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Proof of A Square-Integrable Vector Field Whose Displacement Pairings Vanish to First Order is Zero

lemmalem:coupling-derivative-unique-wasserstein-2026a
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· 5,634 chars · 15 deps · depth 35 Reason: Proof by testing the hypothesis against the displacement couplings induced by the maps id + t xi, then dividing by t and letting the slack tend to zero.

Test the hypothesis against the displacement couplings induced by the maps id + t xi, whose cost is t2t^2 times the squared norm of xi and whose pairing with the field is t times the inner product; divide by t and let the slack tend to zero.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied here to the data named in the statement above.

Step 1: the pairings along displacement couplings. Let ξL2(μ;Rd)\xi\in L^{2}(\mu;\mathbb{R}^{d}) and let tRt\in\mathbb{R} be positive. Fix a representative of ξ\xi, again written ξ\xi: a Borel map RdRd\mathbb{R}^{d}\to\mathbb{R}^{d} with Rdξ2dμ<\int_{\mathbb{R}^{d}}\lVert\xi\rVert^{2}\,d\mu<\infty, by Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §fields. Let SS be the map xx+tξ(x)x\mapsto x+t\,\xi(x). Each component of SS is the sum of a coordinate map and a real scalar multiple of a Borel real function, hence Borel by claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and a map into Rd\mathbb{R}^{d} with Borel components is Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps; so SS is Borel.

The map SidS-\mathrm{id} is xtξ(x)x\mapsto t\,\xi(x), which represents the class tξt\,\xi of L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) by Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §fields. By the absolute homogeneity of the Euclidean norm, claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, and t=t|t|=t for the positive tt --- by claim 1 of Properties of the Absolute Value in an Ordered Field the value t|t| is tt or t-t, and t=t|t|=-t would give 0t0\le-t, hence t0t\le0 by claim 4 of Elementary Order Arithmetic in an Ordered Field, contradicting 0<t0<t --- one has tξ(x)2=t2ξ(x)2\lVert t\,\xi(x)\rVert^{2}=t^{2}\lVert\xi(x)\rVert^{2} for every xx, so by claim 1 of Linearity and Monotonicity of the Lebesgue Integral

RdSid2dμ=t2Rdξ2dμ=t2ξμ2<.\int_{\mathbb{R}^{d}}\lVert S-\mathrm{id}\rVert^{2}\,d\mu=t^{2}\int_{\mathbb{R}^{d}}\lVert\xi\rVert^{2}\,d\mu=t^{2}\,\lVert\xi\rVert_{\mu}^{2}<\infty .

Therefore The Displacement Pairing of a Square-Integrable Vector Field Along a Coupling §displacement applies to SS: the push-forward S#μS_{\#}\mu belongs to P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}), the coupling πS=(id,S)#μ\pi_{S}=(\mathrm{id},S)_{\#}\mu belongs to Π(μ,S#μ)\Pi(\mu,S_{\#}\mu) with

I(πS)=Sidμ2=t2ξμ2=(tξμ)2,I(\pi_{S})=\lVert S-\mathrm{id}\rVert_{\mu}^{2}=t^{2}\lVert\xi\rVert_{\mu}^{2}=\bigl(t\,\lVert\xi\rVert_{\mu}\bigr)^{2},

and, η\eta being the field of the statement,

J(η,πS)=η,Sidμ=η,tξμ=tη,ξμ,\mathcal{J}(\eta,\pi_{S})=\langle\eta,\,S-\mathrm{id}\rangle_{\mu}=\langle\eta,\,t\,\xi\rangle_{\mu}=t\,\langle\eta,\xi\rangle_{\mu},

the last equality by the homogeneity of the inner product in its second argument, Elementary Identities in a Real Inner Product Space §bilinear.

Step 2: the estimate on the inner products. We show that η,ξμ=0\langle\eta,\xi\rangle_{\mu}=0 for every ξL2(μ;Rd)\xi\in L^{2}(\mu;\mathbb{R}^{d}).

If ξμ=0\lVert\xi\rVert_{\mu}=0 then ξ\xi is the zero class by Elementary Identities in a Real Inner Product Space §vanishing and η,ξμ=0\langle\eta,\xi\rangle_{\mu}=0 by Elementary Identities in a Real Inner Product Space §zero. So assume ξμ\lVert\xi\rVert_{\mu} is positive, the norm being nonnegative.

