Measure Theory, $\sigma$-algebra Folland Problem 23

1.4k Views Asked by At

I'm preparing for my exam. Can anyone help me in this matter, is confusing to me

enter image description here

thank you very much.

2

There are 2 best solutions below

0
On BEST ANSWER

Part b:

Here $\mathcal{P}(\mathbb Q)$ is simply the powerset of $\mathbb Q$. Thus we are trying to show that every subset of $\mathbb Q$ can be obtained by countably many union and complement operations on the sets $(a,b]$.

First observe that any singleton $\{r\}$ can be obtained in the manner, since $$ \{r\}=\bigcap_{\substack{s<r\\s\in \mathbb Q}}(s,r]. $$ Next observe that for any $R\subset \mathbb Q$, we have $$ R=\bigcup_{r\in R}\{r\}. $$ Consequently $\mathcal{P}(\mathbb Q)$ is the $\sigma$-algebra generated by the sets $(a,b]$.

Part c:

Define $\mu(\{r\})$ to be any number you like, for each $r\in\mathbb{Q}$ and extend to all of $\mathcal{P}(\mathbb{Q})$ by $\sigma$-additivity. You get $\mu((a,b])=\infty=\mu_0((a,b])$.

0
On

Let $\mathcal{A}$ be the collection of finite unions of sets of the form $(a,b]\cap\mathbb{Q}$ where $-\infty \leq a < b\leq \infty$

a.) $\mathcal{A}$ is an $\sigma$-algebra on $\mathbb{Q}$

b.) The $\sigma$-algebra generated by $\mathbb{A}$ is $\mathcal{P}(\mathbb{Q})$

c.) Define $\mu_0$ on $\mathcal{A}$ by $\mu_0(\emptyset) = 0$ and $\mu_0(A) = \infty$. Then $\mu_0$ is a premeasure on $\mathcal{A}$, and there is more than one measure on $\mathcal{P}(\mathbb{Q})$ whose restriction to $\mathcal{A}$ is $\mu_0$.

Proof a.) - Let $\varepsilon = \{(a,b]\cap \mathbb{Q}: a,b\in\overline{\mathbb{R}}\}$. Clearly $\emptyset = (0,0]\cap\mathbb{Q}\in\varepsilon$. If $(a_1,b_1]\cap\mathbb{Q}\in\varepsilon$ and $(a_2,b_2]\cap\mathbb{Q}\in\varepsilon$ then their intersection is $(\max\{a_1,a_2\},\min\{b_1,b_2\})\cap\mathbb{Q}\in \varepsilon$. Moreover, the complement of $(a,b]\cap\mathbb{Q}$ is $(-\infty,a]\cap\mathbb{Q}\cup (b,\infty]\cap\mathbb{Q}$ which is a disjoint union of elements of $\varepsilon$ if $a\leq b$. If $a>b$ then the complement of $(a,b]\cap\mathbb{Q}$ is $(-\infty, \infty]\cap\mathbb{Q}\in\varepsilon$. This shows that $\varepsilon$ is an elementary family of subsets of $\mathbb{Q}$, so the collection of finite disjoint unions of members of $\varepsilon$ is an algebra by proposition 1.7. Let $(a_1,b_1]\cap\mathbb{Q}\in\varepsilon$ and $(a_2,b_2]\cap\mathbb{Q}\in\varepsilon$ be not disjoint. Then, $(a_1,b_1]\cap\mathbb{Q}\cup (a_2,b_2]\cap\mathbb{Q} = ((a_1,b_1]\cup (a_2,b_2])\cap\mathbb{Q}$. So we need to figure out what is $(a_1,b_1]\cup (a_2,b_2]$ which we have 4 different outcomes: \begin{align*} (a_1,b_1]\cup (a_2,b_2] =\\ &1. (a_1,b_2] \ \ \text{if} \ \ a_1\leq a_2\leq b_1 < b_2\\ &2. (a_1,b_1] \ \ \text{if} \ \ a_1\leq a_2< b_2 \leq b_1\\ &3. (a_2,b_2] \ \ \text{if} \ \ a_2\leq a_1\leq b_1 \leq b_2\\ &4. (a_2,b_1] \ \ \text{if} \ \ a_2\leq a_1< b_2 \leq b_1\\ \end{align*} which are all in $\varepsilon$ thus $\mathcal{A}$ is the collection of finite disjoint unions of members of $\varepsilon$, so $\mathcal{A}$ is a $\sigma$-algebra.

Proof b.) - Suppose that $r\in\mathbb{Q}$. Then $$\{r\} = \bigcap_{n\geq 1}((r-1/n,r]\cap\mathbb{Q})\in M(\mathcal{A})$$ If $X\subset \mathbb{Q}$, then $X$ is countable, say $X = \{x_1,\ldots\}$. But $\{x_j\}\in M(\mathcal{A})$ for all $j\geq 1$. So $$X = \bigcup_{j\geq 1}\{x_j\}\in M(\mathcal{A})$$ Therefore $M(\mathcal{A}) = \mathcal{P}(\mathbb{Q})$

Proof c.) - It is clear that $\mu_0$ is a premeasure on $\mathcal{A}$. The induced outer measure is $$\mu^*(E) = \inf\{\sum_{1}^{\infty}\mu_0(E_j):E_j\in\mathcal{A},E\subset \bigcup_{1}^{\infty}E_j\}$$ it follows that from theorem 1.14 that $\mu = \mu^*$ is a measure on $\mathcal{P}(\mathbb{Q})$ which extends $\mu_0$.

If $\nu$ is a counting measure on $\mathcal{P}(\mathbb{Q})$ then $\nu(\emptyset) = 0 = \mu_0(\emptyset)$. And for $a<b$, $E = (a,b]\cap\mathbb{Q}$ has infinite cardinality, so $\nu(E) = \infty = \mu_0(E)$ and therefore $\nu|\varepsilon = \mu_0|\varepsilon$. By finite additivity of $\nu$, it follows that $\nu(E) = \infty = \mu_0(E)$ for all $\emptyset \neq E\in\mathcal{A}$. So that $\nu|\mathcal{A} = \mu_0$. But $\nu\{1\} = 1 < \infty = \mu(\{1\})$, so $\nu$ is a different measure on $\mathcal{P}(\mathbb{Q})$ which extends $\mu_0$.