Ch2. Integration Theory (Ex.12 ~ Ex.24)
12. Show that there exist \(f \in L^1\) and a sequence \(\{f_n\} \subset L^1\) such that \(\|f_n - f\|_1 \to 0\) but \(\lim_{n \to \infty} f_n(x) \ne f(x)\).
proof
① Definition of \(I_n\) and \(f_n\)
For every \(n \in \mathbb{N}\),
there exists \(k \in \mathbb{Z}^+\)
such that \(2^k \le n <
2^{k+1}\).
Let \(\ell = n - 2^k\) and
\[I_n = \left[\frac{\ell}{2^{k+1}},
\frac{\ell+1}{2^{k+1}}\right], \quad f_n = \chi_{I_n}.\]
(e.g. when \(n=9\), \(2^3 \le n < 2^4\), \(\ell = 1\), \(I_n
= \left[\frac{1}{16}, \frac{2}{16}\right]\).)
② \(\lim_{n \to \infty} f_n(x) \ne 0\) for \(x \in [0,1]\)
Since \([0,1] = \bigcup I_n\), we have \(x \in I_n\) for some \(n\) with \(2^k \le n < 2^{k+1}\) (\(k = 0,1,2,\dots\)).
For a given integer \(M \in
\mathbb{N}\) such that \(M <
2^k\) for some \(k \in
\mathbb{N}\),
\(x \in I_n\) for some proper \(N \in \mathbb{N}\) with \(2^k \le N < 2^{k+1}\) and \(f_n(x) = 1 > 0\) when \(n = N\).
This holds for all \(M \in
\mathbb{N}\),
so \(\limsup_{n \to \infty} f_n(x) \ne
0\).
③ \(\lim_{n \to \infty} \|f_n\|_{L^1} = 0\)
When \(2^k \le n < 2^{k+1}\),
\[
\int |f_n(x)|\,dx = \frac{1}{2^{k+1}}.
\] As \(n \to \infty\) implies
\(k \to \infty\),
so \(\lim_{n \to \infty} \|f_n\|_1 = \lim_{k
\to \infty} \frac{1}{2^{k+1}} = 0\).
12. Show that there exist \(f \in L^1\) and a sequence \(\{f_n\} \subset L^1\) such that \(\|f_n - f\|_1 \to 0\) but \(\lim_{n \to \infty} f_n(x) \ne f(x)\).
proof
① Definition of \(I_n\) and \(f_n\)
For every \(n \in \mathbb{N}\),
there exists \(k \in \mathbb{Z}^+\)
such that \(2^k \le n <
2^{k+1}\).
Let \(\ell = n - 2^k\) and
\[I_n = \left[\frac{\ell}{2^{k+1}},
\frac{\ell+1}{2^{k+1}}\right], \quad f_n = \chi_{I_n}.\]
(e.g. when \(n=9\), \(2^3 \le n < 2^4\), \(\ell = 1\), \(I_n
= \left[\frac{1}{16}, \frac{2}{16}\right]\).)
② \(\lim_{n \to \infty} f_n(x) \ne 0\) for \(x \in [0,1]\)
Since \([0,1] = \bigcup I_n\), we have \(x \in I_n\) for some \(n\) with \(2^k \le n < 2^{k+1}\) (\(k = 0,1,2,\dots\)).
For a given integer \(M \in
\mathbb{N}\) such that \(M <
2^k\) for some \(k \in
\mathbb{N}\),
\(x \in I_n\) for some proper \(N \in \mathbb{N}\) with \(2^k \le N < 2^{k+1}\) and \(f_n(x) = 1 > 0\) when \(n = N\).
This holds for all \(M \in
\mathbb{N}\),
so \(\limsup_{n \to \infty} f_n(x) \ne
0\).
③ \(\lim_{n \to \infty} \|f_n\|_{L^1} = 0\)
When \(2^k \le n < 2^{k+1}\),
\[
\int |f_n(x)|\,dx = \frac{1}{2^{k+1}}.
\] As \(n \to \infty\) implies
\(k \to \infty\),
so \(\lim_{n \to \infty} \|f_n\|_1 = \lim_{k
\to \infty} \frac{1}{2^{k+1}} = 0\).
14. Let \(V_d\) be a measure of a unit ball in \(\mathbb{R}^d\).
(a) Show that \(V_d = 2 \int_0^1 (1 - x^2)^{\frac{d-1}{2}} dx\).
proof We’ll just accept that \(m(A^t) = m(A)\), where \(A^t = \{(x, -y) : (x, y) \in A\}\) (by reflection symmetry).
