TheoremBase

Work in the probability space (Ω, G, P restricted to G): the indefinite integral of X over the sets of G is a finite signed measure absolutely continuous with respect to it, so the Radon–Nikodym theorem gives a G-measurable density, and integrals of G-measurable functions are the same for P and its restriction. Uniqueness is the uniqueness of densities, and the vector case is componentwise.

Proof

Throughout, P∣GP|_{\mathcal{G}} denotes the restriction of PP to G\mathcal{G}, a probability measure on (Ω,G)(\Omega,\mathcal{G}) (Finite Signed Measures from Finite Measures and from Integrals (iii)); it is σ\sigma-finite, the constant sequence Ω\Omega witnessing this (Measure, Measure Space, and Probability Measure (iv)), so the Radon–Nikodym theorem applies in the measure space (Ω,G,P∣G)(\Omega,\mathcal{G},P|_{\mathcal{G}}). A G\mathcal{G}-measurable Y:Ω→RY:\Omega\to\mathbb{R} is F/B(R)\mathcal{F}/\mathcal{B}(\mathbb{R})-measurable, it lies in L1(Ω,G,P∣G)\mathcal{L}^{1}(\Omega,\mathcal{G},P|_{\mathcal{G}}) if and only if it lies in L1(P)\mathcal{L}^{1}(P), and then

∫GY d(P∣G)=∫GY dP(G∈G)\int_{G}Y\,d(P|_{\mathcal{G}})=\int_{G}Y\,dP\qquad(G\in\mathcal{G})

(Integrals with Respect to the Restriction of a Measure to a Sub-σ-Algebra (ii), Integrals with Respect to the Restriction of a Measure to a Sub-σ-Algebra (iv), with Integrals over Measurable Subsets (vi) for integrability on GG).

Existence. Let X∈L1(P)X\in\mathcal{L}^{1}(P). The function ν\nu on G\mathcal{G},

ν(G)=∫GX dP(G∈G),\nu(G)=\int_{G}X\,dP\qquad(G\in\mathcal{G}),

is a finite signed measure on (Ω,G)(\Omega,\mathcal{G}) that is absolutely continuous with respect to P∣GP|_{\mathcal{G}} (Finite Signed Measures from Finite Measures and from Integrals (iv)). Under the axiom of dependent choice, the Radon–Nikodym theorem for finite signed measures, applied in (Ω,G,P∣G)(\Omega,\mathcal{G},P|_{\mathcal{G}}) (The Radon–Nikodym Theorem for a σ-Finite Measure, and Uniqueness of Densities (iv)), gives Y∈L1(Ω,G,P∣G)Y\in\mathcal{L}^{1}(\Omega,\mathcal{G},P|_{\mathcal{G}}) with ν(G)=∫GY d(P∣G)\nu(G)=\int_{G}Y\,d(P|_{\mathcal{G}}) for every G∈GG\in\mathcal{G}. As an element of L1(Ω,G,P∣G)\mathcal{L}^{1}(\Omega,\mathcal{G},P|_{\mathcal{G}}), YY is G\mathcal{G}-measurable (Integrable Functions and Their Lebesgue Integral (ii)), so by the transfer above Y∈L1(P)Y\in\mathcal{L}^{1}(P) and

∫GY dP=∫GY d(P∣G)=ν(G)=∫GX dP(G∈G).\int_{G}Y\,dP=\int_{G}Y\,d(P|_{\mathcal{G}})=\nu(G)=\int_{G}X\,dP\qquad(G\in\mathcal{G}).

This proves (i).

Uniqueness. Let YY and Y′Y' be as in (ii). By the transfer, both lie in L1(Ω,G,P∣G)\mathcal{L}^{1}(\Omega,\mathcal{G},P|_{\mathcal{G}}) and

∫GY d(P∣G)=∫GX dP=∫GY′ d(P∣G)(G∈G).\int_{G}Y\,d(P|_{\mathcal{G}})=\int_{G}X\,dP=\int_{G}Y'\,d(P|_{\mathcal{G}})\qquad(G\in\mathcal{G}).

The uniqueness of densities in (Ω,G,P∣G)(\Omega,\mathcal{G},P|_{\mathcal{G}}) (The Radon–Nikodym Theorem for a σ-Finite Measure, and Uniqueness of Densities (i)), which uses no choice, shows that {Y≠Y′}\{Y\neq Y'\} belongs to G\mathcal{G} and has P∣GP|_{\mathcal{G}}-measure 00, that is, P(Y≠Y′)=0P(Y\neq Y')=0.

