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Proof of Restricted Lebesgue Measure and Integral Toolkit on a Compact Interval

lemmalem:interval-lebesgue-toolkit-2026a
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Reason: Initial publication of the proof of the interval integration toolkit lemma.

Proof

Throughout, B\mathcal{B}, λ\lambda, B[a,b]\mathcal{B}_{[a,b]}, λ[a,b]\lambda_{[a,b]}, and zero extensions are as in the statement. We use that the Borel σ\sigma-algebra contains every open subset of R\mathbb{R} and, by closure of a σ\sigma-algebra under complements, every closed subset; in particular [a,b]B[a,b]\in\mathcal{B}. We also record for repeated use the monotonicity of a measure: if EFE\subseteq F are members of a σ\sigma-algebra on which μ\mu is a measure, then μ(E)μ(F)\mu(E)\le\mu(F), since μ(F)=μ(E)+μ(FE)\mu(F)=\mu(E)+\mu(F\setminus E) by additivity, with nonnegative terms.

Claim 1. Every member of B[a,b]\mathcal{B}_{[a,b]} has the form S[a,b]S\cap[a,b] with SBS\in\mathcal{B} and hence lies in B\mathcal{B}, being an intersection of two members of B\mathcal{B}. The collection B[a,b]\mathcal{B}_{[a,b]} is a σ\sigma-algebra on [a,b][a,b]: it contains [a,b]=R[a,b][a,b]=\mathbb{R}\cap[a,b]; if E=S[a,b]E=S\cap[a,b] then [a,b]E=(RS)[a,b]B[a,b][a,b]\setminus E=(\mathbb{R}\setminus S)\cap[a,b]\in\mathcal{B}_{[a,b]}; and if En=Sn[a,b]E_n=S_n\cap[a,b] for nNn\in\mathbb{N} then nEn=(nSn)[a,b]B[a,b]\bigcup_nE_n=\bigl(\bigcup_nS_n\bigr)\cap[a,b]\in\mathcal{B}_{[a,b]}. The set function λ[a,b]\lambda_{[a,b]} is a measure: λ[a,b]()=λ()=0\lambda_{[a,b]}(\emptyset)=\lambda(\emptyset)=0, and for pairwise disjoint EnB[a,b]BE_n\in\mathcal{B}_{[a,b]}\subseteq\mathcal{B}, countable additivity of λ\lambda gives λ[a,b](nEn)=nλ[a,b](En)\lambda_{[a,b]}\bigl(\bigcup_nE_n\bigr)=\sum_n\lambda_{[a,b]}(E_n). By claim 4 of Existence of Lebesgue Measure on the Real Line, λ([a,b])=ba\lambda([a,b])=b-a. Finally, multiplying a measure by the positive constant (ba)1(b-a)^{-1} preserves μ()=0\mu(\emptyset)=0 and countable additivity, and gives total mass (ba)1(ba)=1(b-a)^{-1}(b-a)=1, so ([a,b],B[a,b],(ba)1λ[a,b])([a,b],\mathcal{B}_{[a,b]},(b-a)^{-1}\lambda_{[a,b]}) is a probability space.

We record a scaling identity used below: for every constant c>0c>0, every B[a,b]\mathcal{B}_{[a,b]}-measurable h:[a,b][0,]h:[a,b]\to[0,\infty] satisfies hd(cλ[a,b])=chdλ[a,b]\int h\,d(c\,\lambda_{[a,b]})=c\int h\,d\lambda_{[a,b]}. Indeed, by Simple Function and Its Integral the integral of a simple function s=ici1Ais=\sum_ic_i\mathbf{1}_{A_i} with respect to cλ[a,b]c\,\lambda_{[a,b]} is icicλ[a,b](Ai)\sum_ic_i\,c\,\lambda_{[a,b]}(A_i), which is cc times its integral with respect to λ[a,b]\lambda_{[a,b]}; the class of simple functions below hh is the same for both measures, and the supremum defining the integral scales by cc.

Claim 2. Let f:[a,b][0,]f:[a,b]\to[0,\infty] and let AA be a Borel subset of [0,][0,\infty] in the sense of Lebesgue Integral of a Nonnegative Measurable Function. If 0A0\notin A then f~1(A)=f1(A)\tilde f^{-1}(A)=f^{-1}(A), and if 0A0\in A then f~1(A)=f1(A)(R[a,b])\tilde f^{-1}(A)=f^{-1}(A)\cup(\mathbb{R}\setminus[a,b]). If ff is B[a,b]\mathcal{B}_{[a,b]}-measurable then f1(A)B[a,b]Bf^{-1}(A)\in\mathcal{B}_{[a,b]}\subseteq\mathcal{B} and R[a,b]B\mathbb{R}\setminus[a,b]\in\mathcal{B}, so f~\tilde f is B\mathcal{B}-measurable. Conversely, if f~\tilde f is B\mathcal{B}-measurable then f1(A)=f~1(A)[a,b]B[a,b]f^{-1}(A)=\tilde f^{-1}(A)\cap[a,b]\in\mathcal{B}_{[a,b]}.

