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Proof of The Radon-Nikodym Theorem for a Finite Measure and a Sigma-Finite Measure, and Uniqueness of Densities

theoremthm:radon-nikodym-sigma-finite-2026a
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· 17,294 chars · 27 deps · depth 21 Reason: Proof of thm:radon-nikodym-sigma-finite-2026a (von Neumann's argument).

Uniqueness: the nonnegative function 1_E(h1-h2) on E={h1>h2} has integral nu(E)-nu(E)=0, so E is null, and symmetrically. Existence (von Neumann): replace mu by a finite equivalent measure w mu, represent g -> int g dnu on L2(nuL^2(nu + w mu) by the Riesz theorem, and turn the representing function k in [0,1] into the density k/(1-k) times w by a geometric-series and monotone-convergence argument.

Proof

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

Two conventions are used throughout. First, if λ\lambda is a measure on (X,F)(X,\mathcal{F}) and u:XRu:X\to\mathbb{R} is measurable, integrable with respect to λ\lambda and satisfies 0u(x)0\le u(x) for every xx, then its integral in the sense of the integrable case equals its integral as a [0,][0,\infty]-valued map, because by that definition its positive part is uu and its negative part is the zero function; this identification is used without further comment. Second, (B0): if λ\lambda is a finite measure on (X,F)(X,\mathcal{F}) and u:XRu:X\to\mathbb{R} is measurable with u(x)M|u(x)|\le M for every xx, for a real M0M\ge0, then u|u| is measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and by claim 1 of Linearity and Monotonicity of the Lebesgue Integral together with The Integral of an Indicator Function is the Measure of the Set we have XudλXM1Xdλ=Mλ(X)<\int_X|u|\,d\lambda\le\int_X M\mathbf{1}_X\,d\lambda=M\lambda(X)<\infty, so uu is integrable with respect to λ\lambda by the criterion of Measure Spaces and the Lebesgue Integral: Standing Notation §integral.

Claim 1 (Uniqueness). Let h1,h2h_1,h_2 be densities of ν\nu with respect to μ\mu.

Step 1. For i{1,2}i\in\{1,2\}, taking A=XA=X in the defining identity gives Xhidμ=X1Xhidμ=ν(X)\int_X h_i\,d\mu=\int_X\mathbf{1}_Xh_i\,d\mu=\nu(X), a real number because ν\nu is finite. Since 0hi0\le h_i, we have hi=hi|h_i|=h_i, so hih_i is integrable by Measure Spaces and the Lebesgue Integral: Standing Notation §integral, with integral ν(X)\nu(X).

Step 2. Let E={xX:h2(x)<h1(x)}E=\{x\in X:h_2(x)<h_1(x)\}. The difference h1h2h_1-h_2 is measurable by claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, so E={x:0<(h1h2)(x)}E=\{x:0<(h_1-h_2)(x)\} belongs to F\mathcal{F} by claim 3 of Rational Intervals and Rays Generate the Borel Sigma-Algebra of the Real Line. The function u=1E(h1h2)u=\mathbf{1}_E(h_1-h_2) is measurable by claims 1 and 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions; it is positive on EE and 00 off EE. Thus 1Eh1=1Eh2+u\mathbf{1}_Eh_1=\mathbf{1}_Eh_2+u with all three functions nonnegative and measurable, and claim 1 of Linearity and Monotonicity of the Lebesgue Integral gives

X1Eh1dμ=X1Eh2dμ+Xudμin [0,].\int_X\mathbf{1}_Eh_1\,d\mu=\int_X\mathbf{1}_Eh_2\,d\mu+\int_Xu\,d\mu\qquad\text{in }[0,\infty].

Both integrals X1Ehidμ\int_X\mathbf{1}_Eh_i\,d\mu equal ν(E)\nu(E), which is real since ν(E)ν(X)\nu(E)\le\nu(X) by claim 2 of Basic Properties of a Measure. If Xudμ\int_Xu\,d\mu were \infty the right-hand side would be \infty; so it is real, and then it equals 00. By The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §vanishing, u(x)=0u(x)=0 for almost every xx; the set where u0u\ne0 is EE, so EE is null: EBE\subseteq B for some BFB\in\mathcal{F} with μ(B)=0\mu(B)=0. As EFE\in\mathcal{F}, claim 2 of Basic Properties of a Measure gives μ(E)μ(B)=0\mu(E)\le\mu(B)=0.

