TheoremBase

Weak convergence of the graph couplings, tested against truncated bounded continuous functions with an error controlled by the uniform L2 bound, gives convergence of the coordinate pairings with cylindrical functions. Since such test fields are dense, the inner products with v converge, and expanding the squared norm of vjv_j - v together with the norm bound gives strong convergence.

Proof

Each result cited is universally quantified over the data in its own statement. Elementary order and arithmetic of real numbers, including finite sums, squares, maxima and minima, is used through The Real Numbers: Standing Notation and Background §background without further citation.

Step 0 (Notation). By Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §noise-space and The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §basis, the vectors fk=ak1/2ekf_{k}=a_{k}^{1/2}e_{k}, k∈Nk\in\mathbb{N}, form an orthonormal basis of the real Hilbert space XaX^{a}. By Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields, L2(μ;Xa)L^{2}(\mu;X^{a}) is the space of The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §classes taken with the measure space (X,B(X),μ)(X,\mathcal{B}(X),\mu), with E=XaE=X^{a} and with this basis, and its inner product ⟨⋅,⋅⟩μ\langle\cdot,\cdot\rangle_{\mu} and norm ∥⋅∥μ\lVert\cdot\rVert_{\mu} are those of The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §operations; by Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields it is a real Hilbert space, in particular a real inner product space whose norm is ∥⋅∥μ\lVert\cdot\rVert_{\mu}, so that ⟨u,u⟩μ=∥u∥μ2\langle u,u\rangle_{\mu}=\lVert u\rVert_{\mu}^{2} by Real Inner Product Space §norm. Let L2(μ)=L2(X,B(X),μ)L^{2}(\mu)=L^{2}(X,\mathcal{B}(X),\mu), a real inner product space with the inner product ⟨⋅,⋅⟩L2(μ)\langle\cdot,\cdot\rangle_{L^{2}(\mu)} and norm ∥⋅∥L2(μ)\lVert\cdot\rVert_{L^{2}(\mu)} of The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product; by that clause, for 22-integrable g,hg,h the product ghgh is integrable and ⟨g,h⟩L2(μ)=∫Xgh dμ\langle g,h\rangle_{L^{2}(\mu)}=\int_{X}gh\,d\mu, classes being written like their representatives.

For a noise displacement uu for μ\mu and k∈Nk\in\mathbb{N} let u[k]:X→Ru^{[k]}:X\to\mathbb{R} be the function u[k](x)=⟨u(x),fk⟩au^{[k]}(x)=\langle u(x),f_{k}\rangle_{a}; it is the kk-th coordinate of uu in the sense of Measurable Maps into a Hilbert Space with an Orthonormal Basis: Norms, Inner Products and Linear Combinations, Synthesis from Coordinates, Square-Integrability, and Almost-Everywhere Equality (written uku_{k} there; the bracket avoids a clash with the coordinates xkx_{k} of points of XX). It is Borel and 22-integrable with respect to μ\mu by Measurable Maps into a Hilbert Space with an Orthonormal Basis: Norms, Inner Products and Linear Combinations, Synthesis from Coordinates, Square-Integrability, and Almost-Everywhere Equality §operations and Measurable Maps into a Hilbert Space with an Orthonormal Basis: Norms, Inner Products and Linear Combinations, Synthesis from Coordinates, Square-Integrability, and Almost-Everywhere Equality §square-integrable, and its class in L2(μ)L^{2}(\mu), again written u[k]u^{[k]}, is the kk-th coordinate of the class u∈L2(μ;Xa)u\in L^{2}(\mu;X^{a}) in the sense of The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates. Since u(x)∈Xau(x)\in X^{a}, The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §basis gives

u[k](x)=ak−1/2⟨u(x),ek⟩(x∈X).(1)u^{[k]}(x)=a_{k}^{-1/2}\langle u(x),e_{k}\rangle\qquad(x\in X).\qquad(1)

