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The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis

The space of square-integrable Hilbert-valued maps is a real Hilbert space; its inner product is the sum of the scalar L2L^2 inner products of the coordinates, and every square-summable sequence of scalar classes is the coordinate sequence of exactly one element.

Statement

In the settings of The Real Numbers: Standing Notation and Background and Measure Spaces and the Lebesgue Integral: Standing Notation, the measure space of the latter being instantiated at each use by the measure space named, let (S,S,μ)(S,\mathcal{S},\mu) be a measure space, let EE be a real Hilbert space with inner product ⟨⋅,⋅⟩E\langle\cdot,\cdot\rangle_{E}, norm ∣⋅∣E|\cdot|_{E} and an orthonormal basis (fk)k∈N(f_{k})_{k\in\mathbb{N}}, and let the space L2(μ;E)L^{2}(\mu;E) of square-integrable maps, with its operations, inner product ⟨⋅,⋅⟩L2(μ;E)\langle\cdot,\cdot\rangle_{L^{2}(\mu;E)} and norm ∥⋅∥L2(μ;E)\lVert\cdot\rVert_{L^{2}(\mu;E)}, be those of that definition, and the coordinates vk(s)=⟨v(s),fk⟩Ev_{k}(s)=\langle v(s),f_{k}\rangle_{E} of maps v:S→Ev:S\to E as in 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. Let L2(μ)=L2(S,S,μ)L^{2}(\mu)=L^{2}(S,\mathcal{S},\mu) be the real Hilbert space of The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §hilbert, 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.

1. (A real Hilbert space) With the operations, inner product and norm of The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §operations, L2(μ;E)L^{2}(\mu;E) is a real Hilbert space whose zero vector is the class of the constant map with value the zero vector of EE, and ∥⋅∥L2(μ;E)\lVert\cdot\rVert_{L^{2}(\mu;E)} is the norm of its inner product.

2. (Coordinates) For v∈L2(μ;E)v\in L^{2}(\mu;E) and k∈Nk\in\mathbb{N}, the class in L2(μ)L^{2}(\mu) of the coordinate vkv_{k} of a representative of vv does not depend on the representative; it is again written vkv_{k}. For v,w∈L2(μ;E)v,w\in L^{2}(\mu;E), t∈Rt\in\mathbb{R} and k∈Nk\in\mathbb{N} one has (v+w)k=vk+wk(v+w)_{k}=v_{k}+w_{k} and (tv)k=t vk(tv)_{k}=t\,v_{k}; the series ∑k=1∞⟨vk,wk⟩L2(μ)\sum_{k=1}^{\infty}\langle v_{k},w_{k}\rangle_{L^{2}(\mu)} and ∑k=1∞∥vk∥L2(μ)2\sum_{k=1}^{\infty}\lVert v_{k}\rVert_{L^{2}(\mu)}^{2} converge, with

⟨v,w⟩L2(μ;E)=∑k=1∞⟨vk,wk⟩L2(μ),∥v∥L2(μ;E)2=∑k=1∞∥vk∥L2(μ)2.\langle v,w\rangle_{L^{2}(\mu;E)}=\sum_{k=1}^{\infty}\langle v_{k},w_{k}\rangle_{L^{2}(\mu)},\qquad\lVert v\rVert_{L^{2}(\mu;E)}^{2}=\sum_{k=1}^{\infty}\lVert v_{k}\rVert_{L^{2}(\mu)}^{2}.

3. (Synthesis) Let (gk)k∈N(g_{k})_{k\in\mathbb{N}} be a sequence in L2(μ)L^{2}(\mu) such that the series ∑k=1∞∥gk∥L2(μ)2\sum_{k=1}^{\infty}\lVert g_{k}\rVert_{L^{2}(\mu)}^{2} converges. Then there is exactly one v∈L2(μ;E)v\in L^{2}(\mu;E) with vk=gkv_{k}=g_{k} for every k∈Nk\in\mathbb{N}.

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