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Section 11.2 Swapping limits

Note: 2 lectures

Subsection 11.2.1 Continuity

Let us get back to swapping limits and expand on Chapter 6. Let \(\{ f_n \}_{n=1}^\infty\) be a sequence of functions \(f_n \colon X \to Y\) for a set \(X\) and a metric space \(Y\text{.}\) Let \(f \colon X \to Y\) be a function and for every \(x \in X\text{,}\) suppose
\begin{equation*} f(x) = \lim_{n\to \infty} f_n(x) . \end{equation*}
We say the sequence \(\{ f_n \}_{n=1}^\infty\) converges pointwise to \(f\text{.}\)
For \(Y=\C\text{,}\) a series of functions converges pointwise to \(f\) if for every \(x \in X\text{,}\) we have
\begin{equation*} f(x) = \lim_{n\to \infty} \sum_{k=1}^n f_k(x) = \sum_{k=1}^\infty f_k(x) . \end{equation*}
The question is: If \(f_n\) are all continuous, is \(f\) continuous? Differentiable? Integrable? What are the derivatives or integrals of \(f\text{?}\) For example, for continuity of the pointwise limit of a sequence of functions \(\{ f_n \}_{n=1}^\infty\text{,}\) we are asking if
\begin{equation*} \lim_{x\to x_0} \lim_{n\to\infty} f_n(x) \overset{?}{=} \lim_{n\to\infty} \lim_{x\to x_0} f_n(x) . \end{equation*}
A priori, we do not even know if both sides exist, let alone if they equal each other.

Example 11.2.1.

The functions \(f_n \colon \R \to \R\text{,}\)
\begin{equation*} f_n(x) \coloneqq \frac{1}{1+nx^2}, \end{equation*}
are continuous and converge pointwise to the discontinuous function
\begin{equation*} f(x) \coloneqq \begin{cases} 1 & \text{if } x=0, \\ 0 & \text{else.} \end{cases} \end{equation*}
So pointwise convergence is not enough to preserve continuity (nor even boundedness). For that, we need uniform convergence. Let \(f_n \colon X \to Y\) be functions. Then \(\{f_n\}_{n=1}^\infty\) converges uniformly to \(f\) if for every \(\epsilon > 0\text{,}\) there exists an \(M\) such that for all \(n \geq M\) and all \(x \in X\text{,}\) we have
\begin{equation*} d\bigl(f_n(x),f(x)\bigr) < \epsilon . \end{equation*}
A series \(\sum_{n=1}^\infty f_n\) of complex-valued functions converges uniformly if the sequence of partial sums converges uniformly, that is, if for every \(\epsilon > 0\text{,}\) there exists an \(M\) such that for all \(n \geq M\) and all \(x \in X\text{,}\)
\begin{equation*} \abs{\left(\sum_{k=1}^n f_k(x)\right)-f(x)} < \epsilon . \end{equation*}
The simplest property preserved by uniform convergence is boundedness. We leave the proof of the following proposition as an exercise. It is almost identical to the proof for real-valued functions.
If \(X\) is a set and \((Y,d)\) is a metric space, then a sequence \(f_n \colon X \to Y\) is uniformly Cauchy if for every \(\epsilon > 0\text{,}\) there is an \(M\) such that for all \(n, m \geq M\) and all \(x \in X\text{,}\) we have
\begin{equation*} d\bigl(f_n(x),f_m(x)\bigr) < \epsilon . \end{equation*}
The notion is the same as for real-valued functions. The proof of the following proposition is again essentially the same as in that setting and is left as an exercise.
For \(f \colon X \to \C\text{,}\) we write
\begin{equation*} \snorm{f}_X \coloneqq \sup_{x \in X} \sabs{f(x)} . \end{equation*}
We call \(\snorm{\cdot}_X\) the supremum norm or uniform norm, and the subscript denotes the set over which the supremum is taken. Then a sequence of functions \(f_n \colon X \to \C\) converges uniformly to \(f \colon X \to \C\) if and only if
\begin{equation*} \lim_{n\to \infty} \snorm{f_n-f}_X = 0 . \end{equation*}
The supremum norm satisfies the triangle inequality: For every \(x \in X\text{,}\)
\begin{equation*} \sabs{f(x)+g(x)} \leq \sabs{f(x)}+\sabs{g(x)} \leq \snorm{f}_X+\snorm{g}_X . \end{equation*}
Take a supremum on the left to get
\begin{equation*} \snorm{f+g}_X \leq \snorm{f}_X+\snorm{g}_X . \end{equation*}
For a compact metric space \(X\text{,}\) the uniform norm is a norm on the vector space \(C(X,\C)\text{.}\) We leave it as an exercise. While we will not need it, \(C(X,\C)\) is in fact a complex vector space, that is, in the definition of a vector space we can replace \(\R\) with \(\C\text{.}\) Convergence in the metric space \(C(X,\C)\) is uniform convergence.
We will study a couple of types of series of functions, and a useful test for uniform convergence of a series is the so-called Weierstrass \(M\)-test.
Another way to state the theorem is to say that if \(\sum_{n=1}^\infty \snorm{f_n}_X\) converges, then \(\sum_{n=1}^\infty f_n\) converges uniformly. Note that the converse of this theorem is not true. Applying the theorem to \(\sum_{n=1}^\infty \sabs{f_n(x)}\text{,}\) we see that this series also converges uniformly. So the series converges both absolutely and uniformly.

