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Proof of Plan Jets at an Ekeland Point of the Doubled Difference with Logarithmic Confinement on Square-Integrable Noncommutative Laws

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Recovers the partner tuple as an affine image of any realisation of the plan, tests the Ekeland inequality with competitors that move one marginal, and expands the quadratic and logarithmic terms.

Proof

Each result cited is universally quantified over the data in its own statement. Write λ=law(X^)\lambda=\mathrm{law}(\hat{X}), ν=law(Y^)\nu=\mathrm{law}(\hat{Y}) and D=∥X^−Y^∥2D=\lVert\hat{X}-\hat{Y}\rVert_{2}.

Step 0 (tools). (a) Tuple algebra. Fix a tracial W*-probability space (K,N,Ψ)(K,N,\Psi). By Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §pairing and Sums, Real Multiples and the Pairing of Square-Integrable Tuples in a Tracial W*-Probability Space, its L2L^{2} dd-tuples lie in the complex Hilbert space KdK^{d}, sums and real multiples are those of KdK^{d}, the pairing ⟨⋅,⋅⟩2\langle\cdot,\cdot\rangle_{2} is the inner product of KdK^{d} and takes real values on L2L^{2} dd-tuples, and ∥⋅∥2\lVert\cdot\rVert_{2} is the norm of KdK^{d}; the difference Z−WZ-W of Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples is Z+(−1)WZ+(-1)W. By conjugate symmetry and linearity in the second argument (Complex Inner Product Space, conditions 1, 2 and 3) and realness, ⟨⋅,⋅⟩2\langle\cdot,\cdot\rangle_{2} is symmetric and real bilinear on L2L^{2} dd-tuples, so for all L2L^{2} dd-tuples Z,WZ,W,

∥Z+W∥22=∥Z∥22+2⟨Z,W⟩2+∥W∥22.(E)\lVert Z+W\rVert_{2}^{2}=\lVert Z\rVert_{2}^{2}+2\langle Z,W\rangle_{2}+\lVert W\rVert_{2}^{2}.\tag{E}

Moreover ∣⟨Z,W⟩2∣≤∥Z∥2∥W∥2|\langle Z,W\rangle_{2}|\le\lVert Z\rVert_{2}\lVert W\rVert_{2} by Cauchy-Schwarz Inequality in a Complex Inner Product Space, and ∥tZ∥2=∣t∣ ∥Z∥2\lVert tZ\rVert_{2}=|t|\,\lVert Z\rVert_{2} and ∥Z+W∥2≤∥Z∥2+∥W∥2\lVert Z+W\rVert_{2}\le\lVert Z\rVert_{2}+\lVert W\rVert_{2} by claim 2 of The Induced Norm is a Norm, and Induces a Metric.

(b) Φ\Phi on pairs. For L2L^{2} dd-tuples X,YX,Y of (K,N,Ψ)(K,N,\Psi), Every Square-Integrable Noncommutative Law is the Law of a Square-Integrable Tuple; Realisation of Couplings and of Almost Optimal Pairs §coupling gives pr#1law(X,Y)=law(X)\mathrm{pr}^{1}_{\#}\mathrm{law}(X,Y)=\mathrm{law}(X), pr#2law(X,Y)=law(Y)\mathrm{pr}^{2}_{\#}\mathrm{law}(X,Y)=\mathrm{law}(Y) and I(law(X,Y))=∥X−Y∥22\mathcal{I}(\mathrm{law}(X,Y))=\lVert X-Y\rVert_{2}^{2}, and Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §moments gives M^(law(Z))=∥Z∥22\widehat{M}(\mathrm{law}(Z))=\lVert Z\rVert_{2}^{2}. Writing g(Z)=log⁡(1+∥Z∥22)g(Z)=\log(1+\lVert Z\rVert_{2}^{2}), so that G(law(Z))=g(Z)G(\mathrm{law}(Z))=g(Z), and using the lifts,

Φ(law(X,Y))=uN(X)−vN(Y)−12ε∥X−Y∥22−βg(X)−βg(Y).(F)\Phi(\mathrm{law}(X,Y))=u_{N}(X)-v_{N}(Y)-\tfrac{1}{2\varepsilon}\lVert X-Y\rVert_{2}^{2}-\beta g(X)-\beta g(Y).\tag{F}

