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Measures and $ \sigma $-algebras

An outer measure such as $ \mu^*$ is a rather crude object since, even if the $ A_i$ are disjoint, there is generally strict inequality in (1.14). It turns out to be unreasonable to expect equality in (1.14), for disjoint unions, for a function defined on all subsets of $ X$. We therefore restrict attention to smaller collections of subsets.


\begin{definition}
A collection of subsets $\mathcal M$ of a set $X$ is a $\si...
...rrow \bigcup^{\infty}_{i=1} E_i \in{\mathcal M}.$\end{enumerate}\end{definition}

For a general outer measure $ \mu^*$ we define the notion of $ \mu^*$-measurability of a set.


\begin{definition}
A set $E \subset X$ is $\mu^*$-measurable (for an outer meas...
...A \cap E^\complement)  \forall A \subset X   .
\end{equation}\end{definition}


\begin{proposition}
The collection of $\mu^*$-measurable sets for any outer measure is
a $\sigma$-algebra.
\end{proposition}

Proof. Suppose $ E$ is $ \mu^*$-measurable, then $ E^C$ is $ \mu^*$-measurable by the symmetry of (2.1).

Suppose $ A$, $ E$ and $ F$ are any three sets. Then

$\displaystyle A \cap (E \cup F) = (A \cap E \cap F) \cup (A \cap E \cap F^C) \cup (A \cap E^C \cap F)$    
$\displaystyle A \cap (E \cup F)^C = A \cap E^C \cap F^C   .$    

From the subadditivity of $ \mu^*$

\begin{multline*}
\mu^* (A \cap (E \cup F)) + \mu^* (A \cap (E \cup F)^C)\\
\le...
...) \\
+ \mu^* (A \cap E^C \cap F) + \mu^* (A \cap E^C \cap F^C).
\end{multline*}

Now, if $ E$ and $ F$ are $ \mu^*$-measurable then applying the definition twice, for any $ A$,

\begin{multline*}
\mu^* (A) = \mu^* (A \cap E \cap F) + \mu^* (A \cap E \cap
F...
...q \mu^* (A \cap (E \cup F)) + \mu^* (A \cap (E \cup F)^C)
  .
\end{multline*}

The reverse inequality follows from the subadditivity of $ \mu^*$, so $ E \cup F$ is also $ \mu^*$-measurable.

If $ \left\{ E_i \right\}^{\infty}_{i=1}$ is a sequence of disjoint $ \mu^*$-measurable sets, set $ F_n= \bigcup^n_{i=1} E_i$ and $ F = \bigcup^{\infty}_{i=1} E_i$. Then for any $ A$,

$\displaystyle \mu^* (A \cap F_n)$ $\displaystyle = \mu^* (A \cap F_n \cap E_n) + \mu^* (A \cap F_n \cap E^C_n)$    
  $\displaystyle = \mu^* (A \cap E_n) + \mu^* (A \cap F_{n-1})   .$    

Iterating this shows that

$\displaystyle \mu^* (A \cap F_n) = \sum^n_{i=1} \mu^* (A \cap E_j)   .$    

From the $ \mu^*$-measurability of $ F_n$ and the subadditivity of $ \mu^*$,

$\displaystyle \mu^* (A)$ $\displaystyle = \mu^* (A \cap F_n) + \mu^* (A \cap F^C_n)$    
  $\displaystyle \geq \sum^n_{i=1} \mu^* (A \cap E_j) + \mu^* (A \cap F^C)   .$    

Taking the limit as $ n \to \infty$ and using subadditivity,

$\displaystyle \mu^* (A)$ $\displaystyle \geq \sum^n_{i=1} \mu^* (A \cap E_j) + \mu^* (A \cap F^C)$ (13)
  $\displaystyle \geq \mu^* (A \cap F) + \mu^*(A \cap F^C) \ge \mu^* (A)$    

proves that inequalities are equalities, so $ F$ is also $ \mu^*$-measurable.