By The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates the series ∑l=1∞∥u[l]∥L2(μ)2\sum_{l=1}^{\infty}\lVert u^{[l]}\rVert_{L^{2}(\mu)}^{2} converges with sum ∥u∥μ2\lVert u\rVert_{\mu}^{2}. Its terms are nonnegative, so its kk-th term is at most its kk-th partial sum, which is at most its sum by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §dominates; with The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product and Real Inner Product Space §norm this gives

∫X(u[k])2 dμ=∥u[k]∥L2(μ)2≤∥u∥μ2.(2)\int_{X}\bigl(u^{[k]}\bigr)^{2}\,d\mu=\lVert u^{[k]}\rVert_{L^{2}(\mu)}^{2}\le\lVert u\rVert_{\mu}^{2}.\qquad(2)

Write γu=(id,id+u)#μ∈P(X×X)\gamma_{u}=(\mathrm{id},\mathrm{id}+u)_{\#}\mu\in\mathcal{P}(X\times X), defined as in the statement, and γj=γvj\gamma_{j}=\gamma_{v_{j}}, γ=γv\gamma=\gamma_{v}; the hypothesis says γj⇒γ\gamma_{j}\Rightarrow\gamma.

Step 1 (A common bound). By the hypothesis with ε=1\varepsilon=1 there is J0∈NJ_{0}\in\mathbb{N} with ∥vj∥μ≤∥v∥μ+1\lVert v_{j}\rVert_{\mu}\le\lVert v\rVert_{\mu}+1 for J0≤jJ_{0}\le j. Put B=∥v∥μ+1B=\lVert v\rVert_{\mu}+1; then 1≤B1\le B, ∥v∥μ≤B\lVert v\rVert_{\mu}\le B and ∥vj∥μ≤B\lVert v_{j}\rVert_{\mu}\le B for J0≤jJ_{0}\le j, so by (2), for every k∈Nk\in\mathbb{N},

∥v[k]∥L2(μ)2≤B2,∥vj[k]∥L2(μ)2≤B2(J0≤j).(3)\lVert v^{[k]}\rVert_{L^{2}(\mu)}^{2}\le B^{2},\qquad\lVert v_{j}^{[k]}\rVert_{L^{2}(\mu)}^{2}\le B^{2}\quad(J_{0}\le j).\qquad(3)

Step 2 (Convergence against one cylindrical coordinate). Fix k∈Nk\in\mathbb{N} and φ∈FCb1(X)\varphi\in\mathcal{F}C^{1}_{b}(X); its class lies in L2(μ)L^{2}(\mu) by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §square-integrable. We show that (⟨vj[k],φ⟩L2(μ))j∈N\bigl(\langle v_{j}^{[k]},\varphi\rangle_{L^{2}(\mu)}\bigr)_{j\in\mathbb{N}} converges to ⟨v[k],φ⟩L2(μ)\langle v^{[k]},\varphi\rangle_{L^{2}(\mu)}.

By Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §bounded-borel, φ\varphi is bounded; fix a bound GG for it as in Bounded Real-Valued Function on a Set. Moreover φ\varphi is continuous: by Bounded C^1 Cylindrical Functions on a Hilbert Space with an Orthonormal Basis §cylindrical, φ=ψ∘pn\varphi=\psi\circ p_{n} with n∈Nn\in\mathbb{N} and ψ∈Cb1(Rn)\psi\in C^{1}_{b}(\mathbb{R}^{n}); ψ\psi is of class C1C^{1} on Rn\mathbb{R}^{n} by Bounded Continuously Differentiable Functions with Bounded Partial Derivatives on Euclidean Space §bounded, hence continuous on Rn\mathbb{R}^{n} as a map into (R,dR)(\mathbb{R},d_{\mathbb{R}}) by claims 1 and 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous; pnp_{n} is Lipschitz with constant 11 by Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §continuity, hence continuous by A Lipschitz Map is Uniformly Continuous and Continuous; so φ\varphi is continuous on XX by claim 3 of Semicontinuity and Continuity Under Composition with a Continuous Map.