Step 3. Interchanging h1h_1 and h2h_2, the set E={x:h1(x)<h2(x)}E'=\{x:h_1(x)<h_2(x)\} belongs to F\mathcal{F} and μ(E)=0\mu(E')=0. The set {x:h1(x)h2(x)}\{x:h_1(x)\ne h_2(x)\} is the union of the disjoint sets EE and EE', so it belongs to F\mathcal{F} and has measure μ(E)+μ(E)=0\mu(E)+\mu(E')=0 by claim 1 of Basic Properties of a Measure.

Claim 2 (Existence). Suppose μ\mu is σ\sigma-finite and ν(A)=0\nu(A)=0 for every AFA\in\mathcal{F} with μ(A)=0\mu(A)=0.

Step 1 (a finite measure with the null sets of μ\mu). By the definition of σ\sigma-finiteness there is a sequence (Xm)mN(X_m)_{m\in\mathbb{N}} in F\mathcal{F} with X=mXmX=\bigcup_mX_m and μ(Xm)<\mu(X_m)<\infty for every mm. Put D1=X1D_1=X_1 and Dm=Xm(X1Xm1)D_m=X_m\setminus(X_1\cup\dots\cup X_{m-1}) for m2m\ge2; these belong to F\mathcal{F}, are pairwise disjoint, and each xXx\in X lies in exactly one of them, namely DmD_m for the least mm with xXmx\in X_m. Put cm=2m(1+μ(Xm))1c_m=2^{-m}(1+\mu(X_m))^{-1}, a positive real number by claims 5 and 7 of Elementary Order Arithmetic in an Ordered Field, and define w:XRw:X\to\mathbb{R} by w(x)=cmw(x)=c_m for xDmx\in D_m. Then 0<w(x)0<w(x) for every xx. For real aa, the set {x:a<w(x)}\{x:a<w(x)\} is mEm\bigcup_mE_m with Em=DmE_m=D_m if a<cma<c_m and Em=E_m=\varnothing otherwise, a member of F\mathcal{F}; so ww is measurable by claim 3 of Rational Intervals and Rays Generate the Borel Sigma-Algebra of the Real Line. For nNn\in\mathbb{N} let wn=m=1ncm1Dmw_n=\sum_{m=1}^{n}c_m\mathbf{1}_{D_m}, measurable by claims 1 and 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions. For each xx, wn(x)w_n(x) is 00 for nn below the index mm with xDmx\in D_m and w(x)w(x) from then on; so 0wnwn+10\le w_n\le w_{n+1} and w(x)w(x) is the least upper bound of {wn(x):nN}\{w_n(x):n\in\mathbb{N}\}. By claim 1 of Linearity and Monotonicity of the Lebesgue Integral, The Integral of an Indicator Function is the Measure of the Set, the bound μ(Dm)μ(Xm)\mu(D_m)\le\mu(X_m) from claim 2 of Basic Properties of a Measure, the elementary bound μ(Xm)(1+μ(Xm))11\mu(X_m)(1+\mu(X_m))^{-1}\le1, and the formula of Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §geometric with r=12r=\tfrac12,

Xwndμ=m=1ncmμ(Dm)m=1n2m=12n1.\int_Xw_n\,d\mu=\sum_{m=1}^{n}c_m\,\mu(D_m)\le\sum_{m=1}^{n}2^{-m}=1-2^{-n}\le1 .

By Monotone Convergence Theorem, Xwdμ1\int_Xw\,d\mu\le1. By claim 3 of Image Measures, Measures with Densities, and Change of Variables, μ(A)=X1Awdμ\mu'(A)=\int_X\mathbf{1}_Aw\,d\mu (AFA\in\mathcal{F}) defines a measure μ\mu' on (X,F)(X,\mathcal{F}), the measure with density ww with respect to μ\mu, and μ(X)=Xwdμ1\mu'(X)=\int_Xw\,d\mu\le1, so μ\mu' is finite.

For AFA\in\mathcal{F} we have μ(A)=0\mu(A)=0 if and only if μ(A)=0\mu'(A)=0. If μ(A)=0\mu(A)=0 then AA is null and 1Aw\mathbf{1}_Aw vanishes off AA, so μ(A)=0\mu'(A)=0 by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §null-integral. If μ(A)=0\mu'(A)=0 then 1Aw=0\mathbf{1}_Aw=0 almost everywhere by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §vanishing; since w>0w>0, the set where 1Aw0\mathbf{1}_Aw\ne0 is AA, so AA is null, and as AFA\in\mathcal{F} we get μ(A)=0\mu(A)=0 as in Step 2 of Claim 1.

