TheoremBase

Push pi forward under z -> (q(z), z) to a measure on Y x Z with first marginal nu; conditional kernels of pi given q are exactly the kernels of this measure, so existence and uniqueness come from the product theorem. The graph of q has full measure, which puts almost every conditional measure on its fibre, and the integral formulas follow from the kernel lemma and change of variables.

Proof

Each result cited is universally quantified over the data in its own statement.

Throughout, B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z) is the product σ\sigma-algebra on Y×ZY\times Z, generated by the rectangles A×BA\times B with A∈B(Y)A\in\mathcal{B}(Y) and B∈B(Z)B\in\mathcal{B}(Z), and (Y,B(Y))(Y,\mathcal{B}(Y)) is a measurable space by Borel Sigma-Algebra of a Metric Space and claim 2 of Intersections of Sigma-Algebras and Minimality of the Generated Sigma-Algebra.

Step 1 (the graph measure). Define T:Z→Y×ZT:Z\to Y\times Z by T(z)=(q(z),z)T(z)=(q(z),z). Let S\mathcal{S} be the family of the sets E⊆Y×ZE\subseteq Y\times Z with T−1(E)∈B(Z)T^{-1}(E)\in\mathcal{B}(Z). Since T−1(Y×Z)=ZT^{-1}(Y\times Z)=Z, T−1((Y×Z)∖E)=Z∖T−1(E)T^{-1}\bigl((Y\times Z)\setminus E\bigr)=Z\setminus T^{-1}(E) and T−1(⋃mEm)=⋃mT−1(Em)T^{-1}\bigl(\bigcup_{m}E_{m}\bigr)=\bigcup_{m}T^{-1}(E_{m}), and B(Z)\mathcal{B}(Z) is a σ\sigma-algebra, S\mathcal{S} is a σ\sigma-algebra on Y×ZY\times Z (Sigma-Algebra and Measurable Space). For A∈B(Y)A\in\mathcal{B}(Y) and B∈B(Z)B\in\mathcal{B}(Z) we have T−1(A×B)=B∩q−1(A)∈B(Z)T^{-1}(A\times B)=B\cap q^{-1}(A)\in\mathcal{B}(Z), by the measurability of qq. So S\mathcal{S} contains every rectangle, and by claim 2 of Intersections of Sigma-Algebras and Minimality of the Generated Sigma-Algebra it contains B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z); that is, TT is measurable with respect to B(Z)\mathcal{B}(Z) and B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z). By claim 1 of Image Measures, Measures with Densities, and Change of Variables, π^(E)=π(T−1(E))\hat{\pi}(E)=\pi(T^{-1}(E)) defines a probability measure π^\hat{\pi} on (Y×Z,B(Y)⊗B(Z))(Y\times Z,\mathcal{B}(Y)\otimes\mathcal{B}(Z)), and

π^(A×B)=π(B∩q−1(A))(A∈B(Y), B∈B(Z)).(1)\hat{\pi}(A\times B)=\pi\bigl(B\cap q^{-1}(A)\bigr)\qquad(A\in\mathcal{B}(Y),\ B\in\mathcal{B}(Z)).\tag{1}

In particular π^(Y×Z)=1\hat{\pi}(Y\times Z)=1, and the first marginal of π^\hat{\pi} is A↦π^(A×Z)=π(q−1(A))=ν(A)A\mapsto\hat{\pi}(A\times Z)=\pi(q^{-1}(A))=\nu(A). Hence Disintegration of a Probability Measure on a Product with a Polish Factor: Existence and Almost-Everywhere Uniqueness of the Conditional Kernel applies to the measurable space (Y,B(Y))(Y,\mathcal{B}(Y)), the complete separable metric space (Z,d)(Z,d) and the measure π^\hat{\pi}, and the first marginal called μ\mu there is ν\nu.