For positive M∈RM\in\mathbb{R} let cM:R→Rc_{M}:\mathbb{R}\to\mathbb{R}, cM(s)=max⁡{−M,min⁡{M,s}}c_{M}(s)=\max\{-M,\min\{M,s\}\}. Then −M≤cM(s)≤M-M\le c_{M}(s)\le M, and cMc_{M} is the composite of s↦min⁡{M,s}s\mapsto\min\{M,s\} and t↦max⁡{−M,t}t\mapsto\max\{-M,t\}, each of which does not increase distances (elementary order arithmetic under The Real Numbers: Standing Notation and Background §background). Hence, for all s,s′∈Rs,s'\in\mathbb{R},

∣cM(s)∣≤M,∣cM(s)−cM(s′)∣≤∣s−s′∣,∣s−cM(s)∣≤s2M;(4)|c_{M}(s)|\le M,\qquad|c_{M}(s)-c_{M}(s')|\le|s-s'|,\qquad|s-c_{M}(s)|\le\frac{s^{2}}{M};\qquad(4)

for the last, cM(s)=sc_{M}(s)=s if ∣s∣≤M|s|\le M, and ∣s−cM(s)∣=∣s∣−M<∣s∣<s2/M|s-c_{M}(s)|=|s|-M<|s|<s^{2}/M if M<∣s∣M<|s|. Define FM:X×X→RF_{M}:X\times X\to\mathbb{R} by

FM(z)=φ(π1z) cM(ak−1/2⟨π2z−π1z,ek⟩).F_{M}(z)=\varphi(\pi_{1}z)\,c_{M}\bigl(a_{k}^{-1/2}\langle\pi_{2}z-\pi_{1}z,e_{k}\rangle\bigr).

By (4), ∣FM(z)∣≤GM|F_{M}(z)|\le GM for every zz, so FMF_{M} is bounded. It is continuous: let z∈X×Xz\in X\times X and let (zm)m∈N(z_{m})_{m\in\mathbb{N}} converge to zz in X×XX\times X. By Properties of the Product of Two Real Inner Product Spaces §componentwise, X×XX\times X being the product of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pairs, (πizm)m(\pi_{i}z_{m})_{m} converges to πiz\pi_{i}z in XX for i=1,2i=1,2. The coordinate function x↦⟨x,ek⟩x\mapsto\langle x,e_{k}\rangle is Lipschitz by Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §continuity, hence continuous by A Lipschitz Map is Uniformly Continuous and Continuous. By continuity of φ\varphi and of this function and Continuity Between Metric Spaces is Equivalent to Sequential Continuity §sequential, (φ(π1zm))m(\varphi(\pi_{1}z_{m}))_{m} converges to φ(π1z)\varphi(\pi_{1}z) and (⟨πizm,ek⟩)m(\langle\pi_{i}z_{m},e_{k}\rangle)_{m} converges to ⟨πiz,ek⟩\langle\pi_{i}z,e_{k}\rangle for i=1,2i=1,2, in (R,dR)(\mathbb{R},d_{\mathbb{R}}), equivalently in the sense of Limit of a Sequence of Real Numbers by The Real Numbers: Standing Notation and Background §sequences. Since ⟨π2z−π1z,ek⟩=⟨π2z,ek⟩−⟨π1z,ek⟩\langle\pi_{2}z-\pi_{1}z,e_{k}\rangle=\langle\pi_{2}z,e_{k}\rangle-\langle\pi_{1}z,e_{k}\rangle by Elementary Identities in a Real Inner Product Space §bilinear, and likewise for zmz_{m}, the numbers tm=ak−1/2⟨π2zm−π1zm,ek⟩t_{m}=a_{k}^{-1/2}\langle\pi_{2}z_{m}-\pi_{1}z_{m},e_{k}\rangle converge to t=ak−1/2⟨π2z−π1z,ek⟩t=a_{k}^{-1/2}\langle\pi_{2}z-\pi_{1}z,e_{k}\rangle by Arithmetic of Limits of Real Sequences §scalar; then (cM(tm))m(c_{M}(t_{m}))_{m} converges to cM(t)c_{M}(t) by (4), and (FM(zm))m(F_{M}(z_{m}))_{m} converges to FM(z)F_{M}(z) by Arithmetic of Limits of Real Sequences §products. Hence FMF_{M} is continuous on X×XX\times X by Continuity Between Metric Spaces is Equivalent to Sequential Continuity §on-subset, and Borel by claims 2 and 3 of Borel Measurability and Bounded Integration on a Metric Space.