If X′X' is a further L2L^{2} dd-tuple of (K,N,Ψ)(K,N,\Psi), the pairs (X′,Y)(X',Y) and (X,Y)(X,Y) are L2L^{2} 2d2d-tuples (Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §operations) whose difference has coordinates Xj′−XjX'_{j}-X_{j} (j∈[d]j\in[d]) followed by dd zeros, so its L2L^{2} norm is ∥X′−X∥2\lVert X'-X\rVert_{2} by the definition of the norm in Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples, and Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §lipschitz gives W^2(law(X′,Y),law(X,Y))≤∥X′−X∥2\widehat{W}_{2}(\mathrm{law}(X',Y),\mathrm{law}(X,Y))\le\lVert X'-X\rVert_{2}; likewise W^2(law(X,Y′),law(X,Y))≤∥Y′−Y∥2\widehat{W}_{2}(\mathrm{law}(X,Y'),\mathrm{law}(X,Y))\le\lVert Y'-Y\rVert_{2}.

(c) Logarithm. For reals s,s′≥0s,s'\ge0, put t=(1+s′)/(1+s)>0t=(1+s')/(1+s)>0. Then log⁡(1+s′)=log⁡(1+s)+log⁡t\log(1+s')=\log(1+s)+\log t by the product rule in The Natural Logarithm, and log⁡t≤t−1=(s′−s)/(1+s)\log t\le t-1=(s'-s)/(1+s) by The Function slog⁡ss\log s: Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm §log. For L2L^{2} dd-tuples Z,Z′Z,Z' of (K,N,Ψ)(K,N,\Psi), apply this with s=∥Z∥22s=\lVert Z\rVert_{2}^{2}, s′=∥Z′∥22s'=\lVert Z'\rVert_{2}^{2}; by (E) with W=Z′−ZW=Z'-Z, s′−s=2⟨Z,Z′−Z⟩2+∥Z′−Z∥22s'-s=2\langle Z,Z'-Z\rangle_{2}+\lVert Z'-Z\rVert_{2}^{2}, and 1/(1+s)≤11/(1+s)\le1, so

g(Z′)−g(Z)≤⟨21+∥Z∥22Z,  Z′−Z⟩2+∥Z′−Z∥22.(L)g(Z')-g(Z)\le\Bigl\langle\frac{2}{1+\lVert Z\rVert_{2}^{2}}Z,\;Z'-Z\Bigr\rangle_{2}+\lVert Z'-Z\rVert_{2}^{2}.\tag{L}

(d) Norms are law data. If Z,Z′Z,Z' are L2L^{2} dd-tuples (of possibly different spaces) with law(Z)=law(Z′)\mathrm{law}(Z)=\mathrm{law}(Z'), then ∥Z∥2=∥Z′∥2\lVert Z\rVert_{2}=\lVert Z'\rVert_{2} by Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §moments and Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field (claim 3). If law(X,P)=law(X′,P′)\mathrm{law}(X,P)=\mathrm{law}(X',P'), then law(X)=law(X′)\mathrm{law}(X)=\mathrm{law}(X') and law(P)=law(P′)\mathrm{law}(P)=\mathrm{law}(P') by Every Square-Integrable Noncommutative Law is the Law of a Square-Integrable Tuple; Realisation of Couplings and of Almost Optimal Pairs §coupling.

(e) The Ekeland inequality. By hypothesis, Φ(γ)≤Φ(γ^)+δ W^2(γ,γ^)\Phi(\gamma)\le\Phi(\hat{\gamma})+\delta\,\widehat{W}_{2}(\gamma,\hat{\gamma}) for every γ∈Σ2d2\gamma\in\Sigma^{2}_{2d}.

