TheoremBase

The radial map transports the sequence to the compact closed unit ball, where weak sequential compactness gives a limit; tightness puts all of its mass in the open ball, and pushing forward by the inverse map produces the limit measure, cutoffs controlling the error on both sides.

Proof

Each result cited below is universally quantified over the data in its own statement, and is applied to the data named where it is used. Throughout, Bˉ\bar{B}, UU, dBˉd_{\bar{B}}, dUd_{U}, hh and gg are as in The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions, read at the dimension mm, and T\mathcal{T} is the collection of subsets of Rm\mathbb{R}^{m} open in (Rm,dE)(\mathbb{R}^{m},d_{E}). Write B(Bˉ)\mathcal{B}(\bar{B}) and B(U)\mathcal{B}(U) for the Borel σ\sigma-algebras of the metric spaces (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) and (U,dU)(U,d_{U}).

Step 0 (a bound used three times). Let (Z,dZ)(Z,d_{Z}) be a metric space, let ν\nu be a Borel measure on (Z,dZ)(Z,d_{Z}) with ν(Z)<∞\nu(Z)<\infty, let AA belong to the Borel σ\sigma-algebra B(Z)\mathcal{B}(Z) of (Z,dZ)(Z,d_{Z}), let MM be a nonnegative real number, and let u:Z→Ru:Z\to\mathbb{R} be measurable with respect to B(Z)\mathcal{B}(Z) and the Borel σ\sigma-algebra of the real line, with ∣u(z)∣≤M|u(z)|\le M for every z∈Zz\in Z and u(z)=0u(z)=0 for every z∈Z∖Az\in Z\setminus A. Then uu is integrable with respect to ν\nu and

∣∫Zu dν∣≤M ν(A).\Bigl|\int_{Z}u\,d\nu\Bigr|\le M\,\nu(A).

Indeed, uu is integrable with respect to ν\nu by claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space. By The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (vi), applied to (Z,dZ)(Z,d_{Z}), the set AA, the measure ν\nu and the function uu, the restriction u∣Au|_{A} is measurable with respect to B(A)\mathcal{B}(A), is integrable with respect to ν∣A\nu|_{A}, and ∫Zu dν=∫Au∣A d(ν∣A)\int_{Z}u\,d\nu=\int_{A}u|_{A}\,d(\nu|_{A}). By The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (v), ν∣A\nu|_{A} is a Borel measure on (A,dA)(A,d_{A}) with ν∣A(A)=ν(A)\nu|_{A}(A)=\nu(A), which is finite because ν(A)≤ν(Z)<∞\nu(A)\le\nu(Z)<\infty by claim 2 of Basic Properties of a Measure. Since ∣u∣A(z)∣≤M|u|_{A}(z)|\le M for every z∈Az\in A, claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space, applied on (A,dA)(A,d_{A}), gives ∣∫Au∣A d(ν∣A)∣≤M ν∣A(A)=M ν(A)\bigl|\int_{A}u|_{A}\,d(\nu|_{A})\bigr|\le M\,\nu|_{A}(A)=M\,\nu(A).

Step 1 (transport to the closed unit ball). By claims 2 and 3 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions, h(x)∈U⊆Bˉh(x)\in U\subseteq\bar{B} for every x∈Rmx\in\mathbb{R}^{m}, so the map hBˉ:Rm→Bˉh_{\bar{B}}:\mathbb{R}^{m}\to\bar{B} with hBˉ(x)=h(x)h_{\bar{B}}(x)=h(x) is well defined. By claim 3 of that lemma hh is continuous on Rm\mathbb{R}^{m} as a map into (Rm,dE)(\mathbb{R}^{m},d_{E}), so hBˉh_{\bar{B}} is continuous on Rm\mathbb{R}^{m} as a map into (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) by The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (iii). By claim 3 of Borel Measurability and Bounded Integration on a Metric Space, hBˉh_{\bar{B}} is measurable with respect to B(Rm)\mathcal{B}(\mathbb{R}^{m}) and B(Bˉ)\mathcal{B}(\bar{B}).