① \(\mathbb{R}^d \times \{0\}\) has measure 0 (\(d \in \mathbb{N}\))
Let \(E_n = Q_n \times \{0\}\),
where \(Q_n \subset \mathbb{R}^d\) is a
cube centered at the origin with side length \(2n\): \[Q_n =
[-n, n]^d.\] Since \(m(Q_n) =
(2n)^d\) and \(m(\{0\}) =
0\),
\[m(E_n) = (2n)^d \cdot 0 = 0 \quad
(\text{Prop 2.3.6}).\]
Then \(E_n \subset E_{n+1}\) for all
\(n \in \mathbb{N}\) and \(\bigcup_{n=1}^\infty E_n = \mathbb{R}^d \times
\{0\}\),
so \[
m(\mathbb{R}^d \times \{0\}) = \lim_{n \to \infty} m(E_n) = 0 \quad
(\text{Cor 1.3.3}).
\]
② \(E = \{(x, 0) \in \mathbb{R}^{d+1} : |x| > 1\}\), then \(m(B_1^{(d+1)}) = m(B_1^{(d)} \cup E)\)
\(B_1^{(d+1)}\) can be written as
\(B \cup B^t \cup E\),
where \(B = \{(x, y) \in \mathbb{R}^{d+1} :
|x| \le 1, 0 \le y \le (1 - x^2)^{1/2}\}\).
Let \(E = \{(x, 0) \in \mathbb{R}^{d+1} :
|x| > 1\}\),
then \(m(E) = 0\) (\(E \subset \mathbb{R}^d \times \{0\}\)) and
\(E \cap B_1^{(d)} =
\varnothing\).
Then,
\[m(B_1^{(d)} \cup E) = m(B_1^{(d)}) + m(E) =
m(B_1^{(d)}).\]
③ \(A = \{(x, y) \in \mathbb{R}^{d+1} : 0 \le y \le f(x)\}\), then \(m(B_1^{(d+1)}) = 2m(A)\)
Let
\[
f(x) =
\begin{cases}
(1 - x^2)^{1/2}, & |x| \le 1, \\
0, & \text{o.w.}
\end{cases}
\] and
\[A = \{(x, y) \in \mathbb{R}^{d+1} : 0 \le y
\le f(x)\} = B \cup E.\]
Then \(A^t = B^t \cup E\).
Hence,
\[
m(B_1^{(d+1)}) = m(B \cup B^t \cup E)
= m((B \cup E) \cup (B^t \cup E))
= m(A \cup A^t)
= m(A) + m(A^t) - m(A \cap A^t).
\] Since
\[A \cap A^t = \{(x, 0) : x \in
\mathbb{R}^d\},\]
which has measure 0 (by ①),
\[m(B_1^{(d+1)}) = 2m(A).\]
Thus,
\[
m(B_1^{(d+1)}) = V_{d+1} = 2 \int_{-1}^1 f(x)\,dx = 2 \int_0^1 (1 -
x^2)^{d/2} dx.
\] (by Cor. 2.3.8)
(b) Show that \(v_d = 2v_{d-1} \int_0^1 (1 - x^2)^{\frac{d-1}{2}} dx\)
\(B^{(d)}\) can be written as \(B^{(d-1)}_{1-x^2} \times B^{(1)}_x\).
proof
\[ B^{(d)} = \{ (z, x) \in \mathbb{R}^{d-1} \times \mathbb{R} : |x| \le 1 \text{ and } |z| \le (1 - x^2)^{1/2} \}. \]
Then,
\[ m(B^{(d)}) = \int_{B^{(d)}} 1 \, dz \, dx = \int \int_{\{z : (z, x) \in B^{(d)}\}} 1 \, dz \, dx \quad (\text{by Fubini's theorem}) \]
\[ = \int_{-1}^1 \int_{B^{(d-1)}_{\sqrt{1 - x^2}}} 1 \, dz \, dx = \int_{-1}^1 v_{d-1} (1 - x^2)^{\frac{d-1}{2}} dx = 2 v_{d-1} \int_0^1 (1 - x^2)^{\frac{d-1}{2}} dx \]
(c) Show that \(v_d = \pi^{d/2} / \Gamma(\frac{d}{2} + 1)\)
proof
① \(v_1\)
In \(\mathbb{R}^1\), \(B^{(1)}_1\) is an open interval of length
2.
So, \(v_1 = 2\).