In general, for any countable union of $ \mu^*$-measurable sets,

$\displaystyle \bigcup^{\infty}_{j=1} A_j = \bigcup^{\infty}_{j=1} \widetilde{A}_j   ,$    
$\displaystyle \widetilde{A}_j = A_j \backslash \bigcup^{j-1}_{i=1} A_i = A_j \cap \left( \bigcup^{j-1}_{i=1} A_i \right)^C$    

is $ \mu^*$-measurable since the $ \widetilde{A}_j$ are disjoint. $ \qedsymbol$

A measure (sometimes called a positive measure) is an extended function defined on the elements of a $ \sigma $-algebra $ \mathcal{M}$:

$\displaystyle \mu : \mathcal{M} \to [0, \infty ]$    

such that

$\displaystyle \mu(\emptyset ) = 0$ and (14)
\begin{displaymath}\begin{split}\mu \left( \bigcup^{\infty}_{i=1} A_i \right) = ...
...cal{M} \hbox{ and } A_i \cap A_j = \phi  &i \neq j.\end{split}\end{displaymath} (15)

The elements of $ \mathcal{M}$ with measure zero, i.e., $ E \in \mathcal{M}$, $ \mu (E)
=0$, are supposed to be `ignorable'. The measure $ \mu$ is said to be complete if

$\displaystyle E \subset X \hbox{ and } \exists F \in \mathcal{M}   ,   \mu (F) =0   ,   E \subset F \Rightarrow E \in \mathcal{M}   .$ (16)

See Problem 4.

The first part of the following important result due to Caratheodory was shown above.


\begin{theorem}
If $\mu^*$ is an outer measure on $X$ then the collection of
$...
...a and
$\mu^*$ restricted to $\mathcal{M}$ is a complete measure.
\end{theorem}

Proof. We have already shown that the collection of $ \mu^*$-measurable subsets of $ X$ is a $ \sigma $-algebra. To see the second part, observe that taking $ A=F$ in (2.2) gives

$\displaystyle \mu^* (F) = \sum_j \mu^* (E_j) \hbox{ if } F = \bigcup^{\infty}_{i=1} E_j$    

and the $ E_j$ are disjoint elements of $ \mathcal{M}$. This is (2.4).

Similarly if $ \mu^*(E) =0$ and $ F \subset E$ then $ \mu^*
(F)=0$. Thus it is enough to show that for any subset $ E\subset X,$ $ \mu^*(E) =0$ implies $ E \in \mathcal{M}$. For any $ A \subset X,$ using the fact that $ \mu^*(A\cap E)=0,$ and the `increasing' property of $ \mu^*$

$\displaystyle \mu^* (A)$ $\displaystyle \leq \mu^* (A \cap E) + \mu^* (A \cap E^C)$    
  $\displaystyle =\mu^* (A \cap E^C) \leq \mu^* (A)$    

shows that these must always be equalities, so $ E \in \mathcal{M}$ (i.e., is $ \mu^*$-measurable). $ \qedsymbol$

Going back to our primary concern, recall that we constructed the outer measure $ \mu^*$ from $ 0 \leq u \in (\mathcal{C}_0 (X))'$ using (1.11) and (1.12). For the measure whose existence follows from Caratheodory's theorem to be much use we need


\begin{proposition}
If $0 \leq u \in (\mathcal{C}_0 (X))'$, for $X$ a locally
...
...} and
\eqref{L2.8} and $\mu$ in \eqref{L2.7} is its measure.
\end{proposition}

Proof. Let $ U\subset X$ be open. We only need to prove (2.1) for all $ A \subset X$ with $ \mu^* (A) < \infty$.2

Suppose first that $ A \subset X$ is open and $ \mu^* (A) < \infty$. Then $ A \cap U$ is open, so given $ \epsilon >0$ there exists $ f \in C(X)$ $ \operatorname{supp}(f) \Subset A \cap U$ with $ 0
\leq f \leq 1$ and

