Mk+1\pi_{k}:M_{k}\to M_{k+1} be the embedding of Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §embedding. By Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §homomorphism, πk\pi_{k} is linear, unital, multiplicative and preserves adjoints, and τΓk+1(πk(S))=τΓk(S)\tau_{\Gamma_{k+1}}(\pi_{k}(S))=\tau_{\Gamma_{k}}(S) for S∈MkS\in M_{k}; so πk\pi_{k} is a trace-preserving embedding of (Hk,Mk,Ωk)(H_{k},M_{k},\Omega_{k}) into (Hk+1,Mk+1,Ωk+1)(H_{k+1},M_{k+1},\Omega_{k+1}) in the sense of Trace-Preserving Embeddings of Tracial W*-Probability Spaces, Their Implementing Isometries and Conditional Expectations §embedding. The same clause and Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §values give

πk(Lxi(k))=Lβk(xi)(k+1)=Lxi(k+1)(i∈[kd]).(4)\pi_{k}(L^{(k)}_{x_{i}})=L^{(k+1)}_{\beta_{k}(x_{i})}=L^{(k+1)}_{x_{i}}\qquad(i\in[kd]).\qquad\text{(4)}

Step 5. The inductive limit. Apply Inductive Limits of Tracial W*-Probability Spaces along Trace-Preserving Embeddings to the spaces and embeddings of Step 4, and fix a tracial W*-probability space (H,M,Ω)(H,M,\Omega) and trace-preserving embeddings ρk\rho_{k} of (Hk,Mk,Ωk)(H_{k},M_{k},\Omega_{k}) into (H,M,Ω)(H,M,\Omega) with the property Inductive Limits of Tracial W*-Probability Spaces along Trace-Preserving Embeddings §compatible.

Step 6. The bounded tuples and their laws. Each Lxi(k)L^{(k)}_{x_{i}} (i∈[kd]i\in[kd]) lies in MkM_{k} by The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots §star-algebra and is self-adjoint by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §adjoint. For k∈Nk\in\mathbb{N}, with the convention of Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws that (k−1)d+j(k-1)d+j means jj when k=1k=1 (used for every such index below), let uku^{k} be the dd-tuple with ujk=Lx(k−1)d+j(k)u^{k}_{j}=L^{(k)}_{x_{(k-1)d+j}} and let sk=ρk(uk)s^{k}=\rho_{k}(u^{k}), the dd-tuple with sjk=ρk(ujk)s^{k}_{j}=\rho_{k}(u^{k}_{j}) (j∈[d]j\in[d]). Then uku^{k} is a self-adjoint dd-tuple in MkM_{k} (Self-Adjoint Tuples in a Tracial W*-Probability Space and Their Laws §tuple), and by Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §embedding sks^{k} is a self-adjoint dd-tuple in MM with λsk=λuk\lambda_{s^{k}}=\lambda_{u^{k}}.

Law of uku^{k}. Let ℓk=(Lx1(k),…,Lxkd(k))\ell^{k}=(L^{(k)}_{x_{1}},\dots,L^{(k)}_{x_{kd}}) and let e=(x(k−1)d+1,…,xkd)e=(x_{(k-1)d+1},\dots,x_{kd}) be the dd-tuple of εk\varepsilon_{k}. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, e(ℓk)=uke(\ell^{k})=u^{k}, so for p∈Pdp\in\mathcal{P}_{d}, Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §substitution gives p(uk)=(εkp)(ℓk)p(u^{k})=(\varepsilon_{k}p)(\ell^{k}), and The Tracial Algebra of a Noncommutative Law is a Tracial W*-Probability Space: the W*-Closure of the Left Multiplications §law for Γk\Gamma_{k} gives ⟨Ωk,(εkp)(ℓk)Ωk⟩=Γk(εkp)\langle\Omega_{k},(\varepsilon_{k}p)(\ell^{k})\Omega_{k}\rangle=\Gamma_{k}(\varepsilon_{k}p). By Self-Adjoint Tuples in a Tracial W*-Probability Space and Their Laws §law and Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §blocks, λuk(p)=Γk(εkp)=λk(p)\lambda_{u^{k}}(p)=\Gamma_{k}(\varepsilon_{k}p)=\lambda_{k}(p). Hence