② \(v_d\)
Let \(x^2 = t\) so that \(2x dx = dt\) \((0 \le t \le 1)\). Then,
\[\begin{align*} \int_0^1 (1 - x^2)^{\frac{d-1}{2}} dx &= \int_0^1 (1 - t)^{\frac{d-1}{2}} \cdot \frac{1}{2} t^{-1/2} dt \\ &= \frac{1}{2} \int_0^1 t^{\frac{1}{2} - 1} (1 - t)^{\frac{d+1}{2} - 1} dt \\ &= \frac{1}{2} \mathrm{Beta}\left( \frac{1}{2}, \frac{d+1}{2} \right) \\ &= \frac{1}{2} \frac{\Gamma(\frac{1}{2}) \Gamma(\frac{d+1}{2})}{\Gamma(\frac{d}{2} + 1)}. \end{align*}\]
Then,
\[ v_d = 2 v_{d-1} \cdot \frac{1}{2} \frac{\Gamma(\frac{1}{2}) \Gamma(\frac{d+1}{2})}{\Gamma(\frac{d}{2} + 1)} = v_{d-1} \pi^{1/2} \frac{\Gamma(\frac{d+1}{2})}{\Gamma(\frac{d}{2} + 1)}. \]
So,
\[ v_d = v_1 (\pi^{1/2})^{d-1} \frac{\Gamma(\frac{d+1}{2})}{\Gamma(\frac{d}{2} + 1)} = 2 (\pi^{1/2})^{d-1} \frac{1}{2} \frac{\Gamma(\frac{1}{2}) \Gamma(\frac{d+1}{2})}{\Gamma(\frac{d}{2} + 1)} = \frac{(\pi)^{d/2}}{\Gamma(\frac{d}{2} + 1)}. \]
(PMA 8.18, 8.20)
15. Consider the function \(f(x) = \begin{cases}x^{1/2}, & 0 < x < 1 \\0, & \text{o.w.}\end{cases}\) For a fixed enumeration \(\{r_n\}\) of the rationals \(\mathbb{Q}\), let \(F(x) = \sum_{n=1}^\infty 2^{-n} f(x - r_n)\). Then, show that
(1) \(\int_{\mathbb{R}} f(x) dx = 2\)
proof
①
\(f\) is continuous on \([a, b]\) \((0
< a < b < 1)\), so \(f \in
\mathbb{R}\) on \([a,b]\) (PMA
6.8).
Then
\[ \int_{[a,b]} f(x) dx = \int_a^b x^{1/2} dx = \left[\frac{1}{\frac{3}{2}}x^{3/2}\right]_a^b = 2(b^{1/2} - a^{1/2}) = \int_{[a,b]} f(x) dx \]
(thm 2.1.5).
Let the number \(b'\) greater than
\(1/2\).
②
Let \(f_n(x) =
\begin{cases}
f(x), & n \le x \le b \\
0, & \text{o.w.}
\end{cases}\)
and \(f(x) = 0\) for \(x \in \mathbb{R}\).
For \(x \in [\frac{1}{n+1}, \frac{1}{n})\), \(f_{n,m}(x) > 0\) and \(f_{n,m}(x) = 0\).
This leads to \(f_{n,m}(x) \ge
f_n(x)\) \((x \in
\mathbb{R})\).
\(f_n\) is measurable, and \(\lim_{n \to \infty} f_n(x) = f(x)
\chi_{(0,b)}(x)\) for every \(x \in
\mathbb{R}\).
So
\[ \lim_{n \to \infty} \int f_n(x) dx = \int f(x)\chi_{(0,b)}(x) dx \]
(thm 2.1.9, monotone convergence theorem).
\[ \int_{a}^{b} f_n(x) dx = 2(b - \sqrt{\frac{1}{n}}) \]
so
\[ \int f(x) \chi_{(0,b)}(x) dx = 2b. \]
Similar approach to the right limit of the interval \([a,b]\) leads to \(\int_0^1 f(x) dx = 2.\)
(2) \(|F(x)| < \infty\) a.e. \(x\)
proof
By translation invariance,
\[\int f(x - r_n) dx = \int f(x) dx =
2.\]
\(f\) is non-negative and measurable, so
\[\begin{align*} \int F(x) dx &= \int \sum_{n=1}^\infty 2^{-n} f(x - r_n) dx \\ &= \sum_{n=1}^\infty 2^{-n} \int f(x - r_n) dx \quad (\text{MCT}) \\ &= \sum_{n=1}^\infty 2^{-n} \times 2 = 2. \end{align*}\]
Since \(\int F < \infty\), \(|F(x)| < \infty\) a.e. \(x \in \mathbb{R}\).
(3) Show that \(F\) is unbounded on every open interval.
proof
① \(r_n \in I\)
Let \(I = (a, b)\) be some open
interval of \(\mathbb{R}\),
then \(I\) contains some rational \(r_n\): \(a <
r_n < b\)
(\(\because \mathbb{Q}\) is
dense in \(\mathbb{R}\)).
