Chapter 6

The Lebesgue Integral

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Problem 6.1.1

Let E∈FE \in \mathscr {F}.

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(a)

μ(E)=0\mu (E)=0 iff IEs(s)=0\mathcal{I}_{E}^{s}(s)=0 for every s∈Ss \in \mathbb {S}.

(b)

For any c⩾0,IEs(c)=cμ(E)c \geqslant 0, \mathcal{I}_{E}^{s}(c)=c \mu (E).

Problem 6.1.2

Let t,s,s1,s2,…∈St, s, s_{1}, s_{2}, \ldots \in \mathbb {S}. Why can't we say that IEs(as+bt)=aIEs(s)+bIEs(t)\mathfrak {I}_{E}^{s}(a s+ b t)=a \mathfrak {I}_{E}^{s}(s)+b \mathfrak {I}_{E}^{s}(t) for every a,b∈Ra, b \in \mathbb {R}, as compared to saying that the result holds for every 0⩽a,b<∞0 \leqslant a, b<\infty ? Also, why can't we necessarily write IEs(∑i=1∞cisi)=∑i=1∞ciIEs(si)\mathcal{I}_{E}^{s}\left(\sum_{i=1}^{\infty } c_{i} s_{i}\right)=\sum_{i=1}^{\infty } c_{i} \mathcal{I}_{E}^{s}\left(s_{i}\right) ?

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Problem 6.1.3

Let E∈FE \in \mathscr {F} be such that μ(E)>0\mu (E)>0. Then IEs(s)=0\mathcal{I}_{E}^{s}(s)=0 iff s=0μs=0 \mu-a. e. on E. In particular, Is(s)=0\mathcal{I}^{\mathcal{s}}(s)=0 iff s=0μs=0 \mu-a. e. [on Ω\Omega ].

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Problem 6.1.4

Let E∈FE \in \mathcal{F} and s∈Ss \in \mathbb {S}.

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(a)

If μ(E)<∞\mu (E)<\infty, then IEs(s)<∞\mathcal{I}_{E}^{s}(s)<\infty, but the converse is not necessarily true.

(b)

If μ(E)=∞\mu (E)=\infty and IEs(s)=∞\mathcal{I}_{E}^{s}(s)=\infty, then μ({ω∈E:s(ω)>0})>0\mu (\left\{ \omega \in E: s(\omega )>0\right\} )>0, but the converse is not necessarily true.

(c)

Let μ(E)=∞\mu (E)=\infty. Then IEI(s)<∞\mathcal{I}_{E}^{\mathcal{I}}(s)<\infty iff μ({ω∈E:s(ω)>0})<∞\mu (\left\{ \omega \in E: s(\omega )>0\right\} )<\infty.

Problem 6.1.5

Suppose that {En}n=1∞\left\{ E_{n}\right\}_{n=1}^{\infty } is a nonincreasing sequence of F\mathcal{F}-sets. Also, let s∈Ss \in \mathbb {S}.

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(a)

It is not necessarily the case that lim⁡nIEns(s)=Ilim⁡nEns(s)\lim_{n} \mathcal{I}_{E_{n}}^{s}(s)=\mathcal{I}_{\lim_{n} E_{n}}^{s}(s).

(b)

If IEns(s)<∞\mathcal{I}_{E_{n}}^{s}(s)<\infty for some n∈Nn \in \mathbb {N}, then lim⁡nIEns(s)=Ilim⁡nEns(s)\lim_{n} \mathcal{I}_{E_{n}}^{s}(s)=\mathcal{I}_{\lim_{n} E_{n}}^{s}(s).

(c)

If {En}n=1∞\left\{ E_{n}\right\}_{n=1}^{\infty } is no longer nonincreasing but is still such that lim⁡nEn\lim_{n} E_{n} exists, state conditions under which lim⁡nIEns(s)=Ilim⁡nEns(s)\lim_{n} \mathfrak {I}_{E_{n}}^{s}(s)=\mathfrak {I}_{\lim_{n} E_{n}}^{s}(s).

Problem 6.1.6

Let s∈Ss \in \mathbb {S} and recall (S7), where vsv_{s} is the measure on F\mathcal{F} with νs(B)=IBs(s)\nu_{s}(B)=\mathcal{I}_{B}^{s}(s) for every B∈FB \in \mathcal{F}. Then, for any E∈FE \in \mathcal{F} and t∈St \in \mathfrak {S}, we have IEs(t;νs)=IEs(ts;μ)\mathcal{I}_{E}^{s}\left(t ; \nu_{s}\right)=\mathcal{I}_{E}^{s}(t s ; \mu ).

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Problem 6.1.7

Let A∈FA \in \mathcal{F} be nonempty, and let s∈Ss \in \mathfrak {S}. Let FA={E⊆A:E∈F}\mathcal{F}_{A}=\left\{ E \subseteq A: E \in \mathcal{F}\right\}, and let μA\mu_{A} denote the restriction of μ\mu from F\mathcal{F} to FA\mathcal{F}_{A}. Finally, let sAs_{A} denote the restriction of ss from Ω\Omega to AA.

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(a)

(A,FA,μA)\left(A, \mathcal{F}_{A}, \mu_{A}\right) is a measure space.

(b)

If I\mathcal{I} denotes this section's functional relative to ( A,FA,μAA, \mathcal{F}_{A}, \mu_{A} ), then we have IEs(s;μ)=JE(sA;μA)\mathcal{I}_{E}^{s}(s ; \mu )=\mathcal{J}_{E}\left(s_{A} ; \mu_{A}\right) for every E∈FAE \in \mathcal{F}_{A}.

Problem 6.1.8

Let A∈F\{∅}A \in \mathcal{F} \backslash \left\{ \varnothing \right\}, and suppose that s:A→[0,∞)s: A \rightarrow [0, \infty ) is simple and F/B∗\mathcal{F} / \mathcal{B}^{*}-measurable. Let E∈FAE \in \mathcal{F}_{A}, where FA\mathcal{F}_{A} is defined in the previous exercise. Consider two programs:

Program 1 Extend ss from AA to Ω\Omega as follows: Let s∗∈Ss^{*} \in \mathbb {S} be such that s∗=ss^{*}=s on AA and s∗=0s^{*}=0 on AcA^{c}.

Program 2 Do not extend ss from AA to Ω\Omega as in Program 1, but instead view ss as a function defined everywhere relative to the measure space ( A,FA,μAA, \mathscr {F}_{A}, \mu_{A} ), where the notation is as in the previous exercise.

These two programs are equivalent in the sense that IEs(s∗;μ)=IE(s;μA)\mathcal{I}_{E}^{s}\left(s^{*} ; \mu \right)=\mathscr {I}_{E}\left(s ; \mu_{A}\right), where IEs\mathfrak {I}_{E}^{s} is this section's functional relative to the measure space ( Ω,F,μ\Omega , \mathcal{F}, \mu ), and JE\mathscr {J}_{E} is this section's functional relative to the measure space ( A,FA,μAA, \mathscr {F}_{A}, \mu_{A} ).

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Problem 6.1.9

Quickly prove the following "almost everywhere" modification of (S3) and (S4). As usual, s,t∈Ss, t \in \mathbb {S} and all sets are in F\mathcal{F}.