λsk=λk(k∈N).(5)\lambda_{s^{k}}=\lambda_{k}\qquad(k\in\mathbb{N}).\qquad\text{(5)}

Consecutive pairs. Let vkv^{k} be the 2d2d-tuple in Mk+1M_{k+1} with vik=Lx(k−1)d+i(k+1)v^{k}_{i}=L^{(k+1)}_{x_{(k-1)d+i}} (i∈[2d]i\in[2d]), a self-adjoint 2d2d-tuple in Mk+1M_{k+1} by the first paragraph of this step. For j∈[d]j\in[d], (k−1)d+j∈[kd](k-1)d+j\in[kd], so Inductive Limits of Tracial W*-Probability Spaces along Trace-Preserving Embeddings §compatible and (4) give sjk=ρk+1(πk(ujk))=ρk+1(Lx(k−1)d+j(k+1))=ρk+1(vjk)s^{k}_{j}=\rho_{k+1}(\pi_{k}(u^{k}_{j}))=\rho_{k+1}(L^{(k+1)}_{x_{(k-1)d+j}})=\rho_{k+1}(v^{k}_{j}); and vd+jk=Lxkd+j(k+1)=ujk+1v^{k}_{d+j}=L^{(k+1)}_{x_{kd+j}}=u^{k+1}_{j}, so ρk+1(vd+jk)=sjk+1\rho_{k+1}(v^{k}_{d+j})=s^{k+1}_{j}. Thus ρk+1(vk)=(sk,sk+1)\rho_{k+1}(v^{k})=(s^{k},s^{k+1}). The computation of the previous paragraph, with Γk+1\Gamma_{k+1}, ℓk+1\ell^{k+1} and the 2d2d-tuple (x(k−1)d+1,…,x(k+1)d)(x_{(k-1)d+1},\dots,x_{(k+1)d}) of δk\delta_{k} in place of Γk\Gamma_{k}, ℓk\ell^{k} and ee, and with Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §links in place of Gluing a Chain of Noncommutative Couplings into Consistent Joint Laws §blocks, gives λvk(q)=Γk+1(δkq)=γk(q)\lambda_{v^{k}}(q)=\Gamma_{k+1}(\delta_{k}q)=\gamma_{k}(q) for q∈P2dq\in\mathcal{P}_{2d}. By Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §embedding (with 2d2d in place of dd), λ(sk,sk+1)=λvk=γk\lambda_{(s^{k},s^{k+1})}=\lambda_{v^{k}}=\gamma_{k}. By Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §coupling and (3),

∑j=1d∥sjkΩ−sjk+1Ω∥2=I(γk)<4θk2.\sum_{j=1}^{d}\lVert s^{k}_{j}\Omega-s^{k+1}_{j}\Omega\rVert^{2}=I(\gamma_{k})<4\theta_{k}^{2}.

Each summand is nonnegative, so each is at most the sum; and for nonnegative reals a,ba,b, a2<b2a^{2}<b^{2} implies a<ba<b. Hence

∥sjkΩ−sjk+1Ω∥<2θk(k∈N, j∈[d]).(6)\lVert s^{k}_{j}\Omega-s^{k+1}_{j}\Omega\rVert<2\theta_{k}\qquad(k\in\mathbb{N},\ j\in[d]).\qquad\text{(6)}

Step 7. The limit tuple. Fix j∈[d]j\in[d] and k∈Nk\in\mathbb{N}. We show by induction on l≥k+1l\ge k+1 that ∥sjkΩ−sjlΩ∥<4θk−4θl\lVert s^{k}_{j}\Omega-s^{l}_{j}\Omega\rVert<4\theta_{k}-4\theta_{l}. For l=k+1l=k+1 this is (6), since 4θk−4θk+1=2θk4\theta_{k}-4\theta_{k+1}=2\theta_{k}. If it holds for ll, then the triangle inequality of the metric of HH (claim 3 of The Induced Norm is a Norm, and Induces a Metric and condition 4 of Metric Space) and (6) give