Step 2 (conditional kernels given qq are the kernels of π^\hat{\pi}). Let κ\kappa be a probability kernel from (Y,B(Y))(Y,\mathcal{B}(Y)) to (Z,B(Z))(Z,\mathcal{B}(Z)). We claim that κ\kappa is a conditional kernel of π\pi given qq in the sense of The Conditional Kernel of a Probability Measure Given a Measurable Map §conditional-kernel if and only if π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa. If κ\kappa is a conditional kernel of π\pi given qq, then by (1)

π^(A×B)=∫Y1A(y) κ(y,B) ν(dy)(A∈B(Y), B∈B(Z)),\hat{\pi}(A\times B)=\int_{Y}\mathbf{1}_{A}(y)\,\kappa(y,B)\,\nu(dy)\qquad(A\in\mathcal{B}(Y),\ B\in\mathcal{B}(Z)),

so π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa by Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §rectangles, applied to the probability measure ν\nu on (Y,B(Y))(Y,\mathcal{B}(Y)). Conversely, if π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa, then by (1) and Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §composite, π(B∩q−1(A))=π^(A×B)=(ν⊗κ)(A×B)=∫Y1A(y) κ(y,B) ν(dy)\pi\bigl(B\cap q^{-1}(A)\bigr)=\hat{\pi}(A\times B)=(\nu\otimes\kappa)(A\times B)=\int_{Y}\mathbf{1}_{A}(y)\,\kappa(y,B)\,\nu(dy) for all A∈B(Y)A\in\mathcal{B}(Y) and B∈B(Z)B\in\mathcal{B}(Z), which is the defining identity of a conditional kernel of π\pi given qq.

Claim 1. By Disintegration of a Probability Measure on a Product with a Polish Factor: Existence and Almost-Everywhere Uniqueness of the Conditional Kernel §existence there is a probability kernel κ\kappa from (Y,B(Y))(Y,\mathcal{B}(Y)) to (Z,B(Z))(Z,\mathcal{B}(Z)) with π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa; by Step 2 it is a conditional kernel of π\pi given qq.

Claim 2. If κ\kappa and κ′\kappa' are conditional kernels of π\pi given qq, then π^=ν⊗κ=ν⊗κ′\hat{\pi}=\nu\otimes\kappa=\nu\otimes\kappa' by Step 2, and Disintegration of a Probability Measure on a Product with a Polish Factor: Existence and Almost-Everywhere Uniqueness of the Conditional Kernel §uniqueness shows that the set of the y∈Yy\in Y with κy≠κy′\kappa_{y}\ne\kappa'_{y} belongs to B(Y)\mathcal{B}(Y) and has ν\nu-measure 00.

Claim 3. Let κ\kappa be a conditional kernel of π\pi given qq, so that π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa by Step 2. Let Y×YY\times Y carry the product metric dY×Yd_{Y\times Y}, a metric by claim 1 of The Product Metric is a Metric, and let Δ={(y,y):y∈Y}\Delta=\{(y,y):y\in Y\}. The set Δ\Delta is closed in Y×YY\times Y for the topology of the subsets that are open in (Y×Y,dY×Y)(Y\times Y,d_{Y\times Y}): given (y,y′)∉Δ(y,y')\notin\Delta, put r=dY(y,y′)/2>0r=d_{Y}(y,y')/2>0; if dY×Y((y,y′),(w,w′))<rd_{Y\times Y}\bigl((y,y'),(w,w')\bigr)<r, then dY(y,w)<rd_{Y}(y,w)<r and dY(y′,w′)<rd_{Y}(y',w')<r by claim 3 of The Product Metric is a Metric, so by the triangle inequality dY(w,w′)≥dY(y,y′)−dY(y,w)−dY(y′,w′)>0d_{Y}(w,w')\ge d_{Y}(y,y')-d_{Y}(y,w)-d_{Y}(y',w')>0 and (w,w′)∉Δ(w,w')\notin\Delta. Thus (Y×Y)∖Δ(Y\times Y)\setminus\Delta is open in (Y×Y,dY×Y)(Y\times Y,d_{Y\times Y}) by Open Subset of a Metric Space, so Δ\Delta is closed (Closed Subset of a Topological Space) and belongs to the Borel σ\sigma-algebra B(Y×Y)\mathcal{B}(Y\times Y) of (Y×Y,dY×Y)(Y\times Y,d_{Y\times Y}) by claim 1 of Borel Measurability and Bounded Integration on a Metric Space. As (Y,dY)(Y,d_{Y}) is separable, The Borel Sigma-Algebra of a Product of Two Separable Metric Spaces is the Product Sigma-Algebra §product, applied with both factors equal to (Y,dY)(Y,d_{Y}), gives B(Y×Y)=B(Y)⊗B(Y)\mathcal{B}(Y\times Y)=\mathcal{B}(Y)\otimes\mathcal{B}(Y), so Δ∈B(Y)⊗B(Y)\Delta\in\mathcal{B}(Y)\otimes\mathcal{B}(Y).