[(S3): if s=ts=t on EE, then IFs(s)=IFs(t)\mathcal{I}_{F}^{s}(s)=\mathcal{I}_{F}^{s}(t) for every F⊆EF \subseteq E. (S4): s⩽ts \leqslant t [on Ω\Omega] implies IEs(s)⩽IEs(t)\mathcal{I}_{E}^{s}(s) \leqslant \mathcal{I}_{E}^{s}(t); more generally, if s⩽ts \leqslant t on EE, then IFs(s)⩽IFs(t)\mathcal{I}_{F}^{s}(s) \leqslant \mathcal{I}_{F}^{s}(t) for every F⊆EF \subseteq E.]

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(a)

If s=tμs=t \mu-a.e. on EE, then IFs(s)=IFs(t)\mathfrak {I}_{F}^{s}(s)=\mathfrak {I}_{F}^{s}(t) for every F⊆EF \subseteq E.

(b)

If s⩽tμs \leqslant t \mu-a. e. on EE, then IFs(s)⩽IFs(t)\mathcal{I}_{F}^{s}(s) \leqslant \mathcal{I}_{F}^{s}(t) for every F⊆EF \subseteq E.

Problem 6.2.1

Prove

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(a)

(N3') If f=gμf=g \mu-a.e. on EE, then IFn(f)=IFn(g)\mathfrak {I}_{F}^{n}(f)=\mathfrak {I}_{F}^{n}(g) for any F⊆EF \subseteq E.

(b)

(N4') If f⩽gμf \leqslant g \mu-a. e. on EE, then IFn(f)⩽IFn(g)\mathcal{I}_{F}^{n}(f) \leqslant \mathcal{I}_{F}^{n}(g) for any F⊆EF \subseteq E.

(c)

(N7') If f,f1,f2,…∈ℜf, f_{1}, f_{2}, \ldots \in \Re and f=lim⁡nfnμf=\lim_{n} f_{n} \mu-a.e. on EE, then IEn(f)=lim⁡nIEn(fn)\mathcal{I}_{E}^{n}(f)= \lim_{n} \mathcal{I}_{E}^{n}\left(f_{n}\right).

(d)

If f⩽Mμf \leqslant M \mu-a.e. on EE for some M∈[0,∞]M \in [0, \infty ], then IEn(f)⩽Mμ(E)\mathcal{I}_{E}^{n}(f) \leqslant M \mu (E).

Problem 6.2.2

It was claimed in (N5) that IEn(cf)=cIEn(f)\mathcal{I}_{E}^{n}(c f)=c \mathcal{I}_{E}^{n}(f) for every c∈[0,∞)c \in [0, \infty ). This result in fact holds in c=∞c=\infty as well: IEn(∞f)=∞IEn(f)\mathfrak {I}_{E}^{n}(\infty f)=\infty \mathfrak {I}_{E}^{n}(f). Therefore, (N5) holds for all c∈[0,∞]c \in [0, \infty ]. Similarly, we may allow the numbers c1,…,cnc_{1}, \ldots , c_{n} to be in [0,∞]\left[0, \infty \right] in the statement (N8).

[(N8)(a): for functions g,f,f1,f2,…∈Ng, f, f_{1}, f_{2}, \ldots \in \mathfrak {N}, IEn(∑i=1ncifi)=∑i=1nciIEn(fi)\mathcal{I}_{E}^{n}\left(\sum_{i=1}^{n} c_{i} f_{i}\right)=\sum_{i=1}^{n} c_{i} \mathcal{I}_{E}^{n}\left(f_{i}\right) for every n∈Nn \in \mathbb {N} and choice of c1,…,cn∈[0,+∞)c_{1}, \ldots , c_{n} \in [0, +\infty ), so that IEn\mathcal{I}_{E}^{n} is linear in this sense; this problem extends that to c1,…,cn∈[0,+∞]c_{1}, \ldots , c_{n} \in [0, +\infty ].]

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Problem 6.2.3

This exercise concerns Fatou's Lemma.

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(a)

Let {An}\left\{ A_{n}\right\} denote a sequence of F\mathcal{F}-sets. Show that μ(lim inf⁡An)⩽lim inf⁡μ(An)\mu \left(\liminf A_{n}\right) \leqslant \liminf \mu \left(A_{n}\right) by using Fatou's Lemma applied to the sequence of indicator functions {  1An}n=1∞\left\{ \; \mathbb {1}_{A_{n}}\right\}_{n=1}^{\infty }.

(b)

Consider (R,B,λ)(\mathbb {R}, \mathfrak {B}, \lambda ). If sn=n2  1[0,1/n]s_{n}=n^{2} \; \mathbb {1}_{\left[0,1 / n\right]} for each n∈Nn \in \mathbb {N}, then In(lim inf⁡sn)=0\mathfrak {I}^{n}\left(\liminf s_{n}\right)=0 while lim inf⁡In(sn)=∞\liminf \mathfrak {I}^{n}\left(s_{n}\right)=\infty,hence strict inequality may hold in Fatou's Lemma.

(c)

In (b), with E∈BE \in B, the sequence   1E,1−  1E,  1E,1−  1E,…\; \mathbb {1}_{E}, 1-\; \mathbb {1}_{E}, \; \mathbb {1}_{E}, 1-\; \mathbb {1}_{E}, \ldots provides another example where strict inequality holds in Fatou's Lemma.

(d)

It is not necessarily the case that lim sup⁡IEn(fn)⩽IEn(lim sup⁡fn)\limsup \mathcal{I}_{E}^{n}\left(f_{n}\right) \leqslant \mathcal{I}_{E}^{n}\left(\limsup f_{n}\right) if μ(E)=∞\mu (E)= \infty. However, if μ(E)<∞\mu (E)<\infty, the inequality holds, hence we have

IEn(lim inf⁡fn)⩽lim inf⁡IEn(fn)⩽lim sup⁡IEn(fn)⩽IEn(lim sup⁡fn) \mathcal{I}_{E}^{n}\left(\liminf f_{n}\right) \leqslant \liminf \mathcal{I}_{E}^{n}\left(f_{n}\right) \leqslant \limsup \mathcal{I}_{E}^{n}\left(f_{n}\right) \leqslant \mathcal{I}_{E}^{n}\left(\limsup f_{n}\right)

by putting everything together.

Problem 6.2.4

Let Ω\Omega denote an arbitrary nonempty set, and fix attention upon a particular ω0∈Ω\omega_{0} \in \Omega. Let F=2Ω\mathcal{F}=2^{\Omega }, and define μ:F→R‾\mu : \mathcal{F} \rightarrow \overline{\mathbb {R}} by writing μ(A)=1\mu (A)=1 if ω0∈A\omega_{0} \in A and μ(A)=0\mu (A)=0 if ω0∉A\omega_{0} \notin A.

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(a)

(Ω,F,μ)(\Omega , \mathcal{F}, \mu ) is a measure space.

(b)

Every f:Ω→Rf: \Omega \rightarrow \mathbb {R} is F/B∗\mathcal{F} / \mathfrak {B}^{*}-measurable.

(c)

Let E∈FE \in \mathcal{F} and f∈ℜf \in \Re. Then IEn(f)=f(ω0)  1E(ω0)\mathcal{I}_{E}^{n}(f)=f\left(\omega_{0}\right) \; \mathbb {1}_{E}\left(\omega_{0}\right).

Problem 6.2.5

Let Ω\Omega denote an uncountable set, and let \mathcal{F}=\left\{ A \subseteq \Omega : A is amc or AcA^{c} is amc. Define μ:F→R‾\mu : \mathcal{F} \rightarrow \overline{\mathbb {R}} for all A∈FA \in \mathcal{F} by writing μ(A)=0\mu (A)=0 if AA is amc and μ(A)=1\mu (A)=1 if AcA^{c} is amc.