For the integrals, we set up a correspondence of simple functions. If ss is a simple function on ([a,b],B[a,b])([a,b],\mathcal{B}_{[a,b]}) with sfs\le f, its zero extension s~\tilde s is simple on (R,B)(\mathbb{R},\mathcal{B}) with s~f~\tilde s\le\tilde f, and by Simple Function and Its Integral the two integrals agree, the added value 00 on R[a,b]\mathbb{R}\setminus[a,b] contributing 00 by the convention 0=00\cdot\infty=0 of Measure, Measure Space, and Probability Measure. Conversely, if ss' is simple on (R,B)(\mathbb{R},\mathcal{B}) with sf~s'\le\tilde f, then s=0s'=0 on R[a,b]\mathbb{R}\setminus[a,b] because f~=0\tilde f=0 there and s0s'\ge0; hence ss' is the zero extension of its restriction to [a,b][a,b], which is simple with s[a,b]fs'\restriction_{[a,b]}\le f and has the same integral. The two suprema in Lebesgue Integral of a Nonnegative Measurable Function therefore coincide, which is the asserted equality. For real-valued ff, apply the above to the positive and negative parts, noting (f+)~=(f~)+\widetilde{(f^{+})}=(\tilde f)^{+} and (f)~=(f~)\widetilde{(f^{-})}=(\tilde f)^{-}, and use Integrable Function and the Lebesgue Integral.

Claim 3. Let f:[a,b]Rf:[a,b]\to\mathbb{R} be continuous. By claims 2 and 3 of Agreement of the Riemann and Lebesgue Integrals for Continuous Functions on a Closed Interval, f~\tilde f is B\mathcal{B}-measurable and λ\lambda-integrable with Rf~dλ\int_{\mathbb{R}}\tilde f\,d\lambda equal to the Riemann integral of ff. By claim 2 above, ff is B[a,b]\mathcal{B}_{[a,b]}-measurable and [a,b]fdλ[a,b]=Rf~dλ\int_{[a,b]}f\,d\lambda_{[a,b]}=\int_{\mathbb{R}}\tilde f\,d\lambda, proving the displayed equality; in particular ff is a random variable on the probability space of claim 1. By Extreme Value Theorem on a Compact Interval there is M0M\ge0 with fM|f|\le M on [a,b][a,b]; f2f^{2} is continuous by Sums and Products of Continuous Real-Valued Functions (in its one-dimensional instance), so by the same argument f2f^{2} is measurable with [a,b]f2dλ[a,b]\int_{[a,b]}f^{2}\,d\lambda_{[a,b]} equal to its Riemann integral, which is at most M2(ba)M^{2}(b-a) by claim 4 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals applied to the continuous function f2f^{2} on [a,b][a,b]. By the scaling identity, the expectation of f2f^{2} on the normalized space is (ba)1[a,b]f2dλ[a,b]<(b-a)^{-1}\int_{[a,b]}f^{2}\,d\lambda_{[a,b]}<\infty, so ff is square-integrable there.

Claim 4. Work on the probability space ([a,b],B[a,b],Q)([a,b],\mathcal{B}_{[a,b]},\mathbb{Q}) of claim 1, Q:=(ba)1λ[a,b]\mathbb{Q}:=(b-a)^{-1}\lambda_{[a,b]}, and write EQ\mathbb{E}_{\mathbb{Q}} for its expectation. By the scaling identity, EQ[f2]=(ba)1[a,b]f2dλ[a,b]<\mathbb{E}_{\mathbb{Q}}[f^{2}]=(b-a)^{-1}\int_{[a,b]}f^{2}\,d\lambda_{[a,b]}<\infty and likewise for gg, so ff and gg are square-integrable random variables on this space. By Square-Integrable Random Variables and the Mean-Square Inner Product the product fgfg is Q\mathbb{Q}-integrable, hence λ[a,b]\lambda_{[a,b]}-integrable by the scaling identity applied to (fg)±(fg)^{\pm}, and claim 1 of Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm gives EQ[fg]2EQ[f2]EQ[g2]\bigl|\mathbb{E}_{\mathbb{Q}}[fg]\bigr|^{2}\le\mathbb{E}_{\mathbb{Q}}[f^{2}]\,\mathbb{E}_{\mathbb{Q}}[g^{2}]. Multiplying both sides by (ba)2(b-a)^{2} and using the scaling identity again yields the stated inequality. For the final assertion take g=1g=1, which is measurable with [a,b]g2dλ[a,b]=ba\int_{[a,b]}g^{2}\,d\lambda_{[a,b]}=b-a, and replace ff by f|f|, which satisfies f2=f2|f|^{2}=f^{2} and is measurable: for a Borel set ARA\subseteq\mathbb{R},