② \(f(x - r_n)\) is unbounded on \(I\).
For given \(M > 0\),
\[ f(x - r_n) > M \Leftrightarrow (x - r_n)^{1/2} > M \Leftrightarrow M < \frac{1}{x - r_n} \Leftrightarrow M^2 < \frac{1}{x - r_n} \Leftrightarrow 0 < x - r_n < \frac{1}{M^2} \]
\(\Rightarrow r_n < x < r_n + \frac{1}{M^2}\).
Let \(b_M = \min(b, r_n +
\frac{1}{M^2})\),
then \(f(x - r_n) > M\) holds when
\(x \in (r_n, b_M) \subset (a,
b)\).
This means for every \(M > 0\),
there is \(x \in (r_n, b_M)\) such that
\(f(x - r_n) > M\).
So, \(f(x - r_n)\) is unbounded on
\(I\).
③ \(F\) is unbounded on \(I\).
Thus, for every \(M' > 0\),
there is \(x \in I\) such that
\(F(x) \ge 2^{-n} f(x - r_n) > 2^{-n} M \ge
M'\).
This means \(F\) is unbounded on
\(I\).
Since \(I\) is an arbitrary
interval on \(\mathbb{R}\), \(F\) is unbounded on every interval.
(4) \(\tilde{F} = F\) for a.e. \(x \in \mathbb{R}\), then show that \(\tilde{F}\) is unbounded in any interval.
proof
\(\tilde{F}(x) = F(x)\) for a.e.
\(x \in I\).
There is \(x \in (r_n, b_M) \subset I\)
such that \(F(x) > M'\) for
every \(M'\).
Then, for a.e. \(x \in (r_n, b_M)\),
\(\tilde{F}(x) > M'\)
holds.
Thus, \(\tilde{F}\) is unbounded.
Let \(\tilde{I} = \bigcup I_x\) such
that \(\tilde{F} = F\) on \(I_x\) and \(I_x
\cap I_{x'} = \emptyset\) \((x \ne
x')\).
\(F\) is unbounded on \(I_x \subset I\), so \(\tilde{F}\) is unbounded on \(I\).
16. \(f\) is integrable on \(\mathbb{R}^d\), and \(\delta = (\delta_1, \dots, \delta_d)\) is a d-tuple of non-zero real numbers. Let \(f^\delta(x) = f(\delta x) = f(\delta_1 x_1, \dots, \delta_d x_d)\). Then show that \(f^\delta\) is integrable and \[\int_{\mathbb{R}^d} f^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int_{\mathbb{R}^d} f(x) dx.\](\(\delta x = (\delta_1 x_1, \dots, \delta_d x_d)\))
proof
① \(\chi_{E^\delta}(x) = \chi_E(\delta x)\) (measurable \(E\))
\(\delta x \in E \Leftrightarrow x \in
\delta^{-1}E\), so \(\chi_E(\delta x) =
\chi_{\delta^{-1}E}(x)\).
Then,
\[ \int \chi_E(\delta x) dx = \int \chi_{\delta^{-1}E}(x) dx = m(\delta^{-1}E) = |\delta_1|^{-1} \cdots |\delta_d|^{-1} m(E) \]
(ex 1-9)
\[ = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int \chi_E(x) dx. \]
② For simple function \(\varphi\),
\[ \int \varphi^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int \varphi(x) dx. \]
Let \(\varphi(x) = \sum_{k=1}^m a_k \chi_{E_k}(x)\), then \(\varphi^\delta(x) = \sum_{k=1}^m a_k \chi_{E_k}(\delta x)\).
So,
\[\begin{align*} \int \varphi^\delta(x) dx &= \sum_{k=1}^m a_k \int \chi_{E_k}(\delta x) dx = \sum_{k=1}^m a_k m(\delta^{-1} E_k) \\ &= |\delta_1|^{-1} \cdots |\delta_d|^{-1} \sum_{k=1}^m a_k m(E_k) = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int \varphi(x) dx. \end{align*}\]
③ For measurable & non-negative \(f\),
\[ \int f^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \]
There is a sequence of non-negative simple functions \(\varphi_k\) such that \(\varphi_k \uparrow f\) (thm 1.4.1).
Then it is obvious that \(\varphi_k^\delta
\uparrow f^\delta(x)\).