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(a)

(Ω,F,μ)(\Omega , \mathcal{F}, \mu ) is a measure space.

(b)

f:Ω→R‾f: \Omega \rightarrow \overline{\mathbb {R}} is F/B∗\mathcal{F} / \mathcal{B}^{*}-measurable iff there is c∈R‾c \in \overline{\mathbb {R}} [depending on ff ] with f=cμ−f=c \mu - a. e. on Ω\Omega.

(c)

Let E∈FE \in \mathcal{F} and f∈Nf \in \mathfrak {N}, then IEn(f)=c⋅μ(E)\mathcal{I}_{E}^{n}(f)=c \cdot \mu (E), where cc is the constant such that f=cμf=c \mu-a.e. on Ω\Omega [as given in (b)].

Problem 6.2.6

Let Ω\Omega denote an arbitrary nonempty set, let A⊆ΩA \subseteq \Omega, and let f:Ω→[0,∞]f: \Omega \rightarrow [0, \infty ] be given. Write

∑ω∈A∗f(ω)=sup⁡{∑ω∈Ff(ω):F⊆A,F finite } \sum _{\omega \in A}^{*} f(\omega )=\sup \left\{ \sum _{\omega \in F} f(\omega ): F \subseteq A, F \text{ finite }\right\}
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(a)

Suppose A={ω1,…,ωn}A=\left\{ \omega_{1}, \ldots , \omega_{n}\right\}. Then ∑ω∈A∗f(ω)=∑i=1nf(ωi)\sum_{\omega \in A}^{*} f(\omega )=\sum_{i=1}^{n} f\left(\omega_{i}\right), hence the definition above is consistent with what we're used to in the finite case.

(b)

Suppose A={ω1,ω2,…}A=\left\{ \omega_{1}, \omega_{2}, \ldots \right\} [a countable set]. Then ∑ω∈A∗f(ω)=∑i=1∞f(ωi)\sum_{\omega \in A}^{*} f(\omega )=\sum_{i=1}^{\infty } f\left(\omega_{i}\right).

Problem 6.2.7

Let Ω\Omega denote a nonempty set, let F=2Ω\mathcal{F}=2^{\Omega }, and let μ:F→R‾\mu : \mathcal{F} \rightarrow \overline{\mathbb {R}} be such that μ(A)=\mu (A)= the number of points in AA when AA is finite, and μ(A)=∞\mu (A)=\infty otherwise .

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(a)

( Ω,F,μ\Omega , \mathcal{F}, \mu ) is a measure space. The measure μ\mu is called the counting measure since μ\mu "counts" the number of points in each F\mathcal{F}-set.

(b)

Every f:Ω→R‾f: \Omega \rightarrow \overline{\mathbb {R}} is F/B∗\mathcal{F} / \mathscr {B}^{*}-measurable.

(c)

Given any E∈FE \in \mathcal{F} and f∈Nf \in \mathfrak {N}, we have IEn(f)=∑ω∈E∗f(ω)\mathcal{I}_{E}^{n}(f)=\sum_{\omega \in E}^{*} f(\omega ).

Problem 6.2.8

The previous exercise regarding counting measure has some interesting applications to statements regarding infinite series.

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(a)

If aij⩾0a_{ij} \geqslant 0 for each i,j∈Ni, j \in \mathbb {N}, then

∑i=1∞∑j=1∞aij=∑j=1∞∑i=1∞aij=∑(i,j)∈N2aij, \sum _{i=1}^{\infty } \sum _{j=1}^{\infty } a_{ij}=\sum _{j=1}^{\infty } \sum _{i=1}^{\infty } a_{ij}=\sum _{(i, j) \in \mathbb {N}^{2}} a_{ij},

where the last expression above is a standard unordered sum from advanced calculus. [This is a result that is demonstrated in advanced calculus courses independently of any measure or integration theory, and hence our usage of it before this exercise is not in any way circular. Here, the idea is to prove this by constructing the appropriate space and functions and using the results of the previous exercise.]

(b)

Let {anm:n,m∈N}\left\{ a_{nm}: n, m \in \mathbb {N}\right\} denote a double sequence of nonnegative numbers. Show that ∑n=1∞lim⁡‾manm⩽lim⁡‾m∑n=1∞anm\sum_{n=1}^{\infty } \underline{\lim }_{m} a_{nm} \leqslant \underline{\lim }_{m} \sum_{n=1}^{\infty } a_{nm}.

Problem 6.2.9

Consider the measure space (Ω,F,μ)(\Omega , \mathcal{F}, \mu ), and let E∈FE \in \mathcal{F}. For each f∈Nf \in \mathfrak {N}, define

JˉE(f)=sup⁡∑i=1ninf⁡{f(ω):ω∈Ai∩E}μ(Ai∩E), \bar{\mathcal{J}}_{E}(f)=\sup \sum _{i=1}^{n} \inf \left\{ f(\omega ): \omega \in A_{i} \cap E\right\} \mu \left(A_{i} \cap E\right),

where the supremum is taken over all finite disjoint collections {A1,⋯ ,An}\left\{ A_{1}, \cdots , A_{n}\right\} of F\mathcal{F}-sets with ⋃i=1nAi=Ω\bigcup_{i=1}^{n} A_{i}=\Omega. Then JˉE(f)=IˉE(f)\bar{\mathcal{J}}_{E}(f)=\bar{\mathcal{I}}_{E}(f), so that this is an equivalent formulation of what we have done in this section.

[Recall the arithmetical conventions +∞×0=0×+∞=0+\infty \times 0=0 \times +\infty =0 and inf⁡∅=+∞\inf \varnothing =+\infty for the case when some Ai=∅A_{i}=\varnothing.]

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Problem 6.2.10

Consider the measure space (Ω,F,μ)(\Omega , \mathcal{F}, \mu ), and let E∈FE \in \mathcal{F} and f∈Nf \in \mathfrak {N}. Define JˉE(f)=lim⁡nIE(sn)\bar{\mathcal{J}}_{E}(f)=\lim_{n} \mathcal{I}_{E}\left(s_{n}\right), where {sn}n=1∞\left\{ s_{n}\right\}_{n=1}^{\infty } is a nondecreasing sequence of functions in Sf\mathfrak {S}_{f} such that sn→fs_{n} \rightarrow f. We will show that JˉE(f)=IˉE(f)\bar{\mathcal{J}}_{E}(f)=\bar{\mathcal{I}}_{E}(f) without using MCT, so that this definition could have instead served as our definition.

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(a)

We first want to show that JˉE(f)\bar{\mathcal{J}}_{E}(f) is well-defined, since there are possibly many nondecreasing sequences {sn}n=1∞\left\{ s_{n}\right\}_{n=1}^{\infty } of elements of Sf\mathfrak {S}_{f} with sn→fs_{n} \rightarrow f. Let t∈Sft \in \mathfrak {S}_{f}, so that t⩽lim⁡nsn=ft \leqslant \lim_{n} s_{n}=f. If IE(t)=+∞\mathcal{I}_{E}(t)=+\infty, then lim⁡nIE(sn)=+∞\lim_{n} \mathcal{I}_{E}\left(s_{n}\right)=+\infty.

[By (MF18): for a nonempty A∈FA \in \mathcal{F} and a nonnegative F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable f:A→R‾f: A \rightarrow \overline{\mathbb {R}}, there exists a nondecreasing sequence of nonnegative, finite-valued, F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable simple functions on AA converging pointwise to ff on AA; Sf\mathfrak {S}_{f} denotes the collection of all such simple functions dominated by ff.]