Step 2 (the sum measure). For AFA\in\mathcal{F} put ρ(A)=ν(A)+μ(A)\rho(A)=\nu(A)+\mu'(A), a real number since ν(A)ν(X)\nu(A)\le\nu(X) and μ(A)μ(X)\mu'(A)\le\mu'(X) by claim 2 of Basic Properties of a Measure. Clearly ρ()=0\rho(\varnothing)=0. Let (Am)mN(A_m)_{m\in\mathbb{N}} be pairwise disjoint members of F\mathcal{F}, and let sn=m=1nν(Am)s_n=\sum_{m=1}^{n}\nu(A_m) and tn=m=1nμ(Am)t_n=\sum_{m=1}^{n}\mu'(A_m). By claims 1 and 2 of Basic Properties of a Measure, sn=ν(mnAm)ν(X)s_n=\nu(\bigcup_{m\le n}A_m)\le\nu(X) and likewise tnμ(X)t_n\le\mu'(X), so both sequences are nondecreasing and bounded above; by countable additivity and the definition of the sum of a sequence in that definition, (sn)(s_n) converges to ν(mAm)\nu(\bigcup_mA_m) and (tn)(t_n) to μ(mAm)\mu'(\bigcup_mA_m). Hence, by claim 1 of Arithmetic of Limits of Real Sequences, the partial sums sn+tns_n+t_n of mρ(Am)\sum_m\rho(A_m), which are bounded above by ρ(X)\rho(X), converge to ρ(mAm)\rho(\bigcup_mA_m), and by the same definition this limit is mρ(Am)\sum_m\rho(A_m). So ρ\rho is a finite measure on (X,F)(X,\mathcal{F}) with ρ(X)=ν(X)+μ(X)\rho(X)=\nu(X)+\mu'(X). If ρ(A)=0\rho(A)=0 then ν(A)=μ(A)=0\nu(A)=\mu'(A)=0, being nonnegative reals with sum 00.

(B1) For every measurable f:X[0,]f:X\to[0,\infty], Xfdρ=Xfdν+Xfdμ\int_Xf\,d\rho=\int_Xf\,d\nu+\int_Xf\,d\mu' in [0,][0,\infty]; in particular XfdνXfdρ\int_Xf\,d\nu\le\int_Xf\,d\rho. Indeed, for a nonnegative simple function ss with standard representation i=1rci1Ai\sum_{i=1}^{r}c_i\mathbf{1}_{A_i}, the definition of its integral in Simple Function and Its Integral gives Xsdρ=iciρ(Ai)=iciν(Ai)+iciμ(Ai)=Xsdν+Xsdμ\int_Xs\,d\rho=\sum_ic_i\rho(A_i)=\sum_ic_i\nu(A_i)+\sum_ic_i\mu'(A_i)=\int_Xs\,d\nu+\int_Xs\,d\mu', all real. By Approximation of Measurable Functions by Simple Functions §nonnegative there are nonnegative simple functions snsn+1s_n\le s_{n+1} whose pointwise least upper bound is ff. Put αn=Xsndν\alpha_n=\int_Xs_n\,d\nu and βn=Xsndμ\beta_n=\int_Xs_n\,d\mu', so that Xsndρ=αn+βn\int_Xs_n\,d\rho=\alpha_n+\beta_n. By Monotone Convergence Theorem for ν\nu, μ\mu' and ρ\rho, these nondecreasing sequences have least upper bounds Xfdν\int_Xf\,d\nu, Xfdμ\int_Xf\,d\mu' and Xfdρ\int_Xf\,d\rho in [0,][0,\infty], and converge to them. If Xfdν\int_Xf\,d\nu and Xfdμ\int_Xf\,d\mu' are both real, claim 1 of Arithmetic of Limits of Real Sequences shows that (αn+βn)(\alpha_n+\beta_n) converges to their sum, which is therefore Xfdρ\int_Xf\,d\rho. If one of them, say Xfdν\int_Xf\,d\nu, is \infty, then (αn)(\alpha_n) is not bounded above, hence neither is (αn+βn)(\alpha_n+\beta_n) since βn0\beta_n\ge0, and both sides equal \infty.