∥sjkΩ−sjl+1Ω∥≤∥sjkΩ−sjlΩ∥+∥sjlΩ−sjl+1Ω∥<4θk−4θl+2θl=4θk−4θl+1.\lVert s^{k}_{j}\Omega-s^{l+1}_{j}\Omega\rVert\le\lVert s^{k}_{j}\Omega-s^{l}_{j}\Omega\rVert+\lVert s^{l}_{j}\Omega-s^{l+1}_{j}\Omega\rVert<4\theta_{k}-4\theta_{l}+2\theta_{l}=4\theta_{k}-4\theta_{l+1}.

Hence ∥sjkΩ−sjlΩ∥<4θk\lVert s^{k}_{j}\Omega-s^{l}_{j}\Omega\rVert<4\theta_{k} whenever l>kl>k, and the left side is 00 when l=kl=k. Given real η>0\eta>0, take KK with θk<η/4\theta_{k}<\eta/4 for all k≥Kk\ge K; for k,l≥Kk,l\ge K, by symmetry of the metric we may assume l≥kl\ge k, and then ∥sjkΩ−sjlΩ∥<η\lVert s^{k}_{j}\Omega-s^{l}_{j}\Omega\rVert<\eta. So (sjkΩ)k∈N(s^{k}_{j}\Omega)_{k\in\mathbb{N}} is a Cauchy sequence in HH (Cauchy Sequence in a Metric Space). HH is a complex Hilbert space by Tracial W*-Probability Spaces §space and Cyclic Tracial Operator Algebras and Their Traces §triple, hence complete by Complex Hilbert Space; so by Complete Metric Space the sequence converges in HH to some Xj∈HX_{j}\in H. Each sjkΩs^{k}_{j}\Omega lies in HsaH_{\mathrm{sa}} by Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §law, and HsaH_{\mathrm{sa}} contains the limits of its convergent sequences by Standard Form of a Tracial W*-Probability Space: the Commutation Theorem, Right-Bounded Vectors, Faithfulness and Self-Adjoint Vectors §self-adjoint; so Xj∈HsaX_{j}\in H_{\mathrm{sa}}.

Thus X=(X1,…,Xd)X=(X_{1},\dots,X_{d}) is an L2L^{2} dd-tuple of (H,M,Ω)(H,M,\Omega) (Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples), and (sk)k∈N(s^{k})_{k\in\mathbb{N}} is a sequence of self-adjoint dd-tuples in MM with (sjkΩ)k(s^{k}_{j}\Omega)_{k} converging to XjX_{j} for every jj. By Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §law, law(X)\mathrm{law}(X) is the limit of (κd(λsk))k∈N(\kappa_{d}(\lambda_{s^{k}}))_{k\in\mathbb{N}}, which is the sequence (κd(λk))k∈N(\kappa_{d}(\lambda_{k}))_{k\in\mathbb{N}} by (5). That sequence converges to μ\mu by (2), so law(X)=μ\mathrm{law}(X)=\mu by Uniqueness of Limits in a Metric Space.

Proof of clause 2 (Couplings). Step 1. Existence. Let γ∈Σ2d2\gamma\in\Sigma^{2}_{2d}. Clause 1, with 2d2d in place of dd, gives a tracial W*-probability space (H,M,Ω)(H,M,\Omega) and an L2L^{2} 2d2d-tuple ZZ of it with law(Z)=γ\mathrm{law}(Z)=\gamma. Let X=(Z1,…,Zd)X=(Z_{1},\dots,Z_{d}) and Y=(Zd+1,…,Z2d)Y=(Z_{d+1},\dots,Z_{2d}); their entries lie in HsaH_{\mathrm{sa}}, so they are L2L^{2} dd-tuples by Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples, and (X,Y)=Z(X,Y)=Z by Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §operations. Hence law(X,Y)=γ\mathrm{law}(X,Y)=\gamma.