(b)

If IE(t)<+∞\mathcal{I}_{E}(t)<+\infty, then lim⁡nIE(sn)⩾IE(t)\lim_{n} \mathcal{I}_{E}\left(s_{n}\right) \geqslant \mathcal{I}_{E}(t). This with (a) gives the inequality lim⁡nIE(sn)⩾IE(t)\lim_{n} \mathcal{I}_{E}\left(s_{n}\right) \geqslant \mathcal{I}_{E}(t) in any case.

(c)

Now we may show that this definition is well-defined. Let {sn}n=1∞\left\{ s_{n}\right\}_{n=1}^{\infty } and {tn}n=1∞\left\{ t_{n}\right\}_{n=1}^{\infty } denote two nondecreasing sequences in Sf\mathfrak {S}_{f} with lim⁡nsn=lim⁡ntn=f\lim_{n} s_{n}=\lim_{n} t_{n}=f. Show that lim⁡nIE(sn)=lim⁡nIE(tn)\lim_{n} \mathcal{I}_{E}\left(s_{n}\right)=\lim_{n} \mathcal{I}_{E}\left(t_{n}\right) by using the results of (a) and (b).

(d)

Finally, show that JˉE(f)=IˉE(f)\bar{\mathcal{J}}_{E}(f)=\bar{\mathcal{I}}_{E}(f), which shows that this definition is indeed truly equivalent to our definition. Observe that this alternative definition is defined to directly make MCT automatically true, so that MCT follows as a definition, but the price to be paid is in showing (a)-(c), that is, in showing that this alternative definition is well-defined.

Problem 6.2.11

Let (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) denote a measure space with E∈FE \in \mathcal{F} such that μ(E)<+∞\mu (E)<+\infty, and let f∈Nf \in \mathfrak {N}. Lebesgue's original version of our operator is

JˉE(f)=lim⁡n∑i=1n2ni−12nμ({ω∈E:i−12n⩽f(ω)<i2n}). \bar{\mathcal{J}}_{E}(f)=\lim _{n} \sum _{i=1}^{n 2^{n}} \frac{i-1}{2^{n}} \mu \left(\left\{ \omega \in E: \frac{i-1}{2^{n}} \leqslant f(\omega )<\frac{i}{2^{n}}\right\} \right) .
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(a)

The preceding limit exists, hence the preceding definition makes sense.

(b)

This definition is equivalent to our definition of IˉE(f)\bar{\mathcal{I}}_{E}(f). [Compare with (MF18) in Chapter 5.]

Problem 6.2.12

Let Ω\Omega denote a nonempty set, and let F\mathcal{F} denote a σ\sigma-field on Ω\Omega. For each n∈Nn \in \mathbb {N}, let μn\mu_{n} denote a measure with domain F\mathcal{F}. For each n∈Nn \in \mathbb {N}, let ∑i=1nμi\sum_{i=1}^{n} \mu_{i} denote the measure that assigns the value ∑i=1nμi(A)\sum_{i=1}^{n} \mu_{i}(A) to each A∈FA \in \mathcal{F}.

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(a)

Let s∈Ss \in \mathfrak {S} and n∈Nn \in \mathbb {N}. Then IEs(s;∑i=1nμi)=∑i=1nIEs(s;μi)\mathfrak {I}_{E}^{s}\left(s ; \sum_{i=1}^{n} \mu_{i}\right)=\sum_{i=1}^{n} \mathfrak {I}_{E}^{s}\left(s ; \mu_{i}\right).

(b)

Let f∈Nf \in \mathfrak {N} and n∈Nn \in \mathbb {N}. Then IEn(f;∑i=1nμi)=∑i=1nIEn(f;μi)\mathcal{I}_{E}^{n}\left(f ; \sum_{i=1}^{n} \mu_{i}\right)=\sum_{i=1}^{n} \mathcal{I}_{E}^{n}\left(f ; \mu_{i}\right).

Problem 6.2.13

Let A∈FA \in \mathcal{F} be nonempty, and suppose that f:A→[0,+∞]f: A \rightarrow [0,+\infty ] is F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable. Let E∈FAE \in \mathcal{F}_{A}, where FA\mathcal{F}_{A} is the set of F\mathcal{F}-subsets of AA. Consider two programs:

Program 1: Extend ff from AA to Ω\Omega as follows: let f∗∈Nf^{*} \in \mathfrak {N} be such that f∗=ff^{*}=f on AA and f∗=0f^{*}=0 on AcA^{c}.

Program 2: Do not extend ff from AA to Ω\Omega as in Program 1, but instead view ff as a function defined everywhere relative to the measure space (A,FA,μA)\left(A, \mathcal{F}_{A}, \mu_{A}\right), where μA\mu_{A} is the restriction of μ\mu from F\mathcal{F} to FA\mathcal{F}_{A}.

These two programs are equivalent in the sense that IˉE(f∗;μ)=JˉE(f;μA)\bar{\mathcal{I}}_{E}\left(f^{*} ; \mu \right)=\bar{\mathcal{J}}_{E}\left(f ; \mu_{A}\right), where IˉE\bar{\mathcal{I}}_{E} is this section's functional relative to the measure space (Ω,F,μ)(\Omega , \mathcal{F}, \mu ), and JˉE\bar{\mathcal{J}}_{E} is this section's functional relative to the measure space (A,FA,μA)\left(A, \mathcal{F}_{A}, \mu_{A}\right).

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Remark.
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Our definitions and results in the section exposition assumed that functions were everywhere defined on Ω\Omega, and such an approach may seem somewhat restrictive, since it may not be possible for some naturally occurring functions to be defined everywhere on Ω\Omega. This exercise (together with the following one) shows that such functions are not excluded from consideration nor left out of the scope of the results of this section, since we are justified in "switching our perspective" from (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) to an appropriate "sub-measure-space." Or, if we wish, we may equivalently just extend the domain of our function by defining it to be zero everywhere outside the original domain, and this extended function now has domain Ω\Omega and the theory relative to (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) applies. In either case, the corresponding functionals give the same numbers.

Problem 6.2.14

Keep ( Ω,F,μ\Omega , \mathcal{F}, \mu ) general. Suppose that F0⊆F\mathcal{F}_{0} \subseteq \mathcal{F} is a σ\sigma-field on Ω\Omega, and let μ0\mu_{0} denote the restriction of μ\mu to μ0\mu_{0}. If a nonnegative F/B∗\mathcal{F} / \mathcal{B}^{*} measurable function ff defined on Ω\Omega also happens to be F0/B∗\mathcal{F}_{0} / \mathcal{B}^{*}-measurable in addition, then IEn(f;μ)=IEn(f;μ0)\mathcal{I}_{E}^{n}(f ; \mu )=\mathcal{I}_{E}^{n}\left(f ; \mu_{0}\right) for every E∈F0E \in \mathcal{F}_{0}.

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Remark.
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(Ω,F0,μ0)(\Omega , \mathcal{F}_{0}, \mu_{0}) is clearly a measure space.

Problem 6.2.15

(N16): Suppose that (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) is a σ\sigma-finite measure space, and further suppose that IˉE(f)=IˉE(g)\bar{\mathcal{I}}_{E}(f)=\bar{\mathcal{I}}_{E}(g) for every E∈FE \in \mathcal{F}. Then f=gf=g μ\mu-a.e. on Ω\Omega.