\(\varphi_k^\delta\) is a sequence of
non-negative measurable functions, so
\[ \lim_{k \to \infty} \int \varphi_k^\delta(x) dx = \int f^\delta(x) dx \quad (\text{monotone convergence thm 2.1.9}). \]
Thus,
\[ \int f^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \lim_{k \to \infty} \int \varphi_k(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \quad (\text{: MCT}) \]
④ For real-valued and measurable \(f\),
\[ \int f^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \]
\(f^\delta(x) = f^{\delta+}(x) -
f^{\delta-}(x)\), where \(f^{\delta+} =
\max(f^\delta, 0)\) and \(f^{\delta-} =
\max(-f^\delta, 0)\).
\(f^{\delta+}\) and \(f^{\delta-}\) are non-negative and
measurable. Then,
\[\begin{align*} \int f^\delta(x) dx &= \int f^{\delta+}(x) dx - \int f^{\delta-}(x) dx \\ &= |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f^+(x) dx - |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f^-(x) dx \\ &= |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \end{align*}\]
⑤ If \(f = u + iv \in L^1\), then
\[ \int f^\delta(x) dx = |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \]
\[\begin{align*} \int f^\delta(x) dx &= \int u^\delta(x) dx + i \int v^\delta(x) dx \\ &= |\delta_1|^{-1} \cdots |\delta_d|^{-1} \left( \int u(x) dx + i \int v(x) dx \right) \\ &= |\delta_1|^{-1} \cdots |\delta_d|^{-1} \int f(x) dx. \end{align*}\]
17. \(f\) is defined on \(\mathbb{R}^2\) as follows: for \(n \in \mathbb{Z}^+\), \[f(x, y) =\begin{cases}a_n, & n \le y < n+1 \text{ and } n \le x < n+1 \\-a_n, & n \le x < n+1 \text{ and } n+1 \le y < n+2 \\0, & \text{otherwise.}\end{cases} \] Here, \(a_n = \sum_{k=0}^n b_k\) where \(\{b_k\}\) is a sequence of positive real numbers such that \(\sum_{k=0}^\infty b_k = s < \infty\). Let \(a_0 = 0\) for simplicity.
(a)-1 Show that \(f^y\) is integrable
proof
① \(y < 0\): \(f(x, y) = 0\) for all \(x \in \mathbb{R}\), so \(f^y(x) = 0\) which is integrable.
② \(n \le y < n+1\) \((n \in \mathbb{Z}^+)\)
\[ f(x, y) = \begin{cases} a_n, & n \le x < n+1 \\ -a_{n-1}, & n-1 \le x < n \\ 0, & \text{o.w.} \end{cases} \]
Then, \(f^y(x) = a_n \chi_{[n, n+1)}(x) -
a_{n-1} \chi_{[n-1, n)}(x)\), and
\(\int f^y(x) dx = a_n - a_{n-1} <
\infty.\)
(a)-2 Show that \(f_x\) is integrable & \(\int f_x(y) dy = 0\) \(\forall x \in \mathbb{R}\)
proof
① \(x < 0\): \(f(x, y) = 0\) for all \(y \in \mathbb{R}\), so \(f_x(y) = 0\) and \(\int f_x(y) dy = 0 < \infty\).
② \(n \le x < n+1\) \((n \in \mathbb{Z}^+)\)
\[ f(x, y) = \begin{cases} a_n, & n \le y < n+1 \\ -a_n, & n+1 \le y < n+2 \\ 0, & \text{o.w.} \end{cases} \]
Then, \(f_x(y) = a_n \chi_{[n, n+1)}(y) -
a_n \chi_{[n+1, n+2)}(y)\),
so \(\int f_x(y) dy = a_n - a_n =
0.\)
(a)-3 Show that \(\int_{\mathbb{R}} \int_{\mathbb{R}} f(x, y) dy dx = 0\)
proof
\[ \int_{\mathbb{R}} \int_{\mathbb{R}} f(x, y) dy dx = \int_{\mathbb{R}} 0 dx = 0 \quad (\text{by (a)-2}) \]
(b) Show that \(\int f^y(x) dx\) is integrable on \((0, \infty)\) and \(\iint f(x, y) dx dy = s\)
proof
We’ve shown in (a)-1 that \(\int f^y(x) dx
= a_n - a_{n-1}\) for \(y \in [n,
n+1)\).
Since \(a_n\) is finite for all \(n \in \mathbb{Z}^+\), \(\int f^y(x) dx < \infty\) for \(y \in \mathbb{R}\) (as well as \((0, \mathbb{R}^+)\)).