(B2) If f:XRf:X\to\mathbb{R} is measurable and bounded, then ff is integrable with respect to ν\nu, μ\mu' and ρ\rho by (B0), and Xfdρ=Xfdν+Xfdμ\int_Xf\,d\rho=\int_Xf\,d\nu+\int_Xf\,d\mu': apply (B1) to the bounded nonnegative positive and negative parts f+,ff^{+},f^{-}, whose integrals are all real, and subtract, using the definition of the integral in Integrable Function and the Lebesgue Integral.

Step 3 (the Riesz representation). Let L2\mathcal{L}^2 be the set of 22-integrable functions on (X,F,ρ)(X,\mathcal{F},\rho) and L2=L2(X,F,ρ)L^2=L^2(X,\mathcal{F},\rho) the Lebesgue space; by The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §hilbert it is a real Hilbert space with the inner product of The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product, whose norm is [g]g2[g]\mapsto\lVert g\rVert_2.

(i) Every measurable g:XRg:X\to\mathbb{R} with g(x)M|g(x)|\le M for all xx lies in L2\mathcal{L}^2: by Properties of Real Powers of Nonnegative Real Numbers §monotone, g(x)2M2|g(x)|^2\le M^2, so Xg2dρM2ρ(X)<\int_X|g|^2\,d\rho\le M^2\rho(X)<\infty by claim 1 of Linearity and Monotonicity of the Lebesgue Integral and The Integral of an Indicator Function is the Measure of the Set. In particular the constant function 11 lies in L2\mathcal{L}^2 with 12=ρ(X)1/2\lVert1\rVert_2=\rho(X)^{1/2}, since 12=11^2=1 by Properties of Real Powers of Nonnegative Real Numbers §agreement.

(ii) Let gL2g\in\mathcal{L}^2. The numbers 2,22,2 are conjugate exponents in the sense of Conjugate Exponents and Young's Inequality §conjugate, since 12+12=1\tfrac12+\tfrac12=1, so Hoelder's Inequality, for Two and for Finitely Many Factors §holder applied to gg and 11 gives Xgdρρ(X)1/2g2\int_X|g|\,d\rho\le\rho(X)^{1/2}\lVert g\rVert_2. By (B1) applied to g|g|, XgdνXgdρ<\int_X|g|\,d\nu\le\int_X|g|\,d\rho<\infty, so gg is integrable with respect to ν\nu by Measure Spaces and the Lebesgue Integral: Standing Notation §integral.

(iii) For gL2g\in\mathcal{L}^2 put ([g])=Xgdν\ell([g])=\int_Xg\,d\nu. This is well defined: if [g]=[g][g]=[g'] then, by The Lebesgue Space of Power-Integrable Functions §equivalence, the set where ggg\ne g' is contained in some BFB\in\mathcal{F} with ρ(B)=0\rho(B)=0, hence ν(B)=0\nu(B)=0 by Step 2, so g=gg=g' ν\nu-almost everywhere and Xgdν=Xgdν\int_Xg\,d\nu=\int_Xg'\,d\nu by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison (for the measure ν\nu). By the operations of The Lebesgue Space of Power-Integrable Functions §space and claim 2 of Linearity and Monotonicity of the Lebesgue Integral, \ell is linear. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral and (ii), ([g])Xgdνρ(X)1/2g2|\ell([g])|\le\int_X|g|\,d\nu\le\rho(X)^{1/2}\lVert g\rVert_2, and g2\lVert g\rVert_2 is the norm of [g][g] by The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product and The Lebesgue Space of Power-Integrable Functions §norm. Thus \ell is a bounded linear functional in the sense of Bounded Linear Maps and Bounded Linear Functionals on Real Inner Product Spaces, and the Operator Norm §functional, and The Riesz Representation Theorem for a Real Hilbert Space §existence yields zL2z\in L^2 with (x)=x,z\ell(x)=\langle x,z\rangle for every xL2x\in L^2. Let k0L2k_0\in\mathcal{L}^2 be a representative of zz. By The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product, for every gL2g\in\mathcal{L}^2 the product gk0gk_0 is ρ\rho-integrable and

(B3)Xgdν=Xgk0dρ.\text{(B3)}\qquad\int_Xg\,d\nu=\int_Xgk_0\,d\rho .