We have the following claims related to (N16):

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(a)

If Iˉ(f)\bar{\mathcal{I}}(f) and Iˉ(g)\bar{\mathcal{I}}(g) are finite, and if IˉE(f)=IˉE(g)\bar{\mathcal{I}}_{E}(f)=\bar{\mathcal{I}}_{E}(g) for every E∈FE \in \mathcal{F}, then f=gf=g μ\mu-a.e. on Ω\Omega. [Observe that here we don't need σ\sigma-finiteness because of the assumed finiteness. A simple proof is this: if IˉE(f)⩽IˉE(g)\bar{\mathcal{I}}_{E}(f) \leqslant \bar{\mathcal{I}}_{E}(g) for each E∈FE \in \mathcal{F}, then Iˉ(  1A(f−g))=0\bar{\mathcal{I}}\left(\; \mathbb {1}_{A}(f-g)\right)=0, where A={ω∈Ω:g(ω)<f(ω)}A=\left\{ \omega \in \Omega : g(\omega )<f(\omega )\right\}. Conclude that μ(A)=0\mu (A)=0. Reverse the roles of ff and gg for the result.]

(b)

Suppose that P\mathcal{P} is a π\pi-system that generates F\mathcal{F}: σ(P)=F\sigma (\mathcal{P})=\mathcal{F}. If Iˉ(f)\bar{\mathcal{I}}(f) and Iˉ(g)\bar{\mathcal{I}}(g) are finite, and if IˉE(f)=IˉE(g)\bar{\mathcal{I}}_{E}(f)=\bar{\mathcal{I}}_{E}(g) for every E∈PE \in \mathcal{P}, then f=gf=g μ\mu-a.e. on Ω\Omega.

Problem 6.2.16

Let ff denote a nonnegative F′/B∗\mathcal{F}^{\prime } / \mathcal{B}^{*}-measurable function. We have the two equalities

In(f∘T;μ)=In(f;μ∘T−1)(6.9) \mathcal{I}^{n}(f \circ T ; \mu )=\mathcal{I}^{n}\left(f ; \mu \circ T^{-1}\right) \tag {6.9}

and

LT−1(A′)n(f∘T;μ)=IA′n(f;μ∘T−1)∀A′∈F′(6.10) \mathcal{L}_{T^{-1}\left(A^{\prime }\right)}^{n}(f \circ T ; \mu )=\mathcal{I}_{A^{\prime }}^{n}\left(f ; \mu \circ T^{-1}\right) \quad \forall A^{\prime } \in \mathcal{F}^{\prime } \tag {6.10}
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Problem 6.3.1

Let E∈FE \in \mathcal{F} be such that μ(E)<∞\mu (E)<\infty, and let f∈Mf \in \mathfrak {M} be such that f=0f=0 on EcE^{c} and m⩽f⩽Mm \leqslant f \leqslant M on EE, where m,M∈Rm, M \in \mathbb {R}. Then Ig(f)\mathcal{I}^{g}(f) exists and is finite. Furthermore, we have mμ(E)⩽Ig(f)⩽Mμ(E)m \mu (E) \leqslant \mathcal{I}^{g}(f) \leqslant M \mu (E).

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Problem 6.3.2

Let E∈F,ε>0E \in \mathscr {F}, \varepsilon >0 and let f∈Mf \in \mathfrak {M} be such that IEg(f)\mathcal{I}_{E}^{g}(f) exists and is finite. There exists a subset F⊆EF \subseteq E such that μ(F)<∞\mu (F)<\infty and ∣IEg(f)−IFg(f)∣<ε\left|\mathcal{I}_{E}^{g}(f)-\mathcal{I}_{F}^{g}(f)\right|<\varepsilon.

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Problem 6.3.3

ff is such that IEg(f)\mathcal{I}_{E}^{g}(f) exists and is finite iff for any ε>0\varepsilon >0 there are functions gg and hh in M\mathfrak {M} such that h⩽f⩽gh \leqslant f \leqslant g on EE and IEg(g−h)<ε\mathcal{I}_{E}^{g}(g-h)<\varepsilon.

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Problem 6.3.4

Let f,f1,f2,…f, f_{1}, f_{2}, \ldots denote a sequence of nonnegative functions in M\mathfrak {M}. For each n∈Nn \in \mathbb {N} and E∈FE \in \mathcal{F}, define vn(E)=IEg(fn;μ)v_{n}(E)=\mathcal{I}_{E}^{g}\left(f_{n} ; \mu \right) and v(E)=IEg(f;μ)v(E)=\mathcal{I}_{E}^{g}(f ; \mu ). Furthermore, assume that v(Ω),v1(Ω),v2(Ω),…v(\Omega ), v_{1}(\Omega ), v_{2}(\Omega ), \ldots are finite and fn→fμf_{n} \rightarrow f \mu-a.e. on Ω\Omega. Then

sup⁡{∣v(E)−vn(E)∣:E∈F}⩽Ig(∣fn−f∣;μ)→0 as n→∞. \sup \left\{ \left|v(E)-v_{n}(E)\right|: E \in \mathbb {F}\right\} \leqslant \mathcal{I}^{g}\left(\left|f_{n}-f\right| ; \mu \right) \rightarrow 0 \text{ as } n \rightarrow \infty .
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Problem 6.3.5

Let (Ω,F,μ)=(Rk,Bk,λk)(\Omega , \mathcal{F}, \mu )=\left(\mathbb {R}^{k}, \mathscr {B}^{k}, \lambda_{k}\right) with E∈FE \in \mathcal{F}, and let f∈Mf \in \mathfrak {M} be such that Ig(f)\mathcal{I}^{g}(f) exists and is finite.

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(a)

Suppose that {fn}\left\{ f_{n}\right\} is a sequence of functions in M\mathfrak {M} such that

fn(x)={f(x) if x is such that ∣f(x)∣⩽n and ∥x∥⩽n0 otherwise  f_{n}(\boldsymbol {x})= \begin{cases} f(\boldsymbol {x}) & \text{ if } \boldsymbol {x} \text{ is such that }\left|f(\boldsymbol {x})\right| \leqslant n \text{ and }\left\| \boldsymbol {x}\right\| \leqslant n \\ 0 & \text{ otherwise }\end{cases}

Then lim⁡nIEg(fn)\lim_{n} \mathcal{I}_{E}^{g}\left(f_{n}\right) exists and equals IEg(lim⁡nfn)\mathcal{I}_{E}^{g}\left(\lim_{n} f_{n}\right).

(b)

Reset everything in (a), and this time let fn(x)=f(x)exp⁡(−∥x∥2/n)f_{n}(\boldsymbol {x})=f(\boldsymbol {x}) \exp \left(-\left\| \boldsymbol {x}\right\|^{2} / n\right) for each x∈Rk\boldsymbol {x} \in \mathbb {R}^{k} and n∈Nn \in \mathbb {N}. Then lim⁡nIEg(fn)=IEg(f)\lim_{n} \mathcal{I}_{E}^{g}\left(f_{n}\right)=\mathcal{I}_{E}^{g}(f).

Problem 6.3.6

Suppose that μ(Ω)<∞,{fn}\mu (\Omega )<\infty ,\left\{ f_{n}\right\} is a sequence of functions in M\mathfrak {M} such that there exists M∈RM \in \mathbb {R} with ∣fn∣≤M\left|f_{n}\right| \leq M for each n∈Nn \in \mathbb {N}, and let f∈Mf \in \mathfrak {M} be such that fn→ff_{n} \rightarrow f uniformly on EE. Then lim⁡nIEg(fn)=IEg(f)\lim_{n} \mathcal{I}_{E}^{g}\left(f_{n}\right)=\mathcal{I}_{E}^{g}(f).