For each n∈Nn\in\mathbb{N} let μ~n\tilde{\mu}_{n} be the image measure of μn\mu_{n} under hBˉh_{\bar{B}}, formed by claim 1 of that lemma for the measure space (Rm,B(Rm),μn)(\mathbb{R}^{m},\mathcal{B}(\mathbb{R}^{m}),\mu_{n}) and the measurable space (Bˉ,B(Bˉ))(\bar{B},\mathcal{B}(\bar{B})). By that claim μ~n\tilde{\mu}_{n} is a measure on (Bˉ,B(Bˉ))(\bar{B},\mathcal{B}(\bar{B})), that is, a Borel measure on (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) by Borel Measure on a Metric Space, and μ~n(Bˉ)=μn(Rm)=1\tilde{\mu}_{n}(\bar{B})=\mu_{n}(\mathbb{R}^{m})=1.

Step 2 (extraction). The metric space (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) is compact by claim 2 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions. By Weak Sequential Compactness of Borel Measures of Total Mass One on a Compact Metric Space, applied to it and to the sequence (μ~n)n∈N(\tilde{\mu}_{n})_{n\in\mathbb{N}}, there are a strictly increasing sequence (nj)j∈N(n_{j})_{j\in\mathbb{N}} in N\mathbb{N} and a Borel measure μ~\tilde{\mu} on (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) with μ~(Bˉ)=1\tilde{\mu}(\bar{B})=1 such that (μ~nj)j∈N(\tilde{\mu}_{n_{j}})_{j\in\mathbb{N}} converges weakly to μ~\tilde{\mu}. These (nj)j∈N(n_{j})_{j\in\mathbb{N}} and μ~\tilde{\mu} are fixed for the rest of the proof, before any test function is chosen.

Step 3 (cutoffs adapted to a tolerance). Let ε∈R\varepsilon\in\mathbb{R} satisfy 0<ε0<\varepsilon. Since (μn)n∈N(\mu_{n})_{n\in\mathbb{N}} is tight, Tight Family of Borel Measures on a Metric Space (ii) provides a set K⊆RmK\subseteq\mathbb{R}^{m}, compact in (Rm,T)(\mathbb{R}^{m},\mathcal{T}), with μn(Rm∖K)≤ε\mu_{n}(\mathbb{R}^{m}\setminus K)\le\varepsilon for every n∈Nn\in\mathbb{N}. Distinguish two cases.

Case A: KK is empty. Then Rm∖K=Rm\mathbb{R}^{m}\setminus K=\mathbb{R}^{m}, so 1=μ1(Rm)≤ε1=\mu_{1}(\mathbb{R}^{m})\le\varepsilon.

Case B: KK is nonempty. By claim 4 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions there is a real ρ\rho with 0≤ρ<10\le\rho<1 and ∥h(x)∥≤ρ\lVert h(x)\rVert\le\rho for every x∈Kx\in K. Let σ=2−1(1+ρ)\sigma=2^{-1}(1+\rho) and let χ:Rm→R\chi:\mathbb{R}^{m}\to\mathbb{R} be the map given by claim 5 of that lemma for this ρ\rho, so that ρ<σ<1\rho<\sigma<1, χ\chi is continuous on Rm\mathbb{R}^{m}, 0≤χ≤10\le\chi\le 1, χ(y)=1\chi(y)=1 whenever ∥y∥≤ρ\lVert y\rVert\le\rho, and χ(y)=0\chi(y)=0 whenever σ≤∥y∥\sigma\le\lVert y\rVert. In particular

χ(h(x))=1for every x∈K.(i)\chi(h(x))=1\qquad\text{for every }x\in K. \tag{i}

Let χBˉ\chi_{\bar{B}} be the restriction of χ\chi to Bˉ\bar{B}. It is continuous on Bˉ\bar{B} as a map from (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) to R\mathbb{R}, by claim 4 of Semicontinuity and Continuity Under Composition with a Continuous Map followed by The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (ii), and ∣χBˉ∣≤1|\chi_{\bar{B}}|\le 1; so it is measurable with respect to B(Bˉ)\mathcal{B}(\bar{B}) by claim 3 of Borel Measurability and Bounded Integration on a Metric Space and integrable with respect to each of μ~n\tilde{\mu}_{n} and μ~\tilde{\mu} by claim 6(b) of that lemma. Since h(x)∈Bˉh(x)\in\bar{B} for every xx, the composition χBˉ∘hBˉ\chi_{\bar{B}}\circ h_{\bar{B}} is the map x↦χ(h(x))x\mapsto\chi(h(x)), and claim 2 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables gives, for every nn,

∫Rmχ(h(x)) μn(dx)=∫BˉχBˉ dμ~n.\int_{\mathbb{R}^{m}}\chi(h(x))\,\mu_{n}(dx)=\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}_{n}.