Step 4 (a representative with values in [0,1][0,1]). For AFA\in\mathcal{F}, 1AL2\mathbf{1}_A\in\mathcal{L}^2 by (i), so (B3) and The Integral of an Indicator Function is the Measure of the Set give ν(A)=X1Ak0dρ\nu(A)=\int_X\mathbf{1}_Ak_0\,d\rho. Let P={x:0<k0(x)}P=\{x:0<-k_0(x)\} and Q={x:0<k0(x)1}Q=\{x:0<k_0(x)-1\}; they lie in F\mathcal{F} by claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions and claim 3 of Rational Intervals and Rays Generate the Borel Sigma-Algebra of the Real Line, and they are disjoint. The function u=1Pk0u=-\mathbf{1}_Pk_0 is nonnegative, measurable and ρ\rho-integrable with Xudρ=ν(P)0\int_Xu\,d\rho=-\nu(P)\le0 by claim 2 of Linearity and Monotonicity of the Lebesgue Integral and (B3) with g=1Pg=\mathbf{1}_P; as an integral of a nonnegative function it is also 0\ge0, so it is 00, and The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §vanishing shows that u=0u=0 ρ\rho-almost everywhere. Since u>0u>0 on PP, PP is ρ\rho-null, and ρ(P)=0\rho(P)=0 as in Step 2 of Claim 1. Likewise u=1Qk01Qu'=\mathbf{1}_Qk_0-\mathbf{1}_Q is nonnegative, measurable and ρ\rho-integrable (1Q\mathbf{1}_Q by (B0)), with Xudρ=ν(Q)ρ(Q)0\int_Xu'\,d\rho=\nu(Q)-\rho(Q)\le0, by claim 2 of Linearity and Monotonicity of the Lebesgue Integral, (B3) with g=1Qg=\mathbf{1}_Q, and The Integral of an Indicator Function is the Measure of the Set for X1Qdρ=ρ(Q)\int_X\mathbf{1}_Q\,d\rho=\rho(Q), the inequality holding because ν(Q)ρ(Q)\nu(Q)\le\rho(Q); hence ρ(Q)=0\rho(Q)=0. Put k=min(1,max(0,k0))k=\min(1,\max(0,k_0)), measurable by claims 1 and 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, with 0k(x)10\le k(x)\le1 for every xx and k=k0k=k_0 off PQP\cup Q, where ρ(PQ)=0\rho(P\cup Q)=0 by claim 1 of Basic Properties of a Measure. For gL2g\in\mathcal{L}^2 the functions gkgk and gk0gk_0 therefore agree ρ\rho-almost everywhere, so by The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison and (B3) gkgk is ρ\rho-integrable and

(B4)Xgdν=Xgkdρ(gL2).\text{(B4)}\qquad\int_Xg\,d\nu=\int_Xgk\,d\rho\qquad(g\in\mathcal{L}^2).

Step 5 (splitting ρ\rho). Let g:XRg:X\to\mathbb{R} be measurable and bounded. Then gL2g\in\mathcal{L}^2 by (i), and gkgk is measurable and bounded, so (B4) and (B2) give Xgdν=Xgkdν+Xgkdμ\int_Xg\,d\nu=\int_Xgk\,d\nu+\int_Xgk\,d\mu', all integrands being integrable by (B0). By claim 2 of Linearity and Monotonicity of the Lebesgue Integral,

(B5)Xg(1k)dν=Xgkdμfor every bounded measurable g.\text{(B5)}\qquad\int_Xg(1-k)\,d\nu=\int_Xgk\,d\mu'\qquad\text{for every bounded measurable }g .

Let N={x:k(x)=1}=X{x:0<1k(x)}FN=\{x:k(x)=1\}=X\setminus\{x:0<1-k(x)\}\in\mathcal{F}. With g=1Ng=\mathbf{1}_N the left side of (B5) is the integral of the zero function, which is 00, while gk=1Ngk=\mathbf{1}_N; so μ(N)=0\mu'(N)=0 by The Integral of an Indicator Function is the Measure of the Set. By Step 1, μ(N)=0\mu(N)=0, and by hypothesis ν(N)=0\nu(N)=0. For xNx\notin N we have 0k(x)<10\le k(x)<1.

Step 6 (the density). Fix AFA\in\mathcal{F}. For jNj\in\mathbb{N} let pj=i=0j1kip_j=\sum_{i=0}^{j-1}k^i (with k0=1k^0=1) and qj=i=1jkiq_j=\sum_{i=1}^{j}k^i; they are measurable by claims 1 to 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 0pjj0\le p_j\le j, 0qjj0\le q_j\le j since 0ki10\le k^i\le1. By telescoping, (1k)pj=1kj(1-k)p_j=1-k^j and kpj=qjkp_j=q_j. Applying (B5) to g=1Apjg=\mathbf{1}_Ap_j gives

(B6)X1A(1kj)dν=X1Aqjdμ.\text{(B6)}\qquad\int_X\mathbf{1}_A(1-k^j)\,d\nu=\int_X\mathbf{1}_Aq_j\,d\mu' .