Then,
\[\begin{align*} \iint f(x, y) dx dy &= \sum_{n=0}^\infty \int_n^{n+1} \int_{\mathbb{R}} f^y(x) dx \, dy = \sum_{n=0}^\infty \int_n^{n+1} (a_n - a_{n-1}) dy \\ &= \sum_{n=0}^\infty (a_n - a_{n-1}) = \sum_{k=0}^\infty b_k = s. \end{align*}\]
(c) Show that \(\iint_{\mathbb{R}} |f(x, y)| \, dx \, dy = \infty\)
proof
① \(g(x, y) \overset{\text{def}}{=} |f(x, y)|\) is measurable
Let \(g(x, y) = |f(x, y)|\).
For \(n \le y < n+2\),
\[
g(x, y) =
\begin{cases}
a_n, & n \le y < n+2 \\
0, & \text{o.w.}
\end{cases}
\quad (n \ge 0)
\]
For \(a' \in [a_n,
a_{n+1})\),
\(\{ g > a' \} = \bigcup_{k=n}^\infty
\{ g = a_k \}
= \bigcup_{k=n}^\infty ([k, k+1) \times [k, k+2))\).
\(\{ g = a_k \}\) is a product of
two measurable sets \([k, k+1)\) and
\([k, k+2)\),
so \(\{ g = a_k \}\) is measurable, as
well as \(\{ g > a' \}\).
If \(a < 0\), \(\{ g > a \} = \mathbb{R}^2\), which is
measurable.
Thus, \(g\) is a measurable function on
\(\mathbb{R}^2\).
② \(\int_{\mathbb{R}^2} g = \infty\)
By Tonelli’s theorem,
\[\begin{align*} \int_{\mathbb{R}^2} g &= \int_{\mathbb{R}^2} |f(x, y)| \, dy \, dx = \sum_{n=0}^\infty \int_n^{n+1} \int_{\mathbb{R}} g(x, y) \, dy \, dx \\ &= \sum_{n=0}^\infty \int_n^{n+1} 2a_n \, dx = \sum_{n=0}^\infty 2a_n \ge \sum_{n=0}^\infty 2a_0 = \infty. \end{align*}\]
18. \(f\) is a measurable finite-valued function on \([0,1]\), and \(g(x,y) = |f(x) - f(y)|\) is integrable on \([0,1] \times [0,1]\). Show that \(f(x)\) is integrable on \([0,1]\).
proof
\(g\) is integrable on \([0,1] \times [0,1]\), so \(g^y\) is integrable for a.e. \(y \in [0,1]\) (Fubini’s Thm).
Let \(y_0\) be such that \(\int_0^1 g(x, y_0) dx < \infty\).
Since \(|f(x)| - |f(y_0)| \le |f(x) - f(y_0)| = g(x, y_0) = g^{y_0}(x)\),
\[|f(x)| \le |f(y_0)| + g^{y_0}(x).\]
Then, \[\begin{align*} \int_0^1 |f(x)| dx &\le \int_0^1 |f(y_0)| dx + \int_0^1 g^{y_0}(x) dx \\ &= |f(y_0)| + \int_0^1 g^{y_0}(x) dx. \end{align*}\]
\(f\) is finite for all \(x \in [0,1]\), so \(|f(y_0)| < \infty.\)
\(g^{y_0}\) is integrable, so \(\int_0^1 g^{y_0}(x) dx < \infty.\)
Thus, \(\int_0^1 |f(x)| dx < \infty\) and \(f\) is integrable on \([0,1].\)
19. \(f\) is integrable on \(\mathbb{R}^d\), and let \(E_\alpha = \{ x \in \mathbb{R}^d : |f(x)| > \alpha \}\) for \(\alpha > 0\). Show that \[\int_{\mathbb{R}^d} |f(x)| dx = \int_0^\infty m(E_\alpha) d\alpha\]
proof
① \(\chi_{E_\alpha}\) is measurable
When \(b < 0\), \(\{ \chi_{E_\alpha} > b \} =
\mathbb{R}^d\).
When \(b \ge 1\), \(\{ \chi_{E_\alpha} > b \} =
\emptyset\).
When \(0 \le b < 1\),
\[\begin{align*}
\{ \chi_{E_\alpha} > b \} &= \{ \chi_{E_\alpha} = 1 \} \\
&= \{ x \in E_\alpha \} = \{ |f| > \alpha \} \\
&= \{ f > \alpha \} \cup \{ f < -\alpha \},
\end{align*}\] which is a union of measurable sets.
Since \(\{ \chi_{E_\alpha} > b \}\) is measurable for all \(b \in \mathbb{R}\), \(\chi_{E_\alpha}\) is measurable.