The map x↦1−χ(h(x))x\mapsto 1-\chi(h(x)) is continuous on Rm\mathbb{R}^{m}, hence measurable with respect to B(Rm)\mathcal{B}(\mathbb{R}^{m}) by claim 3 of Borel Measurability and Bounded Integration on a Metric Space, takes values in the interval from 00 to 11, and vanishes on KK by (i). The set Rm∖K\mathbb{R}^{m}\setminus K belongs to B(Rm)\mathcal{B}(\mathbb{R}^{m}) by Compact Subsets of a Metric Space are Closed and Borel (ii), so Step 0, applied with Z=RmZ=\mathbb{R}^{m}, ν=μn\nu=\mu_{n}, A=Rm∖KA=\mathbb{R}^{m}\setminus K and M=1M=1, gives ∫Rm(1−χ(h(x))) μn(dx)≤μn(Rm∖K)≤ε\int_{\mathbb{R}^{m}}(1-\chi(h(x)))\,\mu_{n}(dx)\le\mu_{n}(\mathbb{R}^{m}\setminus K)\le\varepsilon. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion and claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space,

∫Rm(1−χ(h(x))) μn(dx)=1−∫BˉχBˉ dμ~n,\int_{\mathbb{R}^{m}}\bigl(1-\chi(h(x))\bigr)\,\mu_{n}(dx)=1-\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}_{n},

so 1−ε≤∫BˉχBˉ dμ~n1-\varepsilon\le\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}_{n} for every n∈Nn\in\mathbb{N}. By Step 2 the sequence (∫BˉχBˉ dμ~nj)j∈N\bigl(\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}_{n_{j}}\bigr)_{j\in\mathbb{N}} converges to ∫BˉχBˉ dμ~\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}, so comparison with the constant sequence of value 1−ε1-\varepsilon, by claim 1 of Order Properties of Limits of Real Sequences, gives

1−ε≤∫BˉχBˉ dμ~.(ii)1-\varepsilon\le\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}. \tag{ii}

Step 4 (the limit measure). We show that μ~(U)=1\tilde{\mu}(U)=1. By claim 2 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions the set UU is open in (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}), hence U∈B(Bˉ)U\in\mathcal{B}(\bar{B}) by claim 1 of Borel Measurability and Bounded Integration on a Metric Space.

Let ε∈R\varepsilon\in\mathbb{R} satisfy 0<ε0<\varepsilon and run Step 3 with it. In Case A we have 1≤ε1\le\varepsilon, so 1−ε≤0≤μ~(U)1-\varepsilon\le 0\le\tilde{\mu}(U). In Case B, let D={y∈Bˉ:∥y∥<σ}D=\{y\in\bar{B}:\lVert y\rVert<\sigma\}. Then D=Bˉ∩VD=\bar{B}\cap V, where VV is the open ball of (Rm,dE)(\mathbb{R}^{m},d_{E}) with centre 00 and radius σ\sigma, open by Open Ball in a Metric Space is Open; so DD is open in (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) by claim 2 of The Restriction of a Metric to a Subset Induces the Subspace Topology and D∈B(Bˉ)D\in\mathcal{B}(\bar{B}) by claim 1 of Borel Measurability and Bounded Integration on a Metric Space. Since σ<1\sigma<1 we have D⊆UD\subseteq U. The map χBˉ\chi_{\bar{B}} vanishes at every y∈Bˉ∖Dy\in\bar{B}\setminus D, because such a yy satisfies σ≤∥y∥\sigma\le\lVert y\rVert. Step 0, applied with Z=BˉZ=\bar{B}, ν=μ~\nu=\tilde{\mu}, A=DA=D and M=1M=1, therefore gives ∫BˉχBˉ dμ~≤μ~(D)\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}\le\tilde{\mu}(D), and μ~(D)≤μ~(U)\tilde{\mu}(D)\le\tilde{\mu}(U) by claim 2 of Basic Properties of a Measure. With (ii) this gives 1−ε≤μ~(U)1-\varepsilon\le\tilde{\mu}(U) again.