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Problem 6.3.7

Let {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } denote a nondecreasing sequence of functions in M\mathfrak {M} such that IEg(fn)\mathcal{I}_{E}^{g}\left(f_{n}\right) exists and is finite for each n∈Nn \in \mathbb {N} and sup⁡n∈NIEg(fn)<∞\sup_{n \in \mathbb {N}} \mathcal{I}_{E}^{g}\left(f_{n}\right)<\infty. Then IEg(lim⁡nfn)\mathcal{I}_{E}^{g}\left(\lim_{n} f_{n}\right) exists, is finite, and equals lim⁡nIEg(fn)\lim_{n} \mathcal{I}_{E}^{g}\left(f_{n}\right). This is one form of Beppo Levi's Theorem.

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Problem 6.3.8

Let {fn},{gn}\left\{ f_{n}\right\} ,\left\{ g_{n}\right\}, and {hn}\left\{ h_{n}\right\} denote sequences of functions in M\mathfrak {M} such that fn→ a.e. f,gn→ a.e. gf_{n} \xrightarrow {\text{ a.e. }} f, g_{n} \xrightarrow {\text{ a.e. }} g, and hn→ a.e. hh_{n} \xrightarrow {\text{ a.e. }} h for some functions f,g,h∈Mf, g, h \in \mathfrak {M}.

Suppose for any p∈{g,g1,g2,…,h,h1,h2,…}p \in \left\{ g, g_{1}, g_{2}, \ldots , h, h_{1}, h_{2}, \ldots \right\} that IEg(p)\mathcal{I}_{E}^{g}(p) exists and is finite. Furthermore, suppose that lim⁡nIEg(gn)=IEg(g)\lim_{n} \mathcal{I}_{E}^{g}\left(g_{n}\right)=\mathcal{I}_{E}^{g}(g) and lim⁡nIEg(hn)=IEg(h)\lim_{n} \mathcal{I}_{E}^{g}\left(h_{n}\right)=\mathcal{I}_{E}^{g}(h). Also, assume that gn⩽fn⩽hng_{n} \leqslant f_{n} \leqslant h_{n} for every n∈Nn \in \mathbb {N}.

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(a)

IEg(fn)\mathcal{I}_{E}^{g}\left(f_{n}\right) exists and is finite for all n∈N,IEg(f)n \in \mathbb {N}, \mathcal{I}_{E}^{g}(f) exists and is finite, and lim⁡nIEg(fn)=IEg(f)\lim_{n} \mathcal{I}_{E}^{g}\left(f_{n}\right)=\mathcal{I}_{E}^{g}(f).

(b)

DCT may be obtained from (a).

Problem 6.3.9

In properties (G6) and (G9), we gave a proof for the "everywhere" case. Prove the "almost everywhere" case for these two properties. [No problems should arise.]

(G6): if f⩽gf \leqslant g μ\mu-a.e. on EE and f,g∈M(E)f, g \in \mathfrak {M}(E), then I‾‾E(f)⩽I‾‾E(g)\overline{\overline{\mathcal{I}}}_{E}(f) \leqslant \overline{\overline{\mathcal{I}}}_{E}(g).

(G9): if I‾‾E(f)\overline{\overline{\mathcal{I}}}_{E}(f) eaif and gg is such that ∣g∣⩽f\left|g\right| \leqslant f μ\mu-a.e. on EE, then I‾‾E(g)\overline{\overline{\mathcal{I}}}_{E}(g) eaif. As a consequence, any f∈Mf \in \mathfrak {M} that is bounded μ\mu-a.e. on a set EE of finite measure and zero μ\mu-a.e. on EcE^{c} is such that I‾‾F(f)\overline{\overline{\mathcal{I}}}_{F}(f) eaif for every F∈FF \in \mathcal{F}.

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Problem 6.3.10

Suppose that for each t∈Rt \in \mathbb {R} we have ft∈Mf_{t} \in \mathfrak {M}, and suppose that lim⁡t→+∞ft(ω)\lim_{t \rightarrow +\infty } f_{t}(\omega ) exists for each ω∈Ω\omega \in \Omega. Next, assume that there exists nonnegative g∈Mg \in \mathfrak {M} such that IˉE(g)\bar{\mathcal{I}}_{E}(g) exists and is finite; further assume that ∣ft∣⩽g\left|f_{t}\right| \leqslant g for each t∈Rt \in \mathbb {R}.

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(a)

IˉE(ft)\bar{\mathcal{I}}_{E}\left(f_{t}\right) exists and is finite.

(b)

IˉE(lim⁡t→+∞ft)\bar{\mathcal{I}}_{E}\left(\lim_{t \rightarrow +\infty } f_{t}\right) exists and is finite. [Show first that lim⁡t→+∞ft∈M\lim_{t \rightarrow +\infty } f_{t} \in \mathfrak {M}.]

(c)

lim⁡t→+∞IˉE(ft)\lim_{t \rightarrow +\infty } \bar{\mathcal{I}}_{E}\left(f_{t}\right) exists and is finite.

(d)

lim⁡t→+∞IˉE(ft)=IˉE(lim⁡t→+∞ft)\lim_{t \rightarrow +\infty } \bar{\mathcal{I}}_{E}\left(f_{t}\right)=\bar{\mathcal{I}}_{E}\left(\lim_{t \rightarrow +\infty } f_{t}\right). [This is a more general form of DCT.]

(e)

Suppose that instead of tt ranging over R\mathbb {R}, we have tt ranging over some interval (a,b)(a, b), where −∞⩽a<b⩽+∞-\infty \leqslant a<b \leqslant +\infty, and suppose that limits are now as t→at \rightarrow a from the right [or t→bt \rightarrow b from the left]. Then (a)-(d) hold in these two modified scenarios.

Problem 6.3.11

Suppose that {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is a sequence of functions in M\mathfrak {M} such that lim⁡nfn\lim_{n} f_{n} exists on Ω\Omega. Next, suppose that {gn}n=1∞\left\{ g_{n}\right\}_{n=1}^{\infty } is a sequence of nonnegative functions in M\mathfrak {M} such that for all n∈Nn \in \mathbb {N} we have (i) IˉE(gn)\bar{\mathcal{I}}_{E}\left(g_{n}\right) exists and is finite and (ii) ∣fn∣⩽gn\left|f_{n}\right| \leqslant g_{n}. Finally, suppose that (iii) lim⁡ngn\lim_{n} g_{n} exists on Ω\Omega, (iv) IˉE(lim⁡ngn)\bar{\mathcal{I}}_{E}\left(\lim_{n} g_{n}\right) exists and is finite, and (v) IˉE(lim⁡ngn)=lim⁡nIˉE(gn)\bar{\mathcal{I}}_{E}\left(\lim_{n} g_{n}\right)=\lim_{n} \bar{\mathcal{I}}_{E}\left(g_{n}\right). Then IˉE(lim⁡nfn)=lim⁡nIˉE(fn)\bar{\mathcal{I}}_{E}\left(\lim_{n} f_{n}\right)=\lim_{n} \bar{\mathcal{I}}_{E}\left(f_{n}\right).

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Remark.
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This is yet another more general form of DCT. As with the previous problem, remember to show that all quantities in fact exist and make sense before showing that they're equal.