② \(\int_0^\infty m(E_\alpha) d\alpha\)
Then, \[\begin{align*} \int_0^\infty m(E_\alpha) d\alpha &= \int_0^\infty \int_{\mathbb{R}^d} \chi_{E_\alpha}(x) dx \, d\alpha \\ &= \int_{\mathbb{R}^d} \int_0^\infty \chi_{E_\alpha}(x) d\alpha \, dx \quad (\text{Tonelli’s thm}) \end{align*}\]
③ Conclusion
For given \(x \in
\mathbb{R}^d\),
\[
\chi_{E_\alpha}(x) =
\begin{cases}
1, & 0 < \alpha < |f(x)|, \\
0, & \alpha \ge |f(x)|.
\end{cases}
\]
(as a function of \(\alpha\)). Then, \[ \int_0^\infty \chi_{E_\alpha}(x) d\alpha = \int_0^{|f(x)|} 1 \, d\alpha = |f(x)|. \]
Thus, \[ \int_0^\infty m(E_\alpha) d\alpha = \int_{\mathbb{R}^d} |f(x)| dx. \]
21. \(f\) and \(g\) are measurable functions on \(\mathbb{R}^d\).
(a) Show that \(f(x - y) g(y)\) is measurable on \(\mathbb{R}^{2d}\).
proof
\(f(x - y)\) is measurable on \(\mathbb{R}^{2d}\) (Thm
2.3.9),
and \(g(y) = g(\pi_2(x, y))\) is
measurable on \(\mathbb{R}^{2d}\)
(Cor 2.3.7).
Then, \(f(x - y) g(y)\) is measurable
(Prop 1.2.7).
(b) If \(f\) and \(g\) are integrable on \(\mathbb{R}^d\), show that \(f(x - y) g(y)\) is integrable on \(\mathbb{R}^{2d}\).
proof
\(f(x - y) g(y)\) is measurable on
\(\mathbb{R}^{2d}\), as well as \(|f(x - y) g(y)|\).
Then,
\[\begin{align*} \iint_{\mathbb{R}^{2d}} |f(x - y) g(y)| \, dy \, dx &= \int_{\mathbb{R}^d} \int_{\mathbb{R}^d} |f(x - y)| |g(y)| \, dy \, dx \\ &= \int_{\mathbb{R}^d} |g(y)| \left( \int_{\mathbb{R}^d} |f(x - y)| \, dx \right) dy \\ &= \int_{\mathbb{R}^d} |f(x)| dx \int_{\mathbb{R}^d} |g(y)| dy < \infty \quad (\because f, g \in L^1). \end{align*}\]
Thus, \(f(x - y) g(y)\) is integrable.
(c) The convolution of \(f, g \in L^1\) is defined as follows:\[(f * g)(x) = \int_{\mathbb{R}^d} f(x - y) g(y) \, dy.\] Show that \(f(x - y) g(y)\) is integrable on \(\mathbb{R}^d\) a.e. \(x\).
proof
\[\begin{align*} \int |(f * g)(x)| dx &\le \int_{\mathbb{R}^d} \int_{\mathbb{R}^d} |f(x - y) g(y)| \, dy \, dx \\ &= \int_{\mathbb{R}^d} \int_{\mathbb{R}^d} |f(x - y) g(y)| \, dx \, dy < \infty \quad (\text{by (b)}). \end{align*}\]
So, \((f * g)(x) = \int f(x - y) g(y) dy
< \infty\) a.e. \(x\),
and thus \(f(x - y) g(y)\) is
integrable on \(\mathbb{R}^d\) a.e.
\(x\).
(d)-1 Show that \(f * g\) is integrable on \(\mathbb{R}^d\) when \(f, g\) are integrable:
\[ \| f * g \|_1 \le \| f \|_1 \, \| g \|_1. \]
proof
\[\begin{align*} \int |(f * g)(x)| dx &\le \int_{\mathbb{R}^d} \int_{\mathbb{R}^d} |f(x - y) g(y)| \, dy \, dx \\ &= \int_{\mathbb{R}^d} |f(x - y)| dx \, |g(y)| dy = \| f \|_1 \, \| g \|_1 < \infty. \end{align*}\]
(d)-2 Show that the equality in (d)-1 holds when \(f\) and \(g\) are non-negative.
proof
The inequality \[ \int_{\mathbb{R}^d} \int_{\mathbb{R}^d} f(x - y) g(y) \, dy \, dx \le \int_{\mathbb{R}^d} f(x - y) g(y) \, dy \, dx \] becomes an equality when \(f(x - y) g(y)\) is non-negative (Thm 2.1.11 (iv)).