The vector case. Let X∈L1(P;Rn)X\in\mathcal{L}^{1}(P;\mathbb{R}^{n}); its components XkX_{k} lie in L1(P)\mathcal{L}^{1}(P) (Integrable Vector- and Matrix-Valued Functions and Their Integrals (i)). A function Y:Ω→RnY:\Omega\to\mathbb{R}^{n} is G\mathcal{G}-measurable, respectively F/B(Rn)\mathcal{F}/\mathcal{B}(\mathbb{R}^{n})-measurable, if and only if all its components are G\mathcal{G}-measurable, respectively F/B(R)\mathcal{F}/\mathcal{B}(\mathbb{R})-measurable (Vector- and Matrix-Valued Measurable Maps: Components, Entries and Continuous Images (i), applied on (Ω,G)(\Omega,\mathcal{G}) and on (Ω,F)(\Omega,\mathcal{F})).

For uniqueness, let YY and Y′Y' be as in (iii). For each k∈[n]k\in[n], (ii) applied to XkX_{k}, YkY_{k} and Yk′Y'_{k} shows that Nk={Yk≠Yk′}N_{k}=\{Y_{k}\neq Y'_{k}\} lies in G\mathcal{G} with P(Nk)=0P(N_{k})=0. Since {Y≠Y′}=⋃k∈[n]Nk\{Y\neq Y'\}=\bigcup_{k\in[n]}N_{k}, by induction on nn this set lies in G\mathcal{G} and P(Y≠Y′)≤∑k=1nP(Nk)=0P(Y\neq Y')\le\sum_{k=1}^{n}P(N_{k})=0 (Closure Properties of σ-Algebras, Intersections and Traces of σ-Algebras, and the Generated σ-Algebra (vii), Basic Properties of a Measure (vii)). This proves (iii); no choice is used.

For existence, assume the axiom of dependent choice. For k∈[n]k\in[n] let Vk\mathcal{V}_{k} be the set of G\mathcal{G}-measurable W∈L1(P)W\in\mathcal{L}^{1}(P) with ∫GW dP=∫GXk dP\int_{G}W\,dP=\int_{G}X_{k}\,dP for every G∈GG\in\mathcal{G}; it is nonempty by (i). Since [n][n] is finite (Finite Sets: the Pigeonhole Principle, Uniqueness of the Length, Subsets, Unions, Products, Images, Bounded Sets of Natural Numbers, Extreme Elements, Sets of Maps, Finite Unions and Finite Choice (vii)), finite choice (Finite Sets: the Pigeonhole Principle, Uniqueness of the Length, Subsets, Unions, Products, Images, Bounded Sets of Natural Numbers, Extreme Elements, Sets of Maps, Finite Unions and Finite Choice (xi)), applied to the family (Vk)k∈[n](\mathcal{V}_{k})_{k\in[n]} of nonempty sets, gives a family (Wk)k∈[n](W_{k})_{k\in[n]} with Wk∈VkW_{k}\in\mathcal{V}_{k} for every k∈[n]k\in[n]. Let Y:Ω→RnY:\Omega\to\mathbb{R}^{n} be the function with components Yk=WkY_{k}=W_{k} for k∈[n]k\in[n] (Component Maps of a Map into Rq\mathbb{R}^{q}, Entry Maps of a Map into Matrices, and Maps Assembled from Them (iii)). Its components are G\mathcal{G}-measurable and lie in L1(P)\mathcal{L}^{1}(P), so YY is G\mathcal{G}-measurable, F/B(Rn)\mathcal{F}/\mathcal{B}(\mathbb{R}^{n})-measurable, and Y∈L1(P;Rn)Y\in\mathcal{L}^{1}(P;\mathbb{R}^{n}), with ∫GYk dP=∫GXk dP\int_{G}Y_{k}\,dP=\int_{G}X_{k}\,dP for every G∈GG\in\mathcal{G} and k∈[n]k\in[n]. This proves (iv), using no choice beyond (i).

Uses of dependent choice. The existence statements use the axiom of dependent choice only through The Radon–Nikodym Theorem for a σ-Finite Measure, and Uniqueness of Densities (iv); the uniqueness statements use no choice.

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