Left side: for xNx\in N, 1A(x)(1k(x)j)=0=1AN(x)\mathbf{1}_A(x)(1-k(x)^j)=0=\mathbf{1}_{A\setminus N}(x) for every jj; for xNx\notin N the sequence (k(x)j)j(k(x)^j)_j converges to 00 by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §geometric, so 1A(x)(1k(x)j)\mathbf{1}_A(x)(1-k(x)^j) converges to 1A(x)=1AN(x)\mathbf{1}_A(x)=\mathbf{1}_{A\setminus N}(x) by claims 1 and 3 of Arithmetic of Limits of Real Sequences. Since 1A(1kj)1|\mathbf{1}_A(1-k^j)|\le1 and the constant 11 is ν\nu-integrable by (B0), claim 3 of Dominated Convergence Theorem shows that the left side of (B6) converges to X1ANdν=ν(AN)\int_X\mathbf{1}_{A\setminus N}\,d\nu=\nu(A\setminus N) (The Integral of an Indicator Function is the Measure of the Set), and ν(AN)=ν(A)\nu(A\setminus N)=\nu(A) because ν(A)=ν(AN)+ν(AN)\nu(A)=\nu(A\setminus N)+\nu(A\cap N) and ν(AN)ν(N)=0\nu(A\cap N)\le\nu(N)=0 by claims 1 and 2 of Basic Properties of a Measure.

Right side: let rj=1ANqjr_j=\mathbf{1}_{A\setminus N}q_j. Since 1Aqj=rj\mathbf{1}_Aq_j=r_j off NN and μ(N)=0\mu'(N)=0, The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison (for μ\mu') gives X1Aqjdμ=Xrjdμ=:aj\int_X\mathbf{1}_Aq_j\,d\mu'=\int_Xr_j\,d\mu'=:a_j. The functions rjr_j are nonnegative, measurable and nondecreasing in jj, so (aj)(a_j) is nondecreasing by claim 1 of Linearity and Monotonicity of the Lebesgue Integral. Define h(x)=k(x)(1k(x))1h'(x)=k(x)(1-k(x))^{-1} for xNx\notin N and h(x)=0h'(x)=0 for xNx\in N. For xNx\notin N, qj(x)q_j(x) are the partial sums of the geometric series ik(x)i\sum_ik(x)^i, which by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §geometric converges with sum h(x)h'(x), and this sum is the least upper bound of the partial sums by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §criterion. Hence at every xx the sequence (1XN(x)qj(x))j(\mathbf{1}_{X\setminus N}(x)q_j(x))_j converges to h(x)h'(x), so hh' is measurable by claim 5 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 1Ah\mathbf{1}_Ah' (measurable by claim 3 there) is the pointwise least upper bound of (rj)(r_j). By Monotone Convergence Theorem, X1Ahdμ\int_X\mathbf{1}_Ah'\,d\mu' is the least upper bound of {aj:jN}\{a_j:j\in\mathbb{N}\}. By (B6) and the previous paragraph, (aj)(a_j) converges to ν(A)\nu(A). For each jj the sequence (amax(i,j))iN(a_{\max(i,j)})_{i\in\mathbb{N}} also converges to ν(A)\nu(A) and dominates the constant aja_j, so ajν(A)a_j\le\nu(A) by claim 1 of Order Properties of Limits of Real Sequences; and if ajUa_j\le U for all jj then ν(A)U\nu(A)\le U by the same claim. So ν(A)\nu(A) is the least upper bound of the aja_j, that is,

ν(A)=X1Ahdμ.\nu(A)=\int_X\mathbf{1}_Ah'\,d\mu' .

Finally, by claim 3 of Image Measures, Measures with Densities, and Change of Variables for the measure μ\mu' with density ww, applied to the measurable 1Ah:X[0,)\mathbf{1}_Ah':X\to[0,\infty), X1Ahdμ=X1Ahwdμ\int_X\mathbf{1}_Ah'\,d\mu'=\int_X\mathbf{1}_Ah'w\,d\mu. Let h=hwh=h'w; it is measurable by claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, real-valued and nonnegative, and ν(A)=X1Ahdμ\nu(A)=\int_X\mathbf{1}_Ah\,d\mu for every AFA\in\mathcal{F}. So hh is a density of ν\nu with respect to μ\mu.

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