24. Consider the convolution \((f * g)(x) = \int_{\mathbb{R}^d} f(x + y) g(y) \, dy \quad (x \in \mathbb{R}^d)\)
(a) Show that \(f * g\) is uniformly continuous when \(\| f \|_1 < \infty\) and \(|g| \le M\) (bounded).
proof
① \(f(x + y) g(y)\) is integrable
\[ \int_{\mathbb{R}^d} |f(x + y) g(y)| dy \le M \int_{\mathbb{R}^d} |f(x + y)| dy = M \int_{\mathbb{R}^d} |f(y)| dy = M \| f \|_1 < \infty. \]
② \(|(f * g)(x) - (f * g)(x')| \le M \| f_{x'} - f \|_1\)
For \(x, x' \in \mathbb{R}^d\),
\[\begin{align*} |(f * g)(x) - (f * g)(x')| &= \left| \int_{\mathbb{R}^d} f(x + y) g(y) dy - \int_{\mathbb{R}^d} f(x' + y) g(y) dy \right| \\ &= \left| \int_{\mathbb{R}^d} (f(x + y) - f(x' + y)) g(y) dy \right| \\ &\le \int_{\mathbb{R}^d} |f(x + y) - f(x' + y)| |g(y)| dy \\ &\le M \int_{\mathbb{R}^d} |f(x + y) - f(x' + y)| dy \quad (\because |g| \le M) \\ &= M \int_{\mathbb{R}^d} |f(y) - f(y - (x - x'))| dy \quad (\text{translation invariance}) \\ &= M \int_{\mathbb{R}^d} |f(y) - f(y - (x - x'))| dy \quad (\text{relative invariance, p.13}) \end{align*}\]
③ Conclusion
For given \(\varepsilon > 0\),
there is \(\delta_0 > 0\) such
that
\(|x - x'| < \delta_0\) implies
\(\| f_{x - x'} - f \|_1 =
\int_{\mathbb{R}^d} |f(y - (x - x')) - f(y)| dy < \varepsilon /
M\)
(\(\because f \in L^1\), Prop
2.2.5).
Then, \(|x - x'| < \delta_0\)
means \(|(f * g)(x) - (f * g)(x')| < M
\varepsilon\).
This holds for all \(\varepsilon >
0\), so \(f * g\) is
uniformly continuous.
(b) If \(g\) is integrable as well, show that \(\lim_{|x| \to \infty} (f * g)(x) = 0\)
proof
For given \(\varepsilon > 0\),
there is a simple function \(f_\varepsilon\) and \(g_\varepsilon\) such that
\(\| f - f_\varepsilon \| <
\frac{\varepsilon}{4 \| g \|_1}\) and \(\| g - g_\varepsilon \| < \frac{\varepsilon}{4
\| f_\varepsilon \|_1}\).
Then,
\[\begin{align*} |(f * g)(x)| &= \left| \int_{\mathbb{R}^d} f(x - y) g(y) dy \right| \\ &\le \int_{\mathbb{R}^d} |f(x - y) - f_\varepsilon(x - y)| |g(y)| dy + \int_{\mathbb{R}^d} |f_\varepsilon(x - y)| |g(y) - g_\varepsilon(y)| dy + \int_{\mathbb{R}^d} |f_\varepsilon(x - y) g_\varepsilon(y)| dy \\ &\le \| f - f_\varepsilon \|_1 \| g \|_1 + \| f_\varepsilon \|_1 \| g - g_\varepsilon \|_1 + \int_{\mathbb{R}^d} |f_\varepsilon(x - y) g_\varepsilon(y)| dy. \end{align*}\]
Since a simple function is integrable and has
compact support (Prop 2.21 (d)),
the last term \(\int |f_\varepsilon(x - y)
g_\varepsilon(y)| dy \to 0\) as \(|x|
\to \infty\) (by density argument).
Thus,
\[
\lim_{|x| \to \infty} (f * g)(x) = 0.
\]
②
\(|x - y| \ge |x| - |y|\), so \(\lim_{|x| \to \infty} |x - y| =
\infty\).
The simple function \(f_\varepsilon\)
is supported on a set of finite measure,
\(\lim_{|x| \to \infty} f_\varepsilon(x - y) =
0\).
So,
\[
\lim_{|x| \to \infty} \int_{\mathbb{R}^d} |f_\varepsilon(x - y)
g_\varepsilon(y)| dy = 0.
\]
③
Then,
\[
\lim_{|x| \to \infty} |(f * g)(x)|
\le \| f - f_\varepsilon \|_1 \| g \|_1 + \| f_\varepsilon \|_1 \| g -
g_\varepsilon \|_1
< 2 \varepsilon,
\]
and this holds for all \(\varepsilon >
0\). Thus,
\[
\lim_{|x| \to \infty} (f * g)(x) = 0.
\]