Thus 1−ε≤μ~(U)1-\varepsilon\le\tilde{\mu}(U) for every positive real ε\varepsilon, so 1≤μ~(U)1\le\tilde{\mu}(U) by claim 2 of Comparison of Real Numbers with Arbitrary Positive Slack; and μ~(U)≤μ~(Bˉ)=1\tilde{\mu}(U)\le\tilde{\mu}(\bar{B})=1 by claim 2 of Basic Properties of a Measure. Hence μ~(U)=1\tilde{\mu}(U)=1.

By The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (v), applied to (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}) and the set U∈B(Bˉ)U\in\mathcal{B}(\bar{B}), the restriction μ~∣U\tilde{\mu}|_{U} is a Borel measure on (U,dU)(U,d_{U}) with μ~∣U(U)=μ~(U)=1\tilde{\mu}|_{U}(U)=\tilde{\mu}(U)=1. By claim 3 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions the map gg is continuous on UU as a map from (U,dU)(U,d_{U}) into (Rm,dE)(\mathbb{R}^{m},d_{E}), hence measurable with respect to B(U)\mathcal{B}(U) and B(Rm)\mathcal{B}(\mathbb{R}^{m}) by claim 3 of Borel Measurability and Bounded Integration on a Metric Space. Let μ\mu be the image measure of μ~∣U\tilde{\mu}|_{U} under gg, formed by claim 1 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables; by that claim μ\mu is a measure on (Rm,B(Rm))(\mathbb{R}^{m},\mathcal{B}(\mathbb{R}^{m})) with μ(Rm)=μ~∣U(U)=1\mu(\mathbb{R}^{m})=\tilde{\mu}|_{U}(U)=1, so μ∈P(Rm)\mu\in\mathcal{P}(\mathbb{R}^{m}) by Probability Measures on Euclidean Space and Random Vectors: Standing Notation (iii).

Step 5 (weak convergence). Let f:Rm→Rf:\mathbb{R}^{m}\to\mathbb{R} be bounded and continuous on Rm\mathbb{R}^{m}, and let MM be a nonnegative real number with ∣f(x)∣≤M|f(x)|\le M for every x∈Rmx\in\mathbb{R}^{m}. Being continuous, ff is measurable with respect to B(Rm)\mathcal{B}(\mathbb{R}^{m}) by claim 3 of Borel Measurability and Bounded Integration on a Metric Space, and integrable with respect to every probability measure on Rm\mathbb{R}^{m} by claim 6(b) of that lemma. Let η∈R\eta\in\mathbb{R} satisfy 0<η0<\eta. The choices are made in this order: η\eta determines ε\varepsilon, then Step 3 determines KK and, in Case B, ρ\rho, σ\sigma and χ\chi, then FF, and finally the index NN.

Put ε=η(2(2M+1))−1\varepsilon=\eta\bigl(2(2M+1)\bigr)^{-1}, a positive real number, and run Step 3 with this ε\varepsilon.

Case A. Here 1≤ε1\le\varepsilon, so η=2(2M+1)ε≥2(2M+1)\eta=2(2M+1)\varepsilon\ge 2(2M+1) and therefore 2M<η2M<\eta. By claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space we have ∣∫Rmf dμnj∣≤M\bigl|\int_{\mathbb{R}^{m}}f\,d\mu_{n_{j}}\bigr|\le M for every jj and ∣∫Rmf dμ∣≤M\bigl|\int_{\mathbb{R}^{m}}f\,d\mu\bigr|\le M, so by claim 5 of Properties of the Absolute Value in an Ordered Field the difference of the two integrals has absolute value at most 2M2M, hence less than η\eta, for every j∈Nj\in\mathbb{N}.

Case B. Let F:Bˉ→RF:\bar{B}\to\mathbb{R} be the map given by claim 6 of The Radial Compactification of Euclidean Space: Norm Continuity, a Homeomorphism onto the Open Unit Ball, Radial Cutoffs, and Extension of Test Functions for the data ρ\rho, σ\sigma, χ\chi and ff of Step 3. Thus FF is continuous on Bˉ\bar{B} as a map from (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}), ∣F∣≤M|F|\le M, F(h(x))=χ(h(x))f(x)F(h(x))=\chi(h(x))f(x) for every x∈Rmx\in\mathbb{R}^{m}, and F(y)=0F(y)=0 whenever y∈Bˉy\in\bar{B} and σ≤∥y∥\sigma\le\lVert y\rVert; in particular F(y)=0F(y)=0 for every y∈Bˉ∖Uy\in\bar{B}\setminus U, since such a yy satisfies ∥y∥=1\lVert y\rVert=1 and σ<1\sigma<1. By claims 3 and 6(b) of Borel Measurability and Bounded Integration on a Metric Space, FF is measurable with respect to B(Bˉ)\mathcal{B}(\bar{B}) and integrable with respect to μ~n\tilde{\mu}_{n} for every nn and with respect to μ~\tilde{\mu}.