Clause 1. Put s=∥X^∥22s=\lVert\hat{X}\rVert_{2}^{2} and κ=2βε/(1+s)\kappa=2\beta\varepsilon/(1+s), so q=(κ/ε)X^q=(\kappa/\varepsilon)\hat{X}. Let πu=law(X^,p+q)\pi_{u}=\mathrm{law}(\hat{X},p+q); by Every Square-Integrable Noncommutative Law is the Law of a Square-Integrable Tuple; Realisation of Couplings and of Almost Optimal Pairs §coupling, pr#1πu=λ\mathrm{pr}^{1}_{\#}\pi_{u}=\lambda, so πu\pi_{u} is a plan at λ\lambda. Let T=(B,0)T=(B,0) be the affine datum from 2d2d to 2d2d variables with, for i,j∈[d]i,j\in[d], Bij=1B_{ij}=1 if i=ji=j and 00 otherwise, Bi,d+j=0B_{i,d+j}=0, Bd+i,j=1+κB_{d+i,j}=1+\kappa if i=ji=j and 00 otherwise, and Bd+i,d+j=−εB_{d+i,d+j}=-\varepsilon if i=ji=j and 00 otherwise. By Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §operations, for all L2L^{2} dd-tuples X,PX,P of any tracial W*-probability space, T(X,P)=(X,(1+κ)X−εP)T(X,P)=(X,(1+\kappa)X-\varepsilon P) (the terms with coefficient 00 vanish). Since εp=X^−Y^\varepsilon p=\hat{X}-\hat{Y} and εq=κX^\varepsilon q=\kappa\hat{X}, we get (1+κ)X^−ε(p+q)=Y^(1+\kappa)\hat{X}-\varepsilon(p+q)=\hat{Y}, so T(X^,p+q)=(X^,Y^)T(\hat{X},p+q)=(\hat{X},\hat{Y}).

Let η>0\eta>0 and put r=η (1/(2ε)+β)−1>0r=\eta\,(1/(2\varepsilon)+\beta)^{-1}>0. Let (K,N,Ψ)(K,N,\Psi) be a tracial W*-probability space and X,P,X′X,P,X' be L2L^{2} dd-tuples of it with law(X,P)=πu\mathrm{law}(X,P)=\pi_{u} and ∥X′−X∥2<r\lVert X'-X\rVert_{2}<r. Put Y=(1+κ)X−εPY=(1+\kappa)X-\varepsilon P. By Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §push-forward (twice),

law(X,Y)=law(T(X,P))=T#πu=law(T(X^,p+q))=law(X^,Y^)=γ^.\mathrm{law}(X,Y)=\mathrm{law}(T(X,P))=T_{\#}\pi_{u}=\mathrm{law}(T(\hat{X},p+q))=\mathrm{law}(\hat{X},\hat{Y})=\hat{\gamma}.

By (d), law(X)=λ\mathrm{law}(X)=\lambda and ∥X∥22=s\lVert X\rVert_{2}^{2}=s; and X−Y=εP−κXX-Y=\varepsilon P-\kappa X, so

P=1ε(X−Y)+2β1+∥X∥22X.(P)P=\tfrac{1}{\varepsilon}(X-Y)+\tfrac{2\beta}{1+\lVert X\rVert_{2}^{2}}X.\tag{P}

By (e) with γ=law(X′,Y)\gamma=\mathrm{law}(X',Y) and (b), Φ(law(X′,Y))≤Φ(law(X,Y))+δ∥X′−X∥2\Phi(\mathrm{law}(X',Y))\le\Phi(\mathrm{law}(X,Y))+\delta\lVert X'-X\rVert_{2}. Expanding both sides by (F) and cancelling vN(Y)v_{N}(Y) and βg(Y)\beta g(Y),

uN(X′)≤uN(X)+12ε(∥X′−Y∥22−∥X−Y∥22)+β(g(X′)−g(X))+δ∥X′−X∥2.u_{N}(X')\le u_{N}(X)+\tfrac{1}{2\varepsilon}\bigl(\lVert X'-Y\rVert_{2}^{2}-\lVert X-Y\rVert_{2}^{2}\bigr)+\beta\bigl(g(X')-g(X)\bigr)+\delta\lVert X'-X\rVert_{2}.

By (E) with Z=X−YZ=X-Y and W=X′−XW=X'-X, ∥X′−Y∥22−∥X−Y∥22=2⟨X−Y,X′−X⟩2+∥X′−X∥22\lVert X'-Y\rVert_{2}^{2}-\lVert X-Y\rVert_{2}^{2}=2\langle X-Y,X'-X\rangle_{2}+\lVert X'-X\rVert_{2}^{2}; by (L) with Z=XZ=X, Z′=X′Z'=X', β(g(X′)−g(X))≤⟨2β1+sX,X′−X⟩2+β∥X′−X∥22\beta(g(X')-g(X))\le\langle\frac{2\beta}{1+s}X,X'-X\rangle_{2}+\beta\lVert X'-X\rVert_{2}^{2}. Adding, using bilinearity, (P) and uN(X)=u(λ)u_{N}(X)=u(\lambda),

uN(X′)≤u(λ)+⟨P,X′−X⟩2+(12ε+β)∥X′−X∥22+δ∥X′−X∥2.u_{N}(X')\le u(\lambda)+\langle P,X'-X\rangle_{2}+\Bigl(\tfrac{1}{2\varepsilon}+\beta\Bigr)\lVert X'-X\rVert_{2}^{2}+\delta\lVert X'-X\rVert_{2}.