$\displaystyle \mu^*(A \cap U)=\mu (A \cap U) \leq u (f)+ \epsilon   .$    

Now, $ A \backslash \operatorname{supp} (f)$ is also open, so we can find $ g \in
C(X)   ,   0 \leq g \leq 1   ,   \operatorname{supp} (g) \Subset A \backslash \operatorname{supp}
(f)$ with

$\displaystyle \mu^*(A \backslash\operatorname{supp} (f))=\mu(A\backslash\operatorname{supp} (f)) \leq u(g) + \epsilon   .$    

Since

$\displaystyle A \backslash \operatorname{supp} (f)$ $\displaystyle \supset A \cap U^C   ,   0 \leq f+g \leq 1   ,   \operatorname{supp} (f+g) \Subset A   ,$    
$\displaystyle \mu (A)$ $\displaystyle \geq u(f+g) =u(f)+u(g)$    
  $\displaystyle > \mu^* (A \cap U) + \mu^* (A \cap U^C) - 2\epsilon$    
  $\displaystyle \geq \mu^* (A) - 2 \epsilon$    

using subadditivity of $ \mu^*.$ Letting $ \epsilon \downarrow 0$ we conclude that

$\displaystyle \mu^* (A) \leq \mu^* (A \cap U) + \mu^* (A \cap U^C) \leq \mu^* (A) = \mu (A)   .$    

This gives (2.1) when $ A$ is open.

In general, if $ E \subset X$ and $ \mu^* (E) < \infty$ then given $ \epsilon >0$ there exists $ A \subset X$ open with $ \mu^* (E) > \mu^*
(A) - \epsilon$. Thus,

$\displaystyle \mu^* (E)$ $\displaystyle \geq \mu^* (A \cap U) + \mu^* (A \cap U^C) -\epsilon$    
  $\displaystyle \geq \mu^* (E \cap U) + \mu^* (E \cap U^C) -\epsilon$    
  $\displaystyle \geq \mu^* (E) - \epsilon   .$    

This shows that (2.1) always holds, so $ U$ is $ \mu^*$-measurable if it is open. We have already observed that $ \mu (U) = \mu^* (U)$ if $ U$ is open. $ \qedsymbol$

Thus we have shown that the $ \sigma $-algebra given by Caratheodory's theorem contains all open sets. You showed in Problem 3 that the intersection of any collection of $ \sigma $-algebras on a given set is a $ \sigma $-algebra. Since $ \mathcal{P} (X)$ is always a $ \sigma $-algebra it follows that for any collection $ \mathcal{E}
\subset \mathcal{P} (X)$ there is always a smallest $ \sigma $-algebra containing $ \mathcal{E}$, namely

$\displaystyle \mathcal{M}_{\mathcal{E}} = \bigcap \left\{ \mathcal{M} \supset \...
...box{ is a $\sigma$-algebra }, \mathcal{M} \subset \mathcal{P} (X) \right\}   .$    

The elements of the smallest $ \sigma $-algebra containing the open sets are called `Borel sets'. A measure defined on the $ \sigma $-algebra of all Borel sets is called a Borel measure. This we have shown:


\begin{proposition}
The measure defined by \eqref{L2.7}, \eqref{L2.8} from $0 \l...
...cal{C}_0
(X))'$ by Caratheodory's theorem is a Borel measure.
\end{proposition}

Proof. This is what Proposition 2.5 says! See how easy proofs are. $ \qedsymbol$

We can even continue in the same vein. A Borel measure is said to be outer regular on $ E \subset X$ if

$\displaystyle \mu (E) = \inf \left\{ \mu (U)   ;   U \supset E   ,   U \hbox{ open} \right\}   .$ (17)

Thus the measure constructed in Proposition 2.5 is outer regular on all Borel sets! A Borel measure is inner regular on $ E$ if

$\displaystyle \mu (E) = \sup \left\{ \mu (K)   ;   K \subset E   ,   K \hbox{ compact} \right\}   .$ (18)

Here we need to know that compact sets are Borel measurable. This is Problem 5.