(a) The approximating side. Since F∘hBˉF\circ h_{\bar{B}} is the map x↦χ(h(x))f(x)x\mapsto\chi(h(x))f(x), claim 2 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables gives ∫BˉF dμ~n=∫Rmχ(h(x))f(x) μn(dx)\int_{\bar{B}}F\,d\tilde{\mu}_{n}=\int_{\mathbb{R}^{m}}\chi(h(x))f(x)\,\mu_{n}(dx) for every nn, and claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion gives

∫Rmf dμn−∫BˉF dμ~n=∫Rm(1−χ(h(x)))f(x) μn(dx).\int_{\mathbb{R}^{m}}f\,d\mu_{n}-\int_{\bar{B}}F\,d\tilde{\mu}_{n}=\int_{\mathbb{R}^{m}}\bigl(1-\chi(h(x))\bigr)f(x)\,\mu_{n}(dx).

The integrand is continuous, hence measurable; it has absolute value at most MM, because 0≤1−χ(h(x))≤10\le 1-\chi(h(x))\le 1 and ∣f∣≤M|f|\le M; and it vanishes on KK by (i). Step 0, applied with Z=RmZ=\mathbb{R}^{m}, ν=μn\nu=\mu_{n} and A=Rm∖KA=\mathbb{R}^{m}\setminus K, gives

∣∫Rmf dμn−∫BˉF dμ~n∣≤M μn(Rm∖K)≤Mε(n∈N).\Bigl|\int_{\mathbb{R}^{m}}f\,d\mu_{n}-\int_{\bar{B}}F\,d\tilde{\mu}_{n}\Bigr|\le M\,\mu_{n}(\mathbb{R}^{m}\setminus K)\le M\varepsilon\qquad(n\in\mathbb{N}).

(b) The limit side. By claim 2 of Image Measures and Measures with a Density: Measures, Integrals and Change of Variables, applied to the image measure μ\mu of μ~∣U\tilde{\mu}|_{U} under gg and to the bounded measurable map ff, we have ∫Rmf dμ=∫Uf∘g d(μ~∣U)\int_{\mathbb{R}^{m}}f\,d\mu=\int_{U}f\circ g\,d(\tilde{\mu}|_{U}). Since FF vanishes on Bˉ∖U\bar{B}\setminus U, The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (vi), applied to (Bˉ,dBˉ)(\bar{B},d_{\bar{B}}), the set UU, the measure μ~\tilde{\mu} and the function FF, gives ∫BˉF dμ~=∫UF∣U d(μ~∣U)\int_{\bar{B}}F\,d\tilde{\mu}=\int_{U}F|_{U}\,d(\tilde{\mu}|_{U}), and F∣UF|_{U} is the map y↦χ(y)f(g(y))y\mapsto\chi(y)f(g(y)) on UU. Writing χU\chi_{U} for the restriction of χ\chi to UU, claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion gives

∫Rmf dμ−∫BˉF dμ~=∫U(1−χU) (f∘g) d(μ~∣U),\int_{\mathbb{R}^{m}}f\,d\mu-\int_{\bar{B}}F\,d\tilde{\mu}=\int_{U}\bigl(1-\chi_{U}\bigr)\,(f\circ g)\,d(\tilde{\mu}|_{U}),

all the integrands being continuous on UU, hence measurable with respect to B(U)\mathcal{B}(U) by claim 3 of Borel Measurability and Bounded Integration on a Metric Space, and bounded, hence integrable by claim 6(b) of that lemma. Pointwise on UU,