Let uu be a noise displacement for μ\mu and x∈Xx\in X. Then π1(x,x+u(x))=x\pi_{1}(x,x+u(x))=x and π2(x,x+u(x))−π1(x,x+u(x))=u(x)\pi_{2}(x,x+u(x))-\pi_{1}(x,x+u(x))=u(x), so by (1)

FM(x,x+u(x))=φ(x) cM(u[k](x)).F_{M}\bigl(x,x+u(x)\bigr)=\varphi(x)\,c_{M}\bigl(u^{[k]}(x)\bigr).

Since FMF_{M} is bounded and Borel and γu\gamma_{u} is a Borel probability measure on X×XX\times X, FMF_{M} is integrable with respect to γu\gamma_{u} by claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space; by claim 2 of Image Measures, Measures with Densities, and Change of Variables, through Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pushforward, the function φ⋅(cM∘u[k])\varphi\cdot(c_{M}\circ u^{[k]}) is integrable with respect to μ\mu and

∫X×XFM dγu=∫Xφ(x) cM(u[k](x)) μ(dx).(5)\int_{X\times X}F_{M}\,d\gamma_{u}=\int_{X}\varphi(x)\,c_{M}\bigl(u^{[k]}(x)\bigr)\,\mu(dx).\qquad(5)

By Step 0, u[k]φu^{[k]}\varphi and (u[k])2(u^{[k]})^{2} are integrable and ⟨u[k],φ⟩L2(μ)=∫Xu[k]φ dμ\langle u^{[k]},\varphi\rangle_{L^{2}(\mu)}=\int_{X}u^{[k]}\varphi\,d\mu. The function hu=u[k]φ−φ⋅(cM∘u[k])h_{u}=u^{[k]}\varphi-\varphi\cdot(c_{M}\circ u^{[k]}) is integrable and, by (4), ∣hu(x)∣≤G ∣u[k](x)−cM(u[k](x))∣≤GM u[k](x)2|h_{u}(x)|\le G\,|u^{[k]}(x)-c_{M}(u^{[k]}(x))|\le\frac{G}{M}\,u^{[k]}(x)^{2} for every x∈Xx\in X. By Linearity and Monotonicity of the Lebesgue Integral §integrable, (5) and (2),

∣⟨u[k],φ⟩L2(μ)−∫X×XFM dγu∣=∣∫Xhu dμ∣≤∫X∣hu∣ dμ≤GM ∥u[k]∥L2(μ)2.(6)\Bigl|\langle u^{[k]},\varphi\rangle_{L^{2}(\mu)}-\int_{X\times X}F_{M}\,d\gamma_{u}\Bigr|=\Bigl|\int_{X}h_{u}\,d\mu\Bigr|\le\int_{X}|h_{u}|\,d\mu\le\frac{G}{M}\,\lVert u^{[k]}\rVert_{L^{2}(\mu)}^{2}.\qquad(6)

Now let ε>0\varepsilon>0. First choose M=1+3GB2/εM=1+3GB^{2}/\varepsilon; it is positive and GB2/M<ε/3GB^{2}/M<\varepsilon/3, since 3GB2<εM3GB^{2}<\varepsilon M. Next, FMF_{M} being bounded and continuous on X×XX\times X and γj⇒γ\gamma_{j}\Rightarrow\gamma in the sense of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §weak, Weak Convergence of Finite Borel Measures on a Metric Space and Limit of a Sequence of Real Numbers give J1∈NJ_{1}\in\mathbb{N} with ∣∫FM dγj−∫FM dγ∣<ε/3\bigl|\int F_{M}\,d\gamma_{j}-\int F_{M}\,d\gamma\bigr|<\varepsilon/3 for J1≤jJ_{1}\le j. For j≥max⁡{J0,J1}j\ge\max\{J_{0},J_{1}\}, (6) with u=vju=v_{j} and with u=vu=v, together with (3), gives

