Section 3.5

Uniqueness of Measures and Extensions

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Problem 3.5.1

If μ1\mu_{1} and μ2\mu_{2} are finite measures with domain σ(P)\sigma (\mathcal{P}) (where P\mathcal{P} denotes a π\pi-system on Ω\Omega ), if Ω\Omega can be expressed as an amc union of P\mathscr {P}-sets, and if μ1=μ2\mu_{1}=\mu_{2} on P\mathscr {P}, then μ1=μ2\mu_{1}=\mu_{2} on σ(P)\sigma (\mathscr {P}).

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Problem 3.5.2

Let μ1\mu_{1} and μ2\mu_{2} denote finite measures with domain σ(P)\sigma (\mathcal{P}), where P\mathcal{P} is a π\pi-system on Ω\Omega, and further suppose that μ1=μ2\mu_{1}=\mu_{2} on P\mathcal{P}. Then μ1=μ2\mu_{1}=\mu_{2}.

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Problem 3.5.3

Let Ω={ω1,ω2,ω3,ω4}\Omega =\left\{ \omega_{1}, \omega_{2}, \omega_{3}, \omega_{4}\right\}, let A\mathcal{A} consist of ∅,{ω1,ω2}\varnothing ,\left\{ \omega_{1}, \omega_{2}\right\}, {ω1,ω3},{ω2,ω4},{ω3,ω4}\left\{ \omega_{1}, \omega_{3}\right\} ,\left\{ \omega_{2}, \omega_{4}\right\} ,\left\{ \omega_{3}, \omega_{4}\right\}, and Ω\Omega, and let μ:A→R\mu : \mathcal{A} \rightarrow \mathbb {R} be defined as follows: μ(Ω)=6,μ(∅)=0\mu (\Omega )=6, \mu (\varnothing )=0, and μ({ω1,ω2})=μ({ω1,ω3})=μ({ω2,ω4})=μ({ω3,ω4})=\mu \left(\left\{ \omega_{1}, \omega_{2}\right\} \right)=\mu \left(\left\{ \omega_{1}, \omega_{3}\right\} \right)=\mu \left(\left\{ \omega_{2}, \omega_{4}\right\} \right)=\mu \left(\left\{ \omega_{3}, \omega_{4}\right\} \right)= 3.

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(a)

A\mathcal{A} is neither a π\pi-system nor a semiring, and σ(A)=2Ω\sigma (\mathcal{A})=2^{\Omega }.

(b)

μ\mu is a measure.

(c)

Define two new distinct measures vv and ξ\xi on the σ\sigma-field 2Ω2^{\Omega } by the following: v({ω1})=v({ω4})=1,v({ω2})=v({ω3})=2,ξ({ω2})=ξ({ω3})=1v\left(\left\{ \omega_{1}\right\} \right)=v\left(\left\{ \omega_{4}\right\} \right)=1, v\left(\left\{ \omega_{2}\right\} \right)=v\left(\left\{ \omega_{3}\right\} \right)=2, \xi \left(\left\{ \omega_{2}\right\} \right)=\xi \left(\left\{ \omega_{3}\right\} \right)=1, and ξ({ω1})=ξ({ω4})=2\xi \left(\left\{ \omega_{1}\right\} \right)=\xi \left(\left\{ \omega_{4}\right\} \right)=2. Then vv and ξ\xi are distinct measure extensions of μ\mu from A\mathcal{A} to σ(A)=2Ω\sigma (\mathcal{A})=2^{\Omega }.

(d)

Let μ∗:2Ω→R\mu^{*}: 2^{\Omega } \rightarrow \mathbb {R} denote the outer measure induced by μ\mu. Then μ∗=μ\mu^{*}=\mu on A\mathcal{A} and μ∗\mu^{*} is a measure.

(e)

μ∗,v\mu^{*}, v, and ξ\xi are distinct measures.

Problem 3.5.4

Let Ω=Q\Omega =\mathbb {Q}, and let A\mathcal{A} consist of the sets {ω∈Q:a<ω⩽b}\left\{ \omega \in \mathbb {Q}: a<\omega \leqslant b\right\}, where a<ba<b and a,b∈Qa, b \in \mathbb {Q}. Also, let ∅∈A\varnothing \in \mathcal{A}.

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(a)

A\mathcal{A} is a semiring and σ(A)=2Ω\sigma (\mathcal{A})=2^{\Omega }.

(b)

Define μ:A→R‾\mu : \mathcal{A} \rightarrow \overline{\mathbb {R}} by stipulating that μ(A)\mu (A) equals the number of points in AA if AA is finite and μ(A)=+∞\mu (A)=+\infty if AA is infinite. Then μ(A)=+∞\mu (A)=+\infty for all A∈A−{∅}A \in \mathcal{A}-\left\{ \varnothing \right\}, hence μ\mu fails to be σ\sigma-finite on A\mathcal{A}.