Since ∥X′−X∥2<r\lVert X'-X\rVert_{2}<r, (12ε+β)∥X′−X∥22≤η∥X′−X∥2(\frac{1}{2\varepsilon}+\beta)\lVert X'-X\rVert_{2}^{2}\le\eta\lVert X'-X\rVert_{2}, whence uN(X′)≤u(λ)+⟨P,X′−X⟩2+(δ+η)∥X′−X∥2u_{N}(X')\le u(\lambda)+\langle P,X'-X\rangle_{2}+(\delta+\eta)\lVert X'-X\rVert_{2}. Thus πu\pi_{u} is a plan superdifferential of uu at λ\lambda with slack δ\delta (Plan Superdifferentials, Plan Subdifferentials and Plan Jets with Slack on Square-Integrable Noncommutative Laws §super), and πu∈Jδ+u(λ)\pi_{u}\in J^{+}_{\delta}u(\lambda) by Plan Superdifferentials, Plan Subdifferentials and Plan Jets with Slack on Square-Integrable Noncommutative Laws §superjet.

Clause 2. Put t=∥Y^∥22t=\lVert\hat{Y}\rVert_{2}^{2} and κ′=2βε/(1+t)\kappa'=2\beta\varepsilon/(1+t), so q′=(κ′/ε)Y^q'=(\kappa'/\varepsilon)\hat{Y}, and let πv=law(Y^,p−q′)\pi_{v}=\mathrm{law}(\hat{Y},p-q'), a plan at ν\nu as before. Let T′T' be the affine datum from 2d2d to 2d2d variables with T′(Y,P)=((1+κ′)Y+εP, Y)T'(Y,P)=((1+\kappa')Y+\varepsilon P,\,Y) for all L2L^{2} dd-tuples Y,PY,P (entries 1+κ′1+\kappa' and ε\varepsilon on the diagonals of the upper blocks, 11 on the diagonal of the lower left block, 00 elsewhere, translation part 00; Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §operations). Since (1+κ′)Y^+ε(p−q′)=Y^+(X^−Y^)=X^(1+\kappa')\hat{Y}+\varepsilon(p-q')=\hat{Y}+(\hat{X}-\hat{Y})=\hat{X}, T′(Y^,p−q′)=(X^,Y^)T'(\hat{Y},p-q')=(\hat{X},\hat{Y}).

Let η>0\eta>0, rr as above, and let Y,P,Y′Y,P,Y' be L2L^{2} dd-tuples of a tracial W*-probability space (K,N,Ψ)(K,N,\Psi) with law(Y,P)=πv\mathrm{law}(Y,P)=\pi_{v} and ∥Y′−Y∥2<r\lVert Y'-Y\rVert_{2}<r. Put X=(1+κ′)Y+εPX=(1+\kappa')Y+\varepsilon P. As in clause 1, law(X,Y)=T#′πv=γ^\mathrm{law}(X,Y)=T'_{\#}\pi_{v}=\hat{\gamma}, law(Y)=ν\mathrm{law}(Y)=\nu, ∥Y∥22=t\lVert Y\rVert_{2}^{2}=t, and P=1ε(X−Y)−2β1+tYP=\frac{1}{\varepsilon}(X-Y)-\frac{2\beta}{1+t}Y. By (e) with γ=law(X,Y′)\gamma=\mathrm{law}(X,Y'), (b) and (F), after cancelling uN(X)u_{N}(X) and βg(X)\beta g(X),

vN(Y′)≥v(ν)−12ε(∥X−Y′∥22−∥X−Y∥22)−β(g(Y′)−g(Y))−δ∥Y′−Y∥2.v_{N}(Y')\ge v(\nu)-\tfrac{1}{2\varepsilon}\bigl(\lVert X-Y'\rVert_{2}^{2}-\lVert X-Y\rVert_{2}^{2}\bigr)-\beta\bigl(g(Y')-g(Y)\bigr)-\delta\lVert Y'-Y\rVert_{2}.