f1(A)=f1((A[0,))((A(0,)))),|f|^{-1}(A)=f^{-1}\Bigl(\bigl(A\cap[0,\infty)\bigr)\cup\bigl(-(A\cap(0,\infty))\bigr)\Bigr),

and B:={x:xB}-B:=\{-x:x\in B\} is Borel for every Borel BB, because the collection of sets BB with BB-B\in\mathcal{B} is a σ\sigma-algebra containing all open sets (the reflection of an open set is open).

Claim 5. On the probability space of claim 1, f0f\ge0 is a random variable with EQ[f]=(ba)10=0\mathbb{E}_{\mathbb{Q}}[f]=(b-a)^{-1}\cdot0=0 by the scaling identity. For every n1n\ge1, Markov's inequality (Markov's and Chebyshev's Inequalities) gives Q(f1/n)nEQ[f]=0\mathbb{Q}(f\ge1/n)\le n\,\mathbb{E}_{\mathbb{Q}}[f]=0, so λ[a,b]({f1/n})=0\lambda_{[a,b]}(\{f\ge1/n\})=0. Since {f>0}=n1{f1/n}\{f>0\}=\bigcup_{n\ge1}\{f\ge1/n\}, countable subadditivity gives λ[a,b]({f>0})=0\lambda_{[a,b]}(\{f>0\})=0; subadditivity follows from countable additivity by replacing An:={f1/n}A_n:=\{f\ge1/n\} with the disjoint sets Bn:=Ani<nAiB_n:=A_n\setminus\bigcup_{i<n}A_i and using λ[a,b](Bn)λ[a,b](An)\lambda_{[a,b]}(B_n)\le\lambda_{[a,b]}(A_n), which is the monotonicity recorded in the preamble.

Claim 6. Write N:=[a,b]DN:=[a,b]\setminus D, so λ[a,b](N)=0\lambda_{[a,b]}(N)=0. For each nn the function hn:=fn1Dh_n:=f_n\mathbf{1}_D is B[a,b]\mathcal{B}_{[a,b]}-measurable: for a Borel set A[0,]A\subseteq[0,\infty], its preimage is fn1(A)Df_n^{-1}(A)\cap D if 0A0\notin A and (fn1(A)D)N\bigl(f_n^{-1}(A)\cap D\bigr)\cup N if 0A0\in A, and both belong to B[a,b]\mathcal{B}_{[a,b]}. For every t[a,b]t\in[a,b] we have hn(t)f(t)h_n(t)\to f(t): on DD this is the hypothesis, and on NN both sides are 00. Hence f=lim infnhnf=\liminf_nh_n pointwise (nonnegative real-valued functions are in particular [0,][0,\infty]-valued), so ff is measurable by Fatou's Lemma.

For the integral identity, let g:[a,b][0,]g:[a,b]\to[0,\infty] be measurable. As in the previous paragraph, g1Dg\mathbf{1}_D and g1Ng\mathbf{1}_N are measurable, and g=g1D+g1Ng=g\mathbf{1}_D+g\mathbf{1}_N pointwise, so by linearity of the integral of nonnegative measurable functions (Linearity and Monotonicity of the Lebesgue Integral) it suffices to show [a,b]g1Ndλ[a,b]=0\int_{[a,b]}g\mathbf{1}_N\,d\lambda_{[a,b]}=0. Let s=ici1Ais=\sum_ic_i\mathbf{1}_{A_i} be any simple function with 0sg1N0\le s\le g\mathbf{1}_N, written with pairwise disjoint AiA_i and, discarding zero terms, with every ci>0c_i>0. For tNt\notin N we have g1N(t)=0g\mathbf{1}_N(t)=0, so s(t)=0s(t)=0 and therefore AiNA_i\subseteq N for every ii; the monotonicity recorded in the preamble gives λ[a,b](Ai)=0\lambda_{[a,b]}(A_i)=0, so the integral of ss is 00. Taking the supremum over such ss in Lebesgue Integral of a Nonnegative Measurable Function yields [a,b]g1Ndλ[a,b]=0\int_{[a,b]}g\mathbf{1}_N\,d\lambda_{[a,b]}=0, as required.

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