∣⟨vj[k],φ⟩L2(μ)−⟨v[k],φ⟩L2(μ)∣<GB2M+ε3+GB2M<ε.\bigl|\langle v_{j}^{[k]},\varphi\rangle_{L^{2}(\mu)}-\langle v^{[k]},\varphi\rangle_{L^{2}(\mu)}\bigr|<\frac{GB^{2}}{M}+\frac{\varepsilon}{3}+\frac{GB^{2}}{M}<\varepsilon .

As ε\varepsilon was arbitrary, the claim of this step follows by Limit of a Sequence of Real Numbers.

Step 3 (Cylindrical test fields). Let m∈Nm\in\mathbb{N} and φ1,…,φm∈FCb1(X)\varphi_{1},\dots,\varphi_{m}\in\mathcal{F}C^{1}_{b}(X). Let hl∈L2(μ)h_{l}\in L^{2}(\mu) be the class of φl\varphi_{l} for l≤ml\le m, which exists by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §square-integrable, and the zero vector for m<lm<l. The partial sums of ∑l=1∞∥hl∥L2(μ)2\sum_{l=1}^{\infty}\lVert h_{l}\rVert_{L^{2}(\mu)}^{2} are constant from index mm on, so the series converges by Series of Real Numbers §convergent, and The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §synthesis gives w∈L2(μ;Xa)w\in L^{2}(\mu;X^{a}) whose ll-th coordinate in the sense of The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates is hlh_{l} for every l∈Nl\in\mathbb{N}; call ww the test field of (φ1,…,φm)(\varphi_{1},\dots,\varphi_{m}). For u∈L2(μ;Xa)u\in L^{2}(\mu;X^{a}) with coordinates u[l]u^{[l]}, The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates gives ⟨u,w⟩μ=∑l=1∞⟨u[l],hl⟩L2(μ)\langle u,w\rangle_{\mu}=\sum_{l=1}^{\infty}\langle u^{[l]},h_{l}\rangle_{L^{2}(\mu)}, whose terms with m<lm<l vanish by Elementary Identities in a Real Inner Product Space §zero; the partial sums are therefore constant from index mm on, and

⟨u,w⟩μ=∑l=1m⟨u[l],φl⟩L2(μ).(7)\langle u,w\rangle_{\mu}=\sum_{l=1}^{m}\langle u^{[l]},\varphi_{l}\rangle_{L^{2}(\mu)}.\qquad(7)

By (7), Step 2 applied with (k,φ)=(l,φl)(k,\varphi)=(l,\varphi_{l}) for each l≤ml\le m, and Arithmetic of Limits of Real Sequences §sums applied m−1m-1 times,

lim⁡j→∞⟨vj,w⟩μ=⟨v,w⟩μ.(8)\lim_{j\to\infty}\langle v_{j},w\rangle_{\mu}=\langle v,w\rangle_{\mu}.\qquad(8)