By (E) with Z=X−YZ=X-Y, W=−(Y′−Y)W=-(Y'-Y), ∥X−Y′∥22−∥X−Y∥22=−2⟨X−Y,Y′−Y⟩2+∥Y′−Y∥22\lVert X-Y'\rVert_{2}^{2}-\lVert X-Y\rVert_{2}^{2}=-2\langle X-Y,Y'-Y\rangle_{2}+\lVert Y'-Y\rVert_{2}^{2}, and by (L), g(Y′)−g(Y)≤⟨21+tY,Y′−Y⟩2+∥Y′−Y∥22g(Y')-g(Y)\le\langle\frac{2}{1+t}Y,Y'-Y\rangle_{2}+\lVert Y'-Y\rVert_{2}^{2}. Hence

vN(Y′)≥v(ν)+⟨P,Y′−Y⟩2−(12ε+β)∥Y′−Y∥22−δ∥Y′−Y∥2≥v(ν)+⟨P,Y′−Y⟩2−(δ+η)∥Y′−Y∥2,v_{N}(Y')\ge v(\nu)+\langle P,Y'-Y\rangle_{2}-\Bigl(\tfrac{1}{2\varepsilon}+\beta\Bigr)\lVert Y'-Y\rVert_{2}^{2}-\delta\lVert Y'-Y\rVert_{2}\ge v(\nu)+\langle P,Y'-Y\rangle_{2}-(\delta+\eta)\lVert Y'-Y\rVert_{2},

so πv∈Jδ−v(ν)\pi_{v}\in J^{-}_{\delta}v(\nu) by Plan Superdifferentials, Plan Subdifferentials and Plan Jets with Slack on Square-Integrable Noncommutative Laws §sub and Plan Superdifferentials, Plan Subdifferentials and Plan Jets with Slack on Square-Integrable Noncommutative Laws §subjet.

Clause 3. Let a=∥X^∥2≥0a=\lVert\hat{X}\rVert_{2}\ge0. From 0≤(a−1)20\le(a-1)^{2} we get 2a≤1+a22a\le1+a^{2}, and trivially a2≤1+a2a^{2}\le1+a^{2}. Hence ∥q∥2=2βa/(1+a2)≤β\lVert q\rVert_{2}=2\beta a/(1+a^{2})\le\beta and (1+a)∥q∥2=2βa/(1+a2)+2βa2/(1+a2)≤β+2β=3β(1+a)\lVert q\rVert_{2}=2\beta a/(1+a^{2})+2\beta a^{2}/(1+a^{2})\le\beta+2\beta=3\beta. The same computation with ∥Y^∥2\lVert\hat{Y}\rVert_{2} bounds q′q'.

Clause 4. Let B≥0B\ge0 be real with ∣u∣≤B|u|\le B and ∣v∣≤B|v|\le B on Σd2\Sigma^{2}_{d} (Bounded Real-Valued Function on a Set). Since I≥0\mathcal{I}\ge0 by Calculus of Square-Integrable Noncommutative Laws: Agreement on Bounded Laws, Lipschitz Estimates, Functoriality of Push-Forwards, Moment Formulas, Positivity, the Cost and the Diagonal Coupling §cost and G≥0G\ge0 (as log⁡(1+s)≥1−(1+s)−1≥0\log(1+s)\ge1-(1+s)^{-1}\ge0 for s≥0s\ge0 by The Function slog⁡ss\log s: Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm §log), Φ≤2B\Phi\le2B and Φ′≤2B\Phi'\le2B, so both suprema exist (Approximation Property of the Supremum and the Infimum in R\mathbb{R}). By the definitions of Φ\Phi and Φ′\Phi' and Every Square-Integrable Noncommutative Law is the Law of a Square-Integrable Tuple; Realisation of Couplings and of Almost Optimal Pairs §coupling (I(γ^)=D2\mathcal{I}(\hat{\gamma})=D^{2}), Φ′(γ^)=Φ(γ^)+(12ε−14ε)D2=Φ(γ^)+14εD2\Phi'(\hat{\gamma})=\Phi(\hat{\gamma})+(\frac{1}{2\varepsilon}-\frac{1}{4\varepsilon})D^{2}=\Phi(\hat{\gamma})+\frac{1}{4\varepsilon}D^{2}. Hence 14εD2=Φ′(γ^)−Φ(γ^)≤sup⁡Φ′−(sup⁡Φ−κ)\frac{1}{4\varepsilon}D^{2}=\Phi'(\hat{\gamma})-\Phi(\hat{\gamma})\le\sup\Phi'-(\sup\Phi-\kappa).

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