TheoremBase

Joint Distribution, Expectations, and Block Independence for Independent Random Variables

Statement

Throughout, rr is a natural number with r≥1r\ge 1, Rr\mathbb{R}^r is Euclidean space, R\mathbb{R} denotes the real numbers, and B(R)\mathcal{B}(\mathbb{R}) the Borel σ\sigma-algebra.

Define the rr-fold product Borel σ\sigma-algebra Br\mathcal{B}_r on Rr\mathbb{R}^r iteratively: B1=B(R)\mathcal{B}_1=\mathcal{B}(\mathbb{R}) and, for 2≤k≤r2\le k\le r, Bk=Bk−1⊗B(R)\mathcal{B}_k=\mathcal{B}_{k-1}\otimes\mathcal{B}(\mathbb{R}), the product σ\sigma-algebra on Rk\mathbb{R}^{k}, identifying the Cartesian product Rk−1×R\mathbb{R}^{k-1}\times\mathbb{R} with Rk\mathbb{R}^{k} via ((x1,…,xk−1),xk)↦(x1,…,xk)((x_1,\dots,x_{k-1}),x_k)\mapsto(x_1,\dots,x_k). Given probability measures ν1,…,νr\nu_1,\dots,\nu_r on (R,B(R))(\mathbb{R},\mathcal{B}(\mathbb{R})), define the probability measure ν1⊗⋯⊗νr\nu_1\otimes\cdots\otimes\nu_r on (Rr,Br)(\mathbb{R}^r,\mathcal{B}_r) iteratively by Existence and Uniqueness of the Product Measure (probability measures are σ\sigma-finite). Call a function φ:Rr→R\varphi:\mathbb{R}^r\to\mathbb{R} jointly Borel if it is measurable from (Rr,Br)(\mathbb{R}^r,\mathcal{B}_r) to (R,B(R))(\mathbb{R},\mathcal{B}(\mathbb{R})).

Let (Ω,F,P)(\Omega,\mathcal{F},P) be a probability space and let V1,…,VrV_1,\dots,V_r be independent random variables on it with distributions ν1,…,νr\nu_1,\dots,\nu_r. Then the following hold.

Claim 1. The map V:Ω→RrV:\Omega\to\mathbb{R}^r given by V(ω)=(V1(ω),…,Vr(ω))V(\omega)=(V_1(\omega),\dots,V_r(\omega)) is measurable from (Ω,F)(\Omega,\mathcal{F}) to (Rr,Br)(\mathbb{R}^r,\mathcal{B}_r), and its distribution PV:Br→[0,1]P_V:\mathcal{B}_r\to[0,1], PV(C)=P(V∈C)P_V(C)=P(V\in C), is a probability measure equal to ν1⊗⋯⊗νr\nu_1\otimes\cdots\otimes\nu_r.

Claim 2. If φ:Rr→R\varphi:\mathbb{R}^r\to\mathbb{R} is jointly Borel and either nonnegative or bounded, then φ(V1,…,Vr)=φ∘V\varphi(V_1,\dots,V_r)=\varphi\circ V is a random variable and its expectation is defined (as an element of [0,∞][0,\infty] in the nonnegative case, and as a real number in the bounded case, where φ∘V\varphi\circ V is integrable), with

E[φ(V1,…,Vr)]=∫Rrφ d(ν1⊗⋯⊗νr).\mathbb{E}[\varphi(V_1,\dots,V_r)]=\int_{\mathbb{R}^r}\varphi\,d(\nu_1\otimes\cdots\otimes\nu_r).

In particular this expectation depends only on φ\varphi and the distributions ν1,…,νr\nu_1,\dots,\nu_r.

Claim 3 (block independence). Let I={i1<⋯<ip}I=\{i_1<\dots<i_p\} and J={j1<⋯<jq}J=\{j_1<\dots<j_q\} be disjoint nonempty subsets of {1,…,r}\{1,\dots,r\}, and let φ:Rp→R\varphi:\mathbb{R}^p\to\mathbb{R} and ψ:Rq→R\psi:\mathbb{R}^q\to\mathbb{R} be jointly Borel. Then φ(Vi1,…,Vip)\varphi(V_{i_1},\dots,V_{i_p}) and ψ(Vj1,…,Vjq)\psi(V_{j_1},\dots,V_{j_q}) are independent random variables.

Claim 4. Each coordinate projection (x1,…,xr)↦xi(x_1,\dots,x_r)\mapsto x_i and the addition map (x1,…,xr)↦x1+⋯+xr(x_1,\dots,x_r)\mapsto x_1+\cdots+x_r are jointly Borel; moreover, if φ:Rr→R\varphi:\mathbb{R}^r\to\mathbb{R} is jointly Borel and t:R→Rt:\mathbb{R}\to\mathbb{R} is Borel measurable, then t∘φt\circ\varphi is jointly Borel.

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