Step 2. Marginals and cost. Now let (H,M,Ω)(H,M,\Omega) be any tracial W*-probability space and X,YX,Y any L2L^{2} dd-tuples of it with law(X,Y)=γ\mathrm{law}(X,Y)=\gamma. By Affine Data and Affine Substitutions of Noncommutative Polynomials §coordinate, pr1=(P1,0)\mathrm{pr}^{1}=(P^{1},0) with Pij1=1P^{1}_{ij}=1 if j=ij=i and 00 otherwise, so by Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §operations, for i∈[d]i\in[d],

(pr1(X,Y))i=0 Ω+∑j=12dPij1(X,Y)j=(X,Y)i=Xi;(\mathrm{pr}^{1}(X,Y))_{i}=0\,\Omega+\sum_{j=1}^{2d}P^{1}_{ij}(X,Y)_{j}=(X,Y)_{i}=X_{i};

likewise Pij2=1P^{2}_{ij}=1 exactly when j=d+ij=d+i, so (pr2(X,Y))i=(X,Y)d+i=Yi(\mathrm{pr}^{2}(X,Y))_{i}=(X,Y)_{d+i}=Y_{i}. Thus pr1(X,Y)=X\mathrm{pr}^{1}(X,Y)=X and pr2(X,Y)=Y\mathrm{pr}^{2}(X,Y)=Y. By Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §push-forward, applied to the L2L^{2} 2d2d-tuple (X,Y)(X,Y) with 2d2d in place of dd and dd in place of nn,

law(X)=law(pr1(X,Y))=pr#1law(X,Y)=pr#1γ,law(Y)=pr#2γ.\mathrm{law}(X)=\mathrm{law}(\mathrm{pr}^{1}(X,Y))=\mathrm{pr}^{1}_{\#}\mathrm{law}(X,Y)=\mathrm{pr}^{1}_{\#}\gamma,\qquad\mathrm{law}(Y)=\mathrm{pr}^{2}_{\#}\gamma.

By Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §coupling, ∥X−Y∥22=I(law(X,Y))=I(γ)\lVert X-Y\rVert_{2}^{2}=\mathcal{I}(\mathrm{law}(X,Y))=\mathcal{I}(\gamma).

Proof of clause 3 (Almost optimal pairs). Let μ,ν∈Σd2\mu,\nu\in\Sigma^{2}_{d} and let ε>0\varepsilon>0 be real. By The Distance between Square-Integrable Noncommutative Laws is the Infimum of the Cost over Their Couplings §approximate there is γ∈Π2(μ,ν)\gamma\in\Pi^{2}(\mu,\nu) with I(γ)≤W^2(μ,ν)2+ε\mathcal{I}(\gamma)\le\widehat{W}_{2}(\mu,\nu)^{2}+\varepsilon; by Square-Integrable Noncommutative Laws: the Wasserstein Completion of the Laws, Affine Push-Forwards, Moments, Couplings and Cost §couplings, γ∈Σ2d2\gamma\in\Sigma^{2}_{2d}, pr#1γ=μ\mathrm{pr}^{1}_{\#}\gamma=\mu and pr#2γ=ν\mathrm{pr}^{2}_{\#}\gamma=\nu. Clause 2 gives a tracial W*-probability space (H,M,Ω)(H,M,\Omega) and L2L^{2} dd-tuples X,YX,Y of it with law(X,Y)=γ\mathrm{law}(X,Y)=\gamma, and then law(X)=pr#1γ=μ\mathrm{law}(X)=\mathrm{pr}^{1}_{\#}\gamma=\mu, law(Y)=pr#2γ=ν\mathrm{law}(Y)=\mathrm{pr}^{2}_{\#}\gamma=\nu and ∥X−Y∥22=I(γ)≤W^2(μ,ν)2+ε\lVert X-Y\rVert_{2}^{2}=\mathcal{I}(\gamma)\le\widehat{W}_{2}(\mu,\nu)^{2}+\varepsilon.

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