\begin{definition}
A \emph{Radon measure} (on a metric space) is a
Borel measur...
...ts, inner
regular on open sets and finite on compact sets.
\par\end{definition}


\begin{proposition}
The measure defined by \eqref{L2.7}, \eqref{L2.8} from $0 \l...
...{C}_0
(X))'$ using Caratheodory's theorem is a Radon measure.
\end{proposition}

Proof. Suppose $ K \subset X$ is compact. Let $ \chi_K$ be the characteristic function of $ K   ,   \chi_K =1$ on $ K   ,  
\chi_K =0$ on $ K^C$. Suppose $ f \in \mathcal{C}_0 (X)   ,   \operatorname{supp} (f)
\Subset X$ and $ f \geq \chi_K$. Set

$\displaystyle U_{\epsilon } = \left\{ x \in X   ;   f (x) > 1-\epsilon \right\}$    

where $ \epsilon >0$ is small. Thus $ U_{\epsilon }$ is open, by the continuity of $ f$ and contains $ K$. Moreover, we can choose $ g \in C (X)  
,   \operatorname{supp} (g) \Subset U_{\epsilon }   ,   0 \leq g \leq 1$ with $ g=1$ near3 $ K$. Thus, $ g \leq (1-\epsilon
)^{-1} f$ and hence

$\displaystyle \mu^* (K) \leq u (g) = (1-\epsilon)^{-1} u (f)   .$    

Letting $ \epsilon \downarrow 0$, and using the measurability of $ K$,

$\displaystyle \mu (K) \leq u (f)$    
$\displaystyle \Rightarrow \mu (K) = \inf \left\{ u (f)   ;   f \in C (X)   ,   \operatorname{supp} (f) \Subset X     , f \geq \chi_K \right\}   .$    

In particular this implies that $ \mu (K) < \infty$ if $ K \Subset X$, but is also proves (2.7). $ \qedsymbol$

Let me now review a little of what we have done. We used the positive functional $ u$ to define an outer measure $ \mu^*$, hence a measure $ \mu$ and then checked the properties of the latter.

This is a pretty nice scheme; getting ahead of myself a little, let me suggest that we try it on something else.

Let us say that $ Q \subset \mathbb{R}^n$ is `rectangular' if it is a product of finite intervals (open, closed or half-open)

$\displaystyle Q= \prod^n_{i=1} (\hbox{or}[a_i   ,   b_i]\hbox{or})  a_i \leq b_i$ (19)

we all agree on its standard volume:

$\displaystyle v(Q) = \prod^n_{i=1} (b_i - a_i ) \in [0, \infty)   .$ (20)

Clearly if we have two such sets, $ Q_1 \subset Q_2$, then $ v(Q_1) \le v(Q_2)$. Let us try to define an outer measure on subsets of $ \mathbb{R}^n$ by

$\displaystyle v^* (A) = \inf \left\{ \sum^{\infty}_{i=1} v(Q_i)   ;   A \subset \bigcup^{\infty}_{i=1} Q_i, Q_i\hbox{ rectangular}\right\}   .$ (21)

We want to show that (2.10) does define an outer measure. This is pretty easy; certainly $ v(\emptyset) =0$. Similarly if $ \left\{ A_i \right\}^{\infty}_{i=1}$ are (disjoint) sets and $ \left\{ Q_{ij} \right\}^{\infty}_{i=1}$ is a covering of $ A_i$ by open rectangles then all the $ Q_{ij}$ together cover $ A= \bigcup_i
A_i$ and

$\displaystyle v^* (A) \leq \sum_i \sum_j v(Q_{ij})$    
$\displaystyle \Rightarrow v^* (A) \leq \sum_i v^* (A_i)   .$    

So we have an outer measure. We also want


\begin{lemma}
If $Q$ is rectangular then $v^*(Q)=v(Q).$\end{lemma}

Assuming this, the measure defined from $ v^*$ using Caratheodory's theorem is called Lebesgue measure.


\begin{proposition}
Lebesgue measure is a Borel measure.
\end{proposition}

To prove this we just need to show that (open) rectangular sets are $ v^*$-measurable.