Define Φ:Y×Z→Y×Y\Phi:Y\times Z\to Y\times Y by Φ(y,z)=(y,q(z))\Phi(y,z)=(y,q(z)). Exactly as for TT in Step 1, the family of the sets E⊆Y×YE\subseteq Y\times Y with Φ−1(E)∈B(Y)⊗B(Z)\Phi^{-1}(E)\in\mathcal{B}(Y)\otimes\mathcal{B}(Z) is a σ\sigma-algebra containing every rectangle A×A′A\times A' with A,A′∈B(Y)A,A'\in\mathcal{B}(Y), because Φ−1(A×A′)=A×q−1(A′)\Phi^{-1}(A\times A')=A\times q^{-1}(A') is a rectangle of B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z); so by claim 2 of Intersections of Sigma-Algebras and Minimality of the Generated Sigma-Algebra that family contains B(Y)⊗B(Y)\mathcal{B}(Y)\otimes\mathcal{B}(Y). Hence

G=Φ−1(Δ)={(y,z)∈Y×Z:q(z)=y}∈B(Y)⊗B(Z).G=\Phi^{-1}(\Delta)=\{(y,z)\in Y\times Z:q(z)=y\}\in\mathcal{B}(Y)\otimes\mathcal{B}(Z).

For every z∈Zz\in Z we have T(z)=(q(z),z)∈GT(z)=(q(z),z)\in G, so T−1(G)=ZT^{-1}(G)=Z and π^(G)=π(Z)=1\hat{\pi}(G)=\pi(Z)=1. The section of GG at y∈Yy\in Y is Gy={z:q(z)=y}=q−1({y})G_{y}=\{z:q(z)=y\}=q^{-1}(\{y\}). Let φ(y)=κ(y,Gy)=κy(q−1({y}))\varphi(y)=\kappa(y,G_{y})=\kappa_{y}\bigl(q^{-1}(\{y\})\bigr). By Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §sections, φ\varphi takes values in [0,1][0,1], is measurable with respect to B(Y)\mathcal{B}(Y) and is integrable with respect to ν\nu, and by Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §composite

∫Yφ(y) ν(dy)=(ν⊗κ)(G)=π^(G)=1.\int_{Y}\varphi(y)\,\nu(dy)=(\nu\otimes\kappa)(G)=\hat{\pi}(G)=1 .

The constant function 11 is integrable with respect to the Borel measure ν\nu on (Y,dY)(Y,d_{Y}), with ∫Y1 ν(dy)=ν(Y)=1\int_{Y}1\,\nu(dy)=\nu(Y)=1, by claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space. By Linearity and Monotonicity of the Lebesgue Integral §integrable, 1−φ1-\varphi is integrable with ∫Y(1−φ(y)) ν(dy)=0\int_{Y}\bigl(1-\varphi(y)\bigr)\,\nu(dy)=0. The function 1−φ1-\varphi is measurable and takes values in [0,1][0,1], so by claim 6(c) of Borel Measurability and Bounded Integration on a Metric Space its integral as a nonnegative function is also 00, and by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §vanishing the set E={y∈Y:φ(y)≠1}E=\{y\in Y:\varphi(y)\ne1\} is ν\nu-null. The set R∖{1}\mathbb{R}\setminus\{1\} is open in the real line with the absolute-value metric by Open Subset of a Metric Space, since for t≠1t\ne1 the open ball about tt of radius ∣t−1∣>0|t-1|>0 does not contain 11; so it belongs to B(R)\mathcal{B}(\mathbb{R}) by claims 1 and 2 of Borel Measurability and Bounded Integration on a Metric Space; hence E=φ−1(R∖{1})∈B(Y)E=\varphi^{-1}(\mathbb{R}\setminus\{1\})\in\mathcal{B}(Y), and being null it has ν(E)=0\nu(E)=0 by Basic Properties of a Measure §monotone. The set of the yy with κy(q−1({y}))=1\kappa_{y}(q^{-1}(\{y\}))=1 is Y∖E∈B(Y)Y\setminus E\in\mathcal{B}(Y), and ν(Y∖E)=ν(Y)−ν(E)=1\nu(Y\setminus E)=\nu(Y)-\nu(E)=1 by Basic Properties of a Measure §differences.

