TheoremBase

For a bounded continuous test function g on Z, the composite g o T is bounded and continuous on Y; the change of variables formula for image measures turns the integrals of g against the image measures into integrals of g o T against the original measures, which converge by hypothesis.

Proof

Each result cited below is universally quantified over the data in its own statement and is applied with the data named at the point of citation.

Write dR(s,t)=∣s−t∣d_{\mathbb{R}}(s,t)=|s-t| for the absolute-value metric on R\mathbb{R}; by claim 2 of Borel Measurability and Bounded Integration on a Metric Space the Borel σ\sigma-algebra of (R,dR)(\mathbb{R},d_{\mathbb{R}}) is the Borel σ\sigma-algebra B(R)\mathcal{B}(\mathbb{R}) of the real line. Let g:Z→Rg:Z\to\mathbb{R} be bounded, with a bound MM, and continuous on ZZ. By Weak Convergence of Finite Borel Measures on a Metric Space it suffices to show that (∫Zg d(T#μj))j∈N\bigl(\int_{Z}g\,d(T_{\#}\mu_{j})\bigr)_{j\in\mathbb{N}} converges to ∫Zg d(T#μ)\int_{Z}g\,d(T_{\#}\mu); note that T#μj(Z)=μj(Y)<∞T_{\#}\mu_{j}(Z)=\mu_{j}(Y)<\infty and T#μ(Z)=μ(Y)<∞T_{\#}\mu(Z)=\mu(Y)<\infty, as recalled in the statement from claim 1 of Image Measures, Measures with Densities, and Change of Variables, so all these measures are finite Borel measures on (Z,dZ)(Z,d_{Z}).

Step 1 (the composite is a bounded continuous function). Let u=g∘T:Y→Ru=g\circ T:Y\to\mathbb{R}. Then ∣u(y)∣=∣g(T(y))∣≤M|u(y)|=|g(T(y))|\le M for every y∈Yy\in Y, so uu is bounded. Let y∈Yy\in Y and let ε\varepsilon be a positive real number. Since gg is continuous at T(y)T(y), Continuous Map Between Metric Spaces gives a positive real δ1\delta_{1} such that every z∈Zz\in Z with dZ(T(y),z)<δ1d_{Z}(T(y),z)<\delta_{1} satisfies dR(g(z),g(T(y)))<εd_{\mathbb{R}}(g(z),g(T(y)))<\varepsilon. Since TT is continuous at yy, the same definition, applied with the positive number δ1\delta_{1}, gives a positive real δ\delta such that every y′∈Yy'\in Y with dY(y,y′)<δd_{Y}(y,y')<\delta satisfies dZ(T(y′),T(y))<δ1d_{Z}(T(y'),T(y))<\delta_{1}, hence dZ(T(y),T(y′))<δ1d_{Z}(T(y),T(y'))<\delta_{1} by the symmetry condition 3 of Metric Space, hence dR(u(y′),u(y))<εd_{\mathbb{R}}(u(y'),u(y))<\varepsilon. These choices are made in the order ε\varepsilon, δ1\delta_{1}, δ\delta. Thus uu is continuous at every point of YY, that is, continuous on YY.

Step 2 (measurability and integrability). By claim 3 of Borel Measurability and Bounded Integration on a Metric Space, applied to the continuous maps g:Z→Rg:Z\to\mathbb{R} and u:Y→Ru:Y\to\mathbb{R} with values in (R,dR)(\mathbb{R},d_{\mathbb{R}}), the function gg is measurable with respect to B(Z)\mathcal{B}(Z) and B(R)\mathcal{B}(\mathbb{R}), and uu is measurable with respect to B(Y)\mathcal{B}(Y) and B(R)\mathcal{B}(\mathbb{R}). Since ∣g∣≤M|g|\le M, claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space shows that gg is integrable with respect to every finite Borel measure on (Z,dZ)(Z,d_{Z}), in particular with respect to T#μjT_{\#}\mu_{j} for every jj and with respect to T#μT_{\#}\mu.

Step 3 (change of variables). Let ν\nu be one of the measures μj\mu_{j}, j∈Nj\in\mathbb{N}, or μ\mu. By claim 2 of Image Measures, Measures with Densities, and Change of Variables, applied to the measure space (Y,B(Y),ν)(Y,\mathcal{B}(Y),\nu), the measurable space (Z,B(Z))(Z,\mathcal{B}(Z)), the measurable map TT and the measurable function gg, which is integrable with respect to T#νT_{\#}\nu by Step 2, the function u=g∘Tu=g\circ T is integrable with respect to ν\nu and

∫Zg d(T#ν)=∫Yg∘T dν.\int_{Z}g\,d(T_{\#}\nu)=\int_{Y}g\circ T\,d\nu .

Step 4 (conclusion). By Step 1, uu is a bounded function on YY that is continuous on YY, so the hypothesis μj⇒μ\mu_{j}\Rightarrow\mu and Weak Convergence of Finite Borel Measures on a Metric Space show that (∫Yu dμj)j∈N\bigl(\int_{Y}u\,d\mu_{j}\bigr)_{j\in\mathbb{N}} converges to ∫Yu dμ\int_{Y}u\,d\mu. By Step 3 these are the numbers ∫Zg d(T#μj)\int_{Z}g\,d(T_{\#}\mu_{j}) and ∫Zg d(T#μ)\int_{Z}g\,d(T_{\#}\mu). As gg was an arbitrary bounded function continuous on ZZ, Weak Convergence of Finite Borel Measures on a Metric Space gives T#μj⇒T#μT_{\#}\mu_{j}\Rightarrow T_{\#}\mu.

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