Problem 6.3.12

Suppose that I∪n=1∞Eng(f)\mathcal{I}_{\cup_{n=1}^{\infty } E_{n}}^{g}(f) exists and is finite, where {En}n=1∞\left\{ E_{n}\right\}_{n=1}^{\infty } is a disjoint sequence of F\mathcal{F}-sets. Then I∪n=1gEn∞(f)=∑n=1∞IEng(f)\mathcal{I}_{\cup_{n=1}^{g} E_{n}}^{\infty }(f)=\sum_{n=1}^{\infty } \mathcal{I}_{E_{n}}^{g}(f), and the convergence of the series is absolute.

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Problem 6.3.13

Assume for each n∈Nn \in \mathbb {N} that (i) Iˉ(fn)\bar{\mathcal{I}}\left(f_{n}\right) exists and is finite and (ii) fnf_{n} is finite. Assume also that ∑n=1∞Iˉ(fn)<+∞\sum_{n=1}^{\infty } \bar{\mathcal{I}}\left(f_{n}\right)<+\infty.

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(a)

For μ\mu-a.e. ω∈Ω\omega \in \Omega, ∑n=1∞fn(ω)\sum_{n=1}^{\infty } f_{n}(\omega ) exists.

(b)

Define gg on Ω\Omega by writing

g(ω)={∑n=1∞fn(ω)if ∑n=1∞fn(ω) exists0otherwise g(\omega )= \begin{cases} \sum _{n=1}^{\infty } f_{n}(\omega ) & \text{if } \sum _{n=1}^{\infty } f_{n}(\omega ) \text{ exists} \\ 0 & \text{otherwise} \end{cases}

Then Iˉ(g)=∑n=1∞Iˉ(fn)\bar{\mathcal{I}}(g)=\sum_{n=1}^{\infty } \bar{\mathcal{I}}\left(f_{n}\right).

(c)

The assumption that each fnf_{n} is finite may be relaxed to saying that each fnf_{n} is finite μ\mu-a.e. on Ω\Omega.

Problem 6.3.14

Suppose that {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is a sequence of elements of N\mathfrak {N} converging to some f∈Nf \in \mathfrak {N}. Furthermore, assume that there is 0⩽M<∞0 \leqslant M<\infty such that Ig(fn)⩽M\mathcal{I}^{g}\left(f_{n}\right) \leqslant M for each n∈Nn \in \mathbb {N}. Then Ig(f)\mathcal{I}^{g}(f) exists, is finite, and is no more than MM.

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Problem 6.4.1

(L10) If f∈L1(E)f \in L^{1}(E) and ∣g∣⩽fμ\left|g\right| \leqslant f \mu-a. e. on EE, then g∈L1(E)g \in L^{1}(E). Also, any ff that is bounded μ\mu-a. e. on a set EE with μ(E)<∞\mu (E)<\infty and is zero μ−\mu - a. e. on EcE^{c} is in L1(E)L^{1}(E). (L16) We have the following, where A′∈F′A^{\prime } \in \mathcal{F}^{\prime } :

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(a)

If φ⩾0\varphi \geqslant 0, then ∫f−1(A′)φ∘f dμ=∫A′φd(μ∘f−1)\int_{f^{-1}\left(A^{\prime }\right)} \varphi \circ f \mathrm{~ d} \mu =\int_{A^{\prime }} \varphi \mathrm{d}\left(\mu \circ f^{-1}\right).

(b)

For general φ,∫f−1(A′)φ∘f dμ\varphi , \int_{f^{-1}\left(A^{\prime }\right)} \varphi \circ f \mathrm{~ d} \mu exists and is finite iff ∫A′φd(μ∘f−1)\int_{A^{\prime }} \varphi \mathrm{d}\left(\mu \circ f^{-1}\right) exists and is finite, and in this case equality obtains.

Problem 6.4.2

Suppose that ∑n=1∞fn\sum_{n=1}^{\infty } f_{n} converges μ\mu-a.e. on Ω\Omega and that for every n∈Nn \in \mathbb {N} we have ∣∑k=1nfk∣⩽g\left|\sum_{k=1}^{n} f_{k}\right| \leqslant g μ\mu-a.e. on Ω\Omega, where g∈L1(Ω)g \in L^{1}(\Omega ).

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(a)

For every n∈Nn \in \mathbb {N} we have fn∈L1(Ω)f_{n} \in L^{1}(\Omega ), and ∑n=1∞fn∈L1(Ω)\sum_{n=1}^{\infty } f_{n} \in L^{1}(\Omega ) as well.

(b)

The equality ∫∑n=1∞fn=∑n=1∞∫fn\int \sum_{n=1}^{\infty } f_{n}=\sum_{n=1}^{\infty } \int f_{n} obtains.

(c)

Prove the following corollary: if ∑n=1∞∫∣fn∣\sum_{n=1}^{\infty } \int \left|f_{n}\right| converges, then ∑n=1∞fn\sum_{n=1}^{\infty } f_{n} converges absolutely μ\mu-a.e. on Ω\Omega and again the equality ∫∑n=1∞fn=∑n=1∞∫fn\int \sum_{n=1}^{\infty } f_{n}=\sum_{n=1}^{\infty } \int f_{n} holds.

Problem 6.4.3

Suppose that f∈L1(Ω)f \in L^{1}(\Omega ).

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(a)

Let An={ω∈Ω:∣f(ω)∣⩾n}A_{n}=\left\{ \omega \in \Omega : \left|f(\omega )\right| \geqslant n\right\}. Then lim⁡n∣fn(ω)∣  1An(ω)=0\lim_{n}\left|f_{n}(\omega )\right| \; \mathbb {1}_{A_{n}}(\omega )=0 for μ\mu-a.e. ω∈Ω\omega \in \Omega.

(b)

Use DCT to show that lim⁡n∫An∣f∣=0\lim_{n} \int_{A_{n}}\left|f\right|=0.

Problem 6.4.4

This exercise deals with the concept of uniform integrability. A sequence {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is called uniformly integrable iff lim⁡msup⁡n∫Am∣fn∣=0\lim_{m} \sup_{n} \int_{A_{m}}\left|f_{n}\right|=0, where the sets A1,A2,…A_{1}, A_{2}, \ldots are as given in the previous exercise: An={ω∈Ω:∣f(ω)∣⩾n}A_{n}=\left\{ \omega \in \Omega : \left|f(\omega )\right| \geqslant n\right\} for f∈L1(Ω)f \in L^{1}(\Omega ).

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(a)

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty and {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is uniformly integrable. Then each fnf_{n} is in L1(Ω)L^{1}(\Omega ).

(b)

If {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } and {gn}n=1∞\left\{ g_{n}\right\}_{n=1}^{\infty } are uniformly integrable, then so is {fn+gn}n=1∞\left\{ f_{n}+g_{n}\right\}_{n=1}^{\infty }.

(c)

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty, fn→ff_{n} \rightarrow f μ\mu-a.e. on Ω\Omega, and {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is uniformly integrable. Then f∈L1(Ω)f \in L^{1}(\Omega ) and lim⁡∫fn=∫f\lim \int f_{n}=\int f.

(d)

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty and that fn→ff_{n} \rightarrow f μ\mu-a.e. on Ω\Omega, where each of f,f1,f2,…f, f_{1}, f_{2}, \ldots is nonnegative and in L1(Ω)L^{1}(\Omega ). If lim⁡∫fn=∫f\lim \int f_{n}=\int f, then {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is uniformly integrable.

(e)

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty, f,f1,f2,…∈L1(Ω)f, f_{1}, f_{2}, \ldots \in L^{1}(\Omega ), and fn→ff_{n} \rightarrow f μ\mu-a.e. on Ω\Omega. Then the following statements are logically equivalent:

  1. {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is uniformly integrable.

