TheoremBase

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

Measurable maps into a Hilbert space with an orthonormal basis are closed under linear combinations and have measurable norms, inner products and coordinates; square-summable measurable coordinates synthesise a measurable map; square-integrable maps have integrable inner products with the Cauchy-Schwarz bound; and almost-everywhere equality is a compatible equivalence relation.

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 EE be a real Hilbert space with inner product ⟨⋅,⋅⟩E\langle\cdot,\cdot\rangle_{E} and norm ∣⋅∣E|\cdot|_{E}, let (fk)k∈N(f_{k})_{k\in\mathbb{N}} be an orthonormal basis of EE, and let B(E)\mathcal{B}(E) be the Borel σ\sigma-algebra of EE for the distance of its norm. Let (S,S)(S,\mathcal{S}) be a measurable space. Measurability of a map S→ES\to E is taken with respect to S\mathcal{S} and B(E)\mathcal{B}(E), and of a function S→RS\to\mathbb{R} with respect to S\mathcal{S} and the Borel σ\sigma-algebra of the real line, both in the sense of Measurable Function and Real-Valued Measurable Function. For maps v,w:S→Ev,w:S\to E, t∈Rt\in\mathbb{R} and k∈Nk\in\mathbb{N}, the maps v+wv+w and tvtv are taken pointwise, vk:S→Rv_{k}:S\to\mathbb{R} is the function vk(s)=⟨v(s),fk⟩Ev_{k}(s)=\langle v(s),f_{k}\rangle_{E}, and ∣v∣E2|v|_{E}^{2} and ⟨v,w⟩E\langle v,w\rangle_{E} denote the functions s↦∣v(s)∣E2s\mapsto|v(s)|_{E}^{2} and s↦⟨v(s),w(s)⟩Es\mapsto\langle v(s),w(s)\rangle_{E}.

1. (Operations) Let v,w:S→Ev,w:S\to E be measurable and t∈Rt\in\mathbb{R}. Then v+wv+w and tvtv are measurable, and the functions vkv_{k} (k∈Nk\in\mathbb{N}), ∣v∣E2|v|_{E}^{2} and ⟨v,w⟩E\langle v,w\rangle_{E} are measurable. For every s∈Ss\in S the series ∑k=1∞vk(s)2\sum_{k=1}^{\infty}v_{k}(s)^{2} converges, and its sum is ∣v(s)∣E2|v(s)|_{E}^{2}.

2. (Synthesis) Let (gk)k∈N(g_{k})_{k\in\mathbb{N}} be a sequence of measurable functions gk:S→Rg_{k}:S\to\mathbb{R} such that for every s∈Ss\in S the series ∑k=1∞gk(s)2\sum_{k=1}^{\infty}g_{k}(s)^{2} converges. Then for every s∈Ss\in S the series ∑k=1∞gk(s)fk\sum_{k=1}^{\infty}g_{k}(s)f_{k} converges in EE, and the map v:S→Ev:S\to E, v(s)=∑k=1∞gk(s)fkv(s)=\sum_{k=1}^{\infty}g_{k}(s)f_{k}, is measurable with vk=gkv_{k}=g_{k} for every k∈Nk\in\mathbb{N}.

3. (Square-integrability) Let μ\mu be a measure on S\mathcal{S}, let v,w:S→Ev,w:S\to E be measurable with ∫S∣v∣E2 dμ<∞\int_{S}|v|_{E}^{2}\,d\mu<\infty and ∫S∣w∣E2 dμ<∞\int_{S}|w|_{E}^{2}\,d\mu<\infty, and let t∈Rt\in\mathbb{R}. Then ∫S∣v+w∣E2 dμ<∞\int_{S}|v+w|_{E}^{2}\,d\mu<\infty and ∫S∣tv∣E2 dμ<∞\int_{S}|tv|_{E}^{2}\,d\mu<\infty; for every k∈Nk\in\mathbb{N} the function vkv_{k} is 22-integrable in the sense of Power-Integrable Functions and the p-Seminorm §space; the function ⟨v,w⟩E\langle v,w\rangle_{E} is integrable with respect to μ\mu; and

∣∫S⟨v,w⟩E dμ∣≤(∫S∣v∣E2 dμ)1/2(∫S∣w∣E2 dμ)1/2.\Bigl|\int_{S}\langle v,w\rangle_{E}\,d\mu\Bigr|\le\Bigl(\int_{S}|v|_{E}^{2}\,d\mu\Bigr)^{1/2}\Bigl(\int_{S}|w|_{E}^{2}\,d\mu\Bigr)^{1/2}.

4. (Almost-everywhere equality) Let μ\mu be a measure on S\mathcal{S}. For measurable u,u′:S→Eu,u':S\to E the set {s∈S:u(s)≠u′(s)}\{s\in S:u(s)\ne u'(s)\} belongs to S\mathcal{S}; write u∼μu′u\sim_{\mu}u' if it has μ\mu-measure 00. On the set of measurable maps S→ES\to E the relation ∼μ\sim_{\mu} is an equivalence relation. Let v,v′,w,w′:S→Ev,v',w,w':S\to E be measurable with v∼μv′v\sim_{\mu}v' and w∼μw′w\sim_{\mu}w', and let t∈Rt\in\mathbb{R}. Then v+w∼μv′+w′v+w\sim_{\mu}v'+w' and tv∼μtv′tv\sim_{\mu}tv'. If moreover ∫S∣v∣E2 dμ<∞\int_{S}|v|_{E}^{2}\,d\mu<\infty and ∫S∣w∣E2 dμ<∞\int_{S}|w|_{E}^{2}\,d\mu<\infty, then ∫S∣v′∣E2 dμ<∞\int_{S}|v'|_{E}^{2}\,d\mu<\infty, ∫S∣w′∣E2 dμ<∞\int_{S}|w'|_{E}^{2}\,d\mu<\infty,

∫S∣v′∣E2 dμ=∫S∣v∣E2 dμ,∫S⟨v′,w′⟩E dμ=∫S⟨v,w⟩E dμ,\int_{S}|v'|_{E}^{2}\,d\mu=\int_{S}|v|_{E}^{2}\,d\mu,\qquad\int_{S}\langle v',w'\rangle_{E}\,d\mu=\int_{S}\langle v,w\rangle_{E}\,d\mu,

and for every k∈Nk\in\mathbb{N} the classes [vk][v_{k}] and [vk′][v'_{k}] of The Lebesgue Space of Power-Integrable Functions §equivalence coincide.

Proofs

Log in to submit a proof.

Loading...

Citations

Loading…

Dependencies

Loading…

Related

0 relations

Curated associations between results. These are editable and subjective — they do not replace the dependency graph, which is derived from the references in the text.

No relations recorded yet.

Comments

Log in to comment.

Loading…