Step 4 (Approximation of vv by test fields). We show: for every δ>0\delta>0 there is a test field ww with ∥v−w∥μ<δ\lVert v-w\rVert_{\mu}<\delta. Let δ>0\delta>0; first mm, then φ1,…,φm\varphi_{1},\dots,\varphi_{m} are chosen. Let sn=∑l=1n∥v[l]∥L2(μ)2s_{n}=\sum_{l=1}^{n}\lVert v^{[l]}\rVert_{L^{2}(\mu)}^{2}. By The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates and Series of Real Numbers §convergent, (sn)n(s_{n})_{n} converges to ∥v∥μ2\lVert v\rVert_{\mu}^{2}, and sn≤∥v∥μ2s_{n}\le\lVert v\rVert_{\mu}^{2} by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §dominates; by Limit of a Sequence of Real Numbers choose m∈Nm\in\mathbb{N} with ∥v∥μ2−sm<δ2/2\lVert v\rVert_{\mu}^{2}-s_{m}<\delta^{2}/2. Next, the set of the classes of the functions in FCb1(X)\mathcal{F}C^{1}_{b}(X) is dense in L2(μ)L^{2}(\mu) by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §density, that is, by Real Hilbert Space §topology and Dense Subset of a Topological Space, its closure for the distance of Real Inner Product Space §distance is L2(μ)L^{2}(\mu); so by Characterization of the Closure in a Metric Space by Open Balls (claim 1 implies claim 3) choose, for each l≤ml\le m, φl∈FCb1(X)\varphi_{l}\in\mathcal{F}C^{1}_{b}(X) with ∥v[l]−φl∥L2(μ)<δ/(2m)\lVert v^{[l]}-\varphi_{l}\rVert_{L^{2}(\mu)}<\delta/(2m). Let ww be the test field of (φ1,…,φm)(\varphi_{1},\dots,\varphi_{m}). By The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates, applied to v−w=v+(−1)wv-w=v+(-1)w, the ll-th coordinate of v−wv-w is v[l]−φlv^{[l]}-\varphi_{l} for l≤ml\le m and v[l]v^{[l]} for m<lm<l, and ∥v−w∥μ2\lVert v-w\rVert_{\mu}^{2} is the sum of the series of their squared norms in L2(μ)L^{2}(\mu). For m≤nm\le n the nn-th partial sum of that series is

∑l=1m∥v[l]−φl∥L2(μ)2+(sn−sm)<m δ24m2+(∥v∥μ2−sm)<δ24+δ22,\sum_{l=1}^{m}\lVert v^{[l]}-\varphi_{l}\rVert_{L^{2}(\mu)}^{2}+(s_{n}-s_{m})<m\,\frac{\delta^{2}}{4m^{2}}+\bigl(\lVert v\rVert_{\mu}^{2}-s_{m}\bigr)<\frac{\delta^{2}}{4}+\frac{\delta^{2}}{2},

and for n<mn<m it is at most the mm-th partial sum, the terms being nonnegative. By Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §criterion the sum is the supremum of the partial sums, so ∥v−w∥μ2≤3δ2/4<δ2\lVert v-w\rVert_{\mu}^{2}\le3\delta^{2}/4<\delta^{2}, and ∥v−w∥μ<δ\lVert v-w\rVert_{\mu}<\delta.

Step 5 (Convergence of the inner products). We show lim⁡j→∞⟨vj,v⟩μ=∥v∥μ2\lim_{j\to\infty}\langle v_{j},v\rangle_{\mu}=\lVert v\rVert_{\mu}^{2}. Let ε>0\varepsilon>0; first put δ=ε/(3B)\delta=\varepsilon/(3B), then choose by Step 4 a test field ww with ∥v−w∥μ<δ\lVert v-w\rVert_{\mu}<\delta, then by (8) choose J2∈NJ_{2}\in\mathbb{N} with ∣⟨vj,w⟩μ−⟨v,w⟩μ∣<ε/3|\langle v_{j},w\rangle_{\mu}-\langle v,w\rangle_{\mu}|<\varepsilon/3 for J2≤jJ_{2}\le j. Let j≥max⁡{J0,J2}j\ge\max\{J_{0},J_{2}\}. By Elementary Identities in a Real Inner Product Space §bilinear in L2(μ;Xa)L^{2}(\mu;X^{a}) and ⟨v,v⟩μ=∥v∥μ2\langle v,v\rangle_{\mu}=\lVert v\rVert_{\mu}^{2},

⟨vj,v⟩μ−∥v∥μ2=⟨vj,v−w⟩μ+(⟨vj,w⟩μ−⟨v,w⟩μ)+⟨v,w−v⟩μ.\langle v_{j},v\rangle_{\mu}-\lVert v\rVert_{\mu}^{2}=\langle v_{j},v-w\rangle_{\mu}+\bigl(\langle v_{j},w\rangle_{\mu}-\langle v,w\rangle_{\mu}\bigr)+\langle v,w-v\rangle_{\mu}.