  2. lim⁡∫∣fn−f∣=0\lim \int \left|f_{n}-f\right|=0.

  3. lim⁡∫∣fn∣→∫∣f∣\lim \int \left|f_{n}\right| \rightarrow \int \left|f\right|.

(f)

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty. Then {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is uniformly integrable iff (i) ∫∣fn∣\int \left|f_{n}\right| is bounded and (ii) for every ε>0\varepsilon >0 there is δ>0\delta >0 such that μ(E)<δ\mu (E)<\delta implies ∫E∣fn∣<ε\int_{E}\left|f_{n}\right|<\varepsilon for every n∈Nn \in \mathbb {N}.

Remark.
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The reader may consult Billingsley's Probability and Measure, Section 16, for the solutions to (a)-(e).

Problem 6.4.5

This problem deals with parametric integrals. Here, we consider a measure space (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) as well as a nondegenerate interval Θ⊆R\Theta \subseteq \mathbb {R} of any form. Suppose that for every θ∈Θ\theta \in \Theta there is a function fθf_{\theta } in L1(Ω,F,μ)L^{1}(\Omega , \mathcal{F}, \mu ) with domain Ω\Omega. That is, for every θ∈Θ\theta \in \Theta we may consider the real number ∫Ωfθ(ω) dμ(ω)\int_{\Omega } f_{\theta }(\omega ) \, d\mu (\omega ). For each θ∈Θ\theta \in \Theta, write F(θ)F(\theta ) for ∫Ωfθ(ω) dμ(ω)\int_{\Omega } f_{\theta }(\omega ) \, d\mu (\omega ). Hold this notation and these assumptions fixed throughout.

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(a)

Make the following additional assumptions:

  1. There exists g∈L1(Ω,F,μ)g \in L^{1}(\Omega , \mathcal{F}, \mu ) with domain Ω\Omega such that ∣fθ(ω)∣⩽g(ω)\left|f_{\theta }(\omega )\right| \leqslant g(\omega ) for every ω∈Ω\omega \in \Omega and θ∈Θ\theta \in \Theta.

  2. The element θ0∈Θ\theta_{0} \in \Theta is such that lim⁡θ→θ0fθ(ω)=fθ0(ω)\lim_{\theta \rightarrow \theta_{0}} f_{\theta }(\omega )=f_{\theta_{0}}(\omega ) for μ\mu-a.e. ω∈Ω\omega \in \Omega. Show that lim⁡θ→θ0F(θ)=F(θ0)\lim_{\theta \rightarrow \theta_{0}} F(\theta )=F\left(\theta_{0}\right), so that FF is continuous at θ0\theta_{0}.

(b)

Forget about the assumptions from (a), and instead make the following new set of assumptions:

  1. For μ\mu-a.e. ω∈Ω\omega \in \Omega we have that fθ(ω)f_{\theta }(\omega ) is differentiable at each θ∈Θ\theta \in \Theta.

  2. There exists g∈L1(Ω,F,μ)g \in L^{1}(\Omega , \mathcal{F}, \mu ) with domain Ω\Omega such that ∣∂∂θfθ(ω)∣⩽g(ω)\left|\frac{\partial }{\partial \theta } f_{\theta }(\omega )\right| \leqslant g(\omega ) for μ\mu-a.e. ω∈Ω\omega \in \Omega and all θ∈Θ\theta \in \Theta. Show that (i) FF is differentiable on Θ\Theta, and (ii) ∂∂θF(θ)=∫Ω∂∂θfθ(ω) dμ(ω)\frac{\partial }{\partial \theta } F(\theta )=\int_{\Omega } \frac{\partial }{\partial \theta } f_{\theta }(\omega ) \, d\mu (\omega ).

Problem 6.4.6

Assume that ff is an F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable function defined μ\mu-a.e. on Ω\Omega such that there are real numbers mm and MM with m⩽f⩽Mm \leqslant f \leqslant M μ\mu-a.e. on Ω\Omega. Also, assume that g∈L1(Ω,F,μ)g \in L^{1}(\Omega , \mathcal{F}, \mu ). Then there is α∈[m,M]\alpha \in [m, M] such that ∫f∣g∣=α∫∣g∣\int f\left|g\right|=\alpha \int \left|g\right|.

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Problem 6.4.7

Let {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } denote a sequence in N\mathfrak {N} with f1⩾f2⩾⋯⩾0f_{1} \geqslant f_{2} \geqslant \cdots \geqslant 0, fn→ff_{n} \rightarrow f on Ω\Omega, and f1∈L1(Ω,F,μ)f_{1} \in L^{1}(\Omega , \mathcal{F}, \mu ). Then lim⁡n∫fn=∫f\lim_{n} \int f_{n}=\int f, and the requirement that f1∈L1(Ω,F,μ)f_{1} \in L^{1}(\Omega , \mathcal{F}, \mu ) is essential. [This mimics MCT somewhat.]

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Problem 6.4.8

Suppose that μ(Ω)<+∞\mu (\Omega )<+\infty, and let {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } denote a uniformly bounded sequence of functions on Ω\Omega with fn→ff_{n} \rightarrow f uniformly on Ω\Omega. Then lim⁡n∫fn=∫f\lim_{n} \int f_{n}=\int f.

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Problem 6.4.9

Suppose that {fn}n=1∞\left\{ f_{n}\right\}_{n=1}^{\infty } is a sequence of functions in L1(Ω,F,μ)L^{1}(\Omega , \mathcal{F}, \mu ) such that the series ∑n=1∞∫∣fn∣\sum_{n=1}^{\infty } \int \left|f_{n}\right| converges. Then ∑n=1∞fn\sum_{n=1}^{\infty } f_{n} converges μ\mu-a.e. on Ω\Omega to a function f∈L1(Ω,F,μ)f \in L^{1}(\Omega , \mathcal{F}, \mu ) and ∫f=∑n=1∞∫fn\int f=\sum_{n=1}^{\infty } \int f_{n}.

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Problem 6.4.10

Let (Ω,F,μ)(\Omega , \mathcal{F}, \mu ) denote a generic measure space, and let (Ω,Fˉ,μˉ)(\Omega , \bar{\mathcal{F}}, \bar{\mu }) denote the completion of (Ω,F,μ)(\Omega , \mathcal{F}, \mu ). Let fˉ\bar{f} denote an Fˉ/B∗\bar{\mathcal{F}}/\mathcal{B}^{*}-measurable function on Ω\Omega. [The bar on ff is just part of the notation; it denotes no operation.]

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(a)

There exists ff on Ω\Omega that is F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable with f=fˉf=\bar{f} μˉ\bar{\mu }-a.e. [Here, look back at the outline of Exercise 2 in Section 5.5, where there F\mathcal{F} consisted of the Borel sets and Fˉ\bar{\mathcal{F}} consisted of the Lebesgue sets. Observe that nothing specific to Euclidean space was used in that outline --- only the general results concerning completion --- hence the same outline will work here.]

(b)

If one of ∫fˉ dμˉ\int \bar{f} \, d\bar{\mu } and ∫f dμ\int f \, d\mu exists, then so does the other and both integrals coincide. Therefore, integrals of Fˉ/B∗\bar{\mathcal{F}}/\mathcal{B}^{*}-measurable functions with respect to μˉ\bar{\mu } are completely determined by the integrals of F/B∗\mathcal{F}/\mathcal{B}^{*}-measurable functions with respect to μ\mu. [It is perhaps best to use the usual approach in proving results about integrals: show that the claim holds for simple, then nonnegative, then measurable functions.]