Claims 4 and 5. Let κ\kappa be a conditional kernel of π\pi given qq, so that π^=ν⊗κ\hat{\pi}=\nu\otimes\kappa by Step 2, and let f:Z→Rf:Z\to\mathbb{R} be measurable with respect to B(Z)\mathcal{B}(Z). Define F:Y×Z→RF:Y\times Z\to\mathbb{R} by F(y,z)=f(z)F(y,z)=f(z). The projection (y,z)↦z(y,z)\mapsto z is measurable with respect to B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z) and B(Z)\mathcal{B}(Z) by claim 5 of Sections of Product-Measurable Sets and Maps Are Measurable, and Insertion Maps into Products Are Measurable, so FF, its composite with ff, is measurable with respect to B(Y)⊗B(Z)\mathcal{B}(Y)\otimes\mathcal{B}(Z) and B(R)\mathcal{B}(\mathbb{R}) by claim 4 of Borel Measurability and Bounded Integration on a Metric Space. For every y∈Yy\in Y the function F(y,⋅)F(y,\cdot) is ff, and F∘T=fF\circ T=f. By claim 2 of Image Measures, Measures with Densities, and Change of Variables, applied to π^\hat{\pi}, the image measure of π\pi under TT, FF is integrable with respect to π^\hat{\pi} if and only if ff is integrable with respect to π\pi, and then

∫Y×ZF dπ^=∫Zf dπ.(2)\int_{Y\times Z}F\,d\hat{\pi}=\int_{Z}f\,d\pi .\tag{2}

For claim 4, let ff be bounded; then FF is bounded. By Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §bounded, applied to ν\nu, κ\kappa and FF: for every yy the function ff is integrable with respect to κy\kappa_{y}; the function y↦∫Zf dκyy\mapsto\int_{Z}f\,d\kappa_{y} is measurable with respect to B(Y)\mathcal{B}(Y) and bounded; FF is integrable with respect to ν⊗κ=π^\nu\otimes\kappa=\hat{\pi}; that function is integrable with respect to ν\nu; and ∫Y×ZF dπ^=∫Y(∫Zf dκy)ν(dy)\int_{Y\times Z}F\,d\hat{\pi}=\int_{Y}\bigl(\int_{Z}f\,d\kappa_{y}\bigr)\nu(dy). Since FF is integrable with respect to π^\hat{\pi}, ff is integrable with respect to π\pi, and (2) gives the displayed identity of claim 4.

For claim 5, let f≥0f\ge0; then F≥0F\ge0, and since F(y,⋅)=fF(y,\cdot)=f, the set NN and the function gg of claim 5 are exactly the set and the function that Integration Against a Probability Kernel: Measurable Sections, the Composite Measure on the Product and the Iterated Integral §nonnegative attaches to FF, ν\nu and κ\kappa. By that clause, N∈B(Y)N\in\mathcal{B}(Y), gg is measurable with respect to B(Y)\mathcal{B}(Y), and FF is integrable with respect to ν⊗κ=π^\nu\otimes\kappa=\hat{\pi} if and only if ν(N)=0\nu(N)=0 and gg is integrable with respect to ν\nu, in which case ∫Y×ZF dπ^=∫Yg(y) ν(dy)\int_{Y\times Z}F\,d\hat{\pi}=\int_{Y}g(y)\,\nu(dy). Combining this with the equivalence and the identity (2) above, ff is integrable with respect to π\pi if and only if ν(N)=0\nu(N)=0 and gg is integrable with respect to ν\nu, and in that case ∫Zf dπ=∫Yg(y) ν(dy)\int_{Z}f\,d\pi=\int_{Y}g(y)\,\nu(dy). ■\blacksquare

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