Let εR\varepsilon\in\mathbb{R} be positive. Then εξμ1\varepsilon\,\lVert\xi\rVert_{\mu}^{-1} is positive by claims 7 and 5 of Elementary Order Arithmetic in an Ordered Field; let θ\theta be a positive real supplied by the hypothesis of the statement for that positive number in place of the ε\varepsilon there. The number θξμ1\theta\,\lVert\xi\rVert_{\mu}^{-1} is positive by the same two claims, and t=θξμ121t=\theta\,\lVert\xi\rVert_{\mu}^{-1}\cdot2^{-1} is positive with t<θξμ1t<\theta\,\lVert\xi\rVert_{\mu}^{-1}, by claim 8 of Elementary Order Arithmetic in an Ordered Field. Multiplying that strict inequality by the positive ξμ\lVert\xi\rVert_{\mu}, by claim 10 of Elementary Order Arithmetic in an Ordered Field, gives tξμ<θt\,\lVert\xi\rVert_{\mu}<\theta; both sides being nonnegative, claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives (tξμ)2<θ2(t\,\lVert\xi\rVert_{\mu})^{2}<\theta^{2}, that is I(πS)<θ2I(\pi_{S})<\theta^{2} for the SS built from this ξ\xi and tt in step 1.

The hypothesis of the statement, applied to ν=S#μ\nu=S_{\#}\mu and π=πS\pi=\pi_{S}, therefore yields

J(η,πS)εξμ1I(πS).\bigl|\mathcal{J}(\eta,\pi_{S})\bigr|\le\varepsilon\,\lVert\xi\rVert_{\mu}^{-1}\,\sqrt{I(\pi_{S})} .

Here I(πS)=tξμ\sqrt{I(\pi_{S})}=t\,\lVert\xi\rVert_{\mu} by Existence and Uniqueness of the Nonnegative Square Root, that number being nonnegative with square I(πS)I(\pi_{S}); and J(η,πS)=tη,ξμ=tη,ξμ|\mathcal{J}(\eta,\pi_{S})|=|t\,\langle\eta,\xi\rangle_{\mu}|=t\,|\langle\eta,\xi\rangle_{\mu}| by step 1, the multiplicativity of the absolute value (claim 4 of Properties of the Absolute Value in an Ordered Field) and t=t|t|=t, established in step 1. So

tη,ξμεξμ1tξμ=εt,t\,\bigl|\langle\eta,\xi\rangle_{\mu}\bigr|\le\varepsilon\,\lVert\xi\rVert_{\mu}^{-1}\,t\,\lVert\xi\rVert_{\mu}=\varepsilon\,t ,

using the associativity and commutativity of multiplication in the field of Field and ξμ1ξμ=1\lVert\xi\rVert_{\mu}^{-1}\lVert\xi\rVert_{\mu}=1. Multiplying by the positive t1t^{-1} (claim 7 of Elementary Order Arithmetic in an Ordered Field), by claim 5 of Elementary Arithmetic in an Ordered Field, gives

η,ξμε.\bigl|\langle\eta,\xi\rangle_{\mu}\bigr|\le\varepsilon .

As ε\varepsilon was an arbitrary positive real and η,ξμ|\langle\eta,\xi\rangle_{\mu}| is nonnegative by claim 1 of Properties of the Absolute Value in an Ordered Field, Comparison of Real Numbers with Arbitrary Positive Slack §vanishing gives η,ξμ=0|\langle\eta,\xi\rangle_{\mu}|=0, whence η,ξμ=0\langle\eta,\xi\rangle_{\mu}=0 by claim 1 of Properties of the Absolute Value in an Ordered Field again.

Step 3: conclusion. Taking ξ=η\xi=\eta in step 2 gives η,ημ=0\langle\eta,\eta\rangle_{\mu}=0, that is ημ=0\lVert\eta\rVert_{\mu}=0 by Real Inner Product Space §norm and Existence and Uniqueness of the Nonnegative Square Root. Hence η\eta is the zero element of L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) by Elementary Identities in a Real Inner Product Space §vanishing.

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