By The Cauchy-Schwarz Inequality in a Real Inner Product Space in L2(μ;Xa)L^{2}(\mu;X^{a}), Elementary Identities in a Real Inner Product Space §homogeneity (giving ∥w−v∥μ=∥v−w∥μ\lVert w-v\rVert_{\mu}=\lVert v-w\rVert_{\mu}) and Step 1,

∣⟨vj,v⟩μ−∥v∥μ2∣<Bδ+ε3+Bδ=ε.\bigl|\langle v_{j},v\rangle_{\mu}-\lVert v\rVert_{\mu}^{2}\bigr|<B\delta+\frac{\varepsilon}{3}+B\delta=\varepsilon .

The claim follows by Limit of a Sequence of Real Numbers.

Step 6 (Conclusion). Let ε>0\varepsilon>0. First put η=min⁡{1,ε2/(2(2∥v∥μ+3))}\eta=\min\bigl\{1,\varepsilon^{2}/\bigl(2(2\lVert v\rVert_{\mu}+3)\bigr)\bigr\}, which is positive; then choose by the hypothesis J3∈NJ_{3}\in\mathbb{N} with ∥vj∥μ≤∥v∥μ+η\lVert v_{j}\rVert_{\mu}\le\lVert v\rVert_{\mu}+\eta for J3≤jJ_{3}\le j, and by Step 5 J4∈NJ_{4}\in\mathbb{N} with ∣⟨vj,v⟩μ−∥v∥μ2∣<η|\langle v_{j},v\rangle_{\mu}-\lVert v\rVert_{\mu}^{2}|<\eta for J4≤jJ_{4}\le j. Let j≥max⁡{J3,J4}j\ge\max\{J_{3},J_{4}\}. Since 0≤∥vj∥μ≤∥v∥μ+η0\le\lVert v_{j}\rVert_{\mu}\le\lVert v\rVert_{\mu}+\eta and η2≤η\eta^{2}\le\eta,

∥vj∥μ2≤∥v∥μ2+2η∥v∥μ+η2≤∥v∥μ2+η(2∥v∥μ+1).\lVert v_{j}\rVert_{\mu}^{2}\le\lVert v\rVert_{\mu}^{2}+2\eta\lVert v\rVert_{\mu}+\eta^{2}\le\lVert v\rVert_{\mu}^{2}+\eta\bigl(2\lVert v\rVert_{\mu}+1\bigr).

By Elementary Identities in a Real Inner Product Space §expansion in L2(μ;Xa)L^{2}(\mu;X^{a}),

∥vj−v∥μ2=(∥vj∥μ2−∥v∥μ2)−2(⟨vj,v⟩μ−∥v∥μ2)<η(2∥v∥μ+1)+2η≤ε22<ε2.\lVert v_{j}-v\rVert_{\mu}^{2}=\bigl(\lVert v_{j}\rVert_{\mu}^{2}-\lVert v\rVert_{\mu}^{2}\bigr)-2\bigl(\langle v_{j},v\rangle_{\mu}-\lVert v\rVert_{\mu}^{2}\bigr)<\eta\bigl(2\lVert v\rVert_{\mu}+1\bigr)+2\eta\le\frac{\varepsilon^{2}}{2}<\varepsilon^{2}.

As 0≤∥vj−v∥μ0\le\lVert v_{j}-v\rVert_{\mu}, this gives ∣∥vj−v∥μ−0∣<ε\bigl|\lVert v_{j}-v\rVert_{\mu}-0\bigr|<\varepsilon for every j≥max⁡{J3,J4}j\ge\max\{J_{3},J_{4}\}. Since ε\varepsilon was arbitrary, lim⁡j→∞∥vj−v∥μ=0\lim_{j\to\infty}\lVert v_{j}-v\rVert_{\mu}=0 by Limit of a Sequence of Real Numbers.

Citations

Loading…

Dependencies

Uses0

Loading…

Comments

Log in to comment.

Loading…