−M(1−χU)≤(1−χU)(f∘g)≤M(1−χU),-M\bigl(1-\chi_{U}\bigr)\le\bigl(1-\chi_{U}\bigr)(f\circ g)\le M\bigl(1-\chi_{U}\bigr),

since 0≤1−χU≤10\le 1-\chi_{U}\le 1 and ∣f∣≤M|f|\le M; integrating and using the monotonicity and the linearity of claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion, together with claim 6 of Properties of the Absolute Value in an Ordered Field,

∣∫Rmf dμ−∫BˉF dμ~∣≤M∫U(1−χU) d(μ~∣U)=M(1−∫UχU d(μ~∣U)),\Bigl|\int_{\mathbb{R}^{m}}f\,d\mu-\int_{\bar{B}}F\,d\tilde{\mu}\Bigr|\le M\int_{U}\bigl(1-\chi_{U}\bigr)\,d(\tilde{\mu}|_{U})=M\Bigl(1-\int_{U}\chi_{U}\,d(\tilde{\mu}|_{U})\Bigr),

the last step by claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space and μ~∣U(U)=1\tilde{\mu}|_{U}(U)=1. Finally χBˉ\chi_{\bar{B}} vanishes on Bˉ∖U\bar{B}\setminus U, so The Metric Subspace: Continuity, the Borel Sigma-Algebra, and the Restriction of a Borel Measure (vi) gives ∫UχU d(μ~∣U)=∫BˉχBˉ dμ~\int_{U}\chi_{U}\,d(\tilde{\mu}|_{U})=\int_{\bar{B}}\chi_{\bar{B}}\,d\tilde{\mu}, which is at least 1−ε1-\varepsilon by (ii). Hence

∣∫Rmf dμ−∫BˉF dμ~∣≤Mε.\Bigl|\int_{\mathbb{R}^{m}}f\,d\mu-\int_{\bar{B}}F\,d\tilde{\mu}\Bigr|\le M\varepsilon .

(c) Conclusion. The map FF is bounded and continuous on Bˉ\bar{B}, so by Step 2 the sequence (∫BˉF dμ~nj)j∈N\bigl(\int_{\bar{B}}F\,d\tilde{\mu}_{n_{j}}\bigr)_{j\in\mathbb{N}} converges to ∫BˉF dμ~\int_{\bar{B}}F\,d\tilde{\mu}; by Limit of a Sequence of Real Numbers there is N∈NN\in\mathbb{N} such that

∣∫BˉF dμ~nj−∫BˉF dμ~∣<εfor every j∈N with N≤j.\Bigl|\int_{\bar{B}}F\,d\tilde{\mu}_{n_{j}}-\int_{\bar{B}}F\,d\tilde{\mu}\Bigr|<\varepsilon\qquad\text{for every }j\in\mathbb{N}\text{ with }N\le j .

For such jj, claim 5 of Properties of the Absolute Value in an Ordered Field, applied twice to the decomposition of ∫f dμnj−∫f dμ\int f\,d\mu_{n_{j}}-\int f\,d\mu into the three differences bounded in (a), (c) and (b), gives

∣∫Rmf dμnj−∫Rmf dμ∣≤Mε+ε+Mε=(2M+1)ε=2−1η<η.\Bigl|\int_{\mathbb{R}^{m}}f\,d\mu_{n_{j}}-\int_{\mathbb{R}^{m}}f\,d\mu\Bigr|\le M\varepsilon+\varepsilon+M\varepsilon=(2M+1)\varepsilon=2^{-1}\eta<\eta .

In both cases we have produced, for the given η\eta, an index NN beyond which the difference of the two integrals has absolute value less than η\eta. As η\eta was an arbitrary positive real number, (∫Rmf dμnj)j∈N\bigl(\int_{\mathbb{R}^{m}}f\,d\mu_{n_{j}}\bigr)_{j\in\mathbb{N}} converges to ∫Rmf dμ\int_{\mathbb{R}^{m}}f\,d\mu in the sense of Limit of a Sequence of Real Numbers. As ff was an arbitrary bounded continuous real-valued map on Rm\mathbb{R}^{m}, the subsequence (μnj)j∈N(\mu_{n_{j}})_{j\in\mathbb{N}} converges weakly to μ\mu on (Rm,dE)(\mathbb{R}^{m},d_{E}) in the sense of Weak Convergence of Finite Borel Measures on a Metric Space.

Citations

Loading…

Dependencies

Uses0

Loading…

Comments

Log in to comment.

Loading…