(c)

Define v:2Ω→R‾v: 2^{\Omega } \rightarrow \overline{\mathbb {R}} by stating that v(A)v(A) equals the number of points in AA if AA is finite and v(A)=+∞v(A)=+\infty if AA is infinite. Next, define ξ\xi by writing ξ(A)=2v(A)\xi (A)=2 v(A) for all A⊆ΩA \subseteq \Omega. Then vv and ξ\xi are distinct σ\sigma-finite measure extensions of μ\mu from A\mathcal{A} to σ(A)\sigma (\mathcal{A}). Therefore, when μ\mu fails to be σ\sigma-finite on A\mathcal{A}, there may be more than one measure extension of μ\mu from A\mathcal{A} to σ(A)\sigma (\mathcal{A}).

(d)

The outer measure μ∗:2Ω→R‾\mu^{*}: 2^{\Omega } \rightarrow \overline{\mathbb {R}} induced by μ\mu is such that μ∗(A)=+∞\mu^{*}(A)=+\infty for any nonempty A⊆ΩA \subseteq \Omega, and μ∗\mu^{*} is a non-σ\sigma-finite measure. Therefore, while we have two distinct σ\sigma-finite measure extensions of μ\mu to σ(A)\sigma (\mathcal{A}), we also have a non-σ\sigma-finite extension of μ\mu to σ(A)\sigma (\mathcal{A}) as well.

(e)

M(μ∗)=2Ω=σ(A)\mathcal{M}\left(\mu^{*}\right)=2^{\Omega }=\sigma (\mathcal{A}).

Problem 3.5.5

We assume the setup of Exercise 3.4.6. The aim of this exercise is to show that if vv is a measure with domain σ(F)\sigma (\mathcal{F}) such that v=μv=\mu on the field F\mathcal{F}, then ν\nu coincides with the measure extension of μ\mu to σ(F)\sigma (\mathcal{F}) guaranteed by Exercise 3.4.6.

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(a)

If B∈σ(F)B \in \sigma (\mathcal{F}), then ν(B)⩽μ∗(B)\nu (B) \leqslant \mu^{*}(B).

(b)

If F∈σ(F)F \in \sigma (\mathcal{F}) and μ∗(F)<+∞\mu^{*}(F)<+\infty, then ν(F)=μ∗(F)\nu (F)=\mu^{*}(F).

(c)

If μ\mu is σ\sigma-finite on F\mathcal{F}, then ν(E)=μ∗(E)\nu (E)=\mu^{*}(E) for all E∈σ(F)E \in \sigma (\mathcal{F}). This gives the uniqueness of the measure extension whose existence is guaranteed by Exercise 3.4.6.

Problem 3.5.6

A lattice on Ω\Omega is a collection L⊆2Ω\mathscr {L} \subseteq 2^{\Omega } such that (i) Ω∈L\Omega \in \mathscr {L}, (ii) ∅∈L\varnothing \in \mathscr {L}, (iii) L\mathscr {L} is closed under (finite) unions, and (iv) L\mathscr {L} is a π\pi-system. We also define the following two collections: D={B\A:A,B∈L,A⊆B}D=\left\{ B \backslash A: A, B \in \mathscr {L}, A \subseteq B\right\}, and U\mathcal{U} will denote the collection of all finite disjoint unions of D\mathfrak {D}-sets.

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(a)

D\mathscr {D} is a π\pi-system.

(b)

U is a π\pi-system.

(c)

UU is closed under complementation.

(d)

UU coincides with the minimal field containing the lattice L\mathscr {L}.

(e)

Let A\mathcal{A} denote a σ\sigma-field on Ω\Omega that contains L\mathscr {L}. Suppose that μ\mu and vv are measures with domain A\mathcal{A} such that μ=ν\mu =\nu on L\mathscr {L}. Furthermore, suppose that Ω=∪An\Omega =\cup A_{n}, where An∈LA_{n} \in \mathscr {L} and μ(An)<+∞\mu \left(A_{n}\right)<+\infty for each n∈Nn \in \mathbb {N}. Then μ=v\mu =v on σ(L)\sigma (\mathscr {L}).

Problem 3.5.7

Let μ\mu and vv denote two σ\sigma-finite measures with domain Bk\mathcal{B}^{k} such that μ=v\mu =v on the subcollection of open subsets of Rk\mathbb {R}^{k}.

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(a)

Show that μ=v\mu =v by appealing to the Uniqueness Theorem.

(b)

Show that μ=v\mu =v by alternatively appealing to Exercise 3.5.6.

(c)

Repeat parts (a) and (b) by replacing the word open with closed.

(d)

Repeat parts (a) and (b) by replacing the word open with compact.

Remark.
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Part (a) is the important part of the exercise.