Suppose that $ \mathcal{M}$ is a $ \sigma $-algebra on a set $ X$4 and $ \mathcal{N}$ is a $ \sigma $-algebra on another set $ Y$. A map $ f: X
\to Y$ is said to be measurable with respect to these given $ \sigma $-algebras on $ X$ and $ Y$ if

$\displaystyle f^{-1} (E) \in \mathcal{M}  \forall E \in \mathcal{N}   .$ (22)

Notice how similar this is to one of the characterizations of continuity for maps between metric spaces in terms of open sets. Indeed this analogy yields a useful result.


\begin{proposition}
Any continuous map $f: X \to Y$ between metric spaces is
me...
...th respect to the Borel $\sigma$-algebras on $X$ and
$Y$.
\par\end{proposition}

Proof. The main point to note here is that $ f^{-1}$ as a map on power sets, is very well behaved for any map. That is if $ f: X
\to Y$ then $ f^{-1}: \mathcal{P}(Y) \to \mathcal{P}(X)$ satisfies:

\begin{displaymath}\begin{gathered}f^{-1} (E^C) = (f ^{-1} (E) )^C \ [1ex] f^{-...
... f^{-1} (\phi) = \phi   ,  f^{-1} (Y) = X   . \end{gathered}\end{displaymath} (23)

Putting these things together one sees that if $ \mathcal{M}$ is any $ \sigma $-algebra on $ X$ then

$\displaystyle \left\{ E \subset Y   ;   f^{-1} (E) \in \mathcal{M} \right\}$ (24)

is always a $ \sigma $-algebra on $ Y$.

Going back to the proof of the proposition, the continuity of $ f$ shows that $ f^{-1}(E) \subset X$ is open if $ E \subset Y$ is open. Thus the $ \sigma $-algebra on $ Y$ defined by (2.13) from the Borel $ \sigma $-algebra on $ X$ contains all open sets. It therefore contains the Borel $ \sigma $-algebra on $ Y$, i.e.,

$\displaystyle f^{-1} (\mathcal{B} (Y)) \subset\mathcal{B}(X)   .$    

$ \qedsymbol$

We are mainly interested in functions on $ X$. If $ \mathcal{M}$ is a $ \sigma $-algebra on $ X$ then $ f:X \to \mathbb{R}$ is measurable if it is measurable with respect to the Borel $ \sigma $-algebra on $ \mathbb{R}$ and $ \mathcal{M}$ on $ X$. More generally, for an extended function $ f: X \to [ - \infty , \infty ]$ we take as the `Borel' $ \sigma $-algebra in $ [- \infty , \infty]$ the smallest $ \sigma $-algebra containing all open subsets of $ \mathbb{R}$ and all sets $ (a, \infty ]$ and $ [- \infty , b);$ in fact it is generated by the sets $ (a,\infty].$ (See Problem 6.)

Our main task is to define the integral of a measurable function: we start with simple functions. Observe that the characteristic function of a set

$\displaystyle \chi_E = \left\{ \begin{array}{cc} 1 & x \in E \ 0 & x \notin E \end{array} \right.$    

is measurable if and only if $ E \in \mathcal{M}$. More generally a simple function,

$\displaystyle f = \sum^N_{i=1} a_i \chi_{E_i}$ (25)

is measurable if the $ E_i$ are measurable. The presentation, (2.14), of a simple function is not unique. We can make it so, getting the minimal presentation, by insisting that all the $ a_i$ are non-zero and

$\displaystyle E_i = \left\{ x \in E   ;   f(x) = a_i \right\}$    

then $ f$ in (2.14) is measurable iff all the $ E_i$ are measurable.


next up previous contents
Next: Integration Up: Lecture notes for 18.155, Previous: Continuous functions   Contents
Richard B. Melrose 2003-02-18