Proof.

Suppose \(\sum_{n=1}^\infty M_n\) converges. Given \(\epsilon > 0\text{,}\) we have that the partial sums of \(\sum_{n=1}^\infty M_n\) are Cauchy so there is an \(N\) such that for all \(m, n \geq N\) with \(m \geq n\text{,}\) we have
\begin{equation*} \sum_{k=n+1}^m M_k < \epsilon . \end{equation*}
We estimate a Cauchy difference of the partial sums of the functions
\begin{equation*} \abs{\sum_{k=n+1}^m f_k(x)} \leq \sum_{k=n+1}^m \sabs{f_k(x)} \leq \sum_{k=n+1}^m M_k < \epsilon . \end{equation*}
The series converges by Proposition 11.1.4. The convergence is uniform, as \(N\) does not depend on \(x\text{.}\) Indeed, for all \(n \geq N\text{,}\)
\begin{equation*} \abs{\sum_{k=1}^\infty f_k(x) - \sum_{k=1}^n f_k(x)} \leq \abs{\sum_{k=n+1}^\infty f_k(x)} \leq \epsilon . \qedhere \end{equation*}

Example 11.2.5.

The series
\begin{equation*} \sum_{n=1}^\infty \frac{\sin(nx)}{n^2} \end{equation*}
converges uniformly on \(\R\text{.}\) See Figure 11.2. This series is a Fourier series, and we will see more of these in a later section. Proof: The series converges uniformly because \(\sum_{n=1}^\infty \frac{1}{n^2}\) converges and
\begin{equation*} \abs{\frac{\sin(nx)}{n^2}} \leq \frac{1}{n^2} . \end{equation*}

Figure 11.2. Plot of \(\sum_{n=1}^\infty \frac{\sin(n x)}{n^2}\) including the first 8 partial sums in various shades of gray.

Example 11.2.6.

The series
\begin{equation*} \sum_{n=0}^\infty \frac{x^n}{n!} \end{equation*}
converges uniformly on every bounded interval. This series is a power series that we will study shortly. Proof: Take the interval \([-r,r] \subset \R\) (every bounded interval is contained in some \([-r,r]\)). The series \(\sum_{n=0}^\infty \frac{r^n}{n!}\) converges by the ratio test, so \(\sum_{n=0}^\infty \frac{x^n}{n!}\) converges uniformly on \([-r,r]\) as
\begin{equation*} \abs{\frac{x^n}{n!} } \leq \frac{r^n}{n!} . \end{equation*}
Now we would love to say something about the limit. For example, is it continuous?
In other words,
\begin{equation*} \lim_{k \to \infty} \lim_{n\to\infty} f_n(x_k) = \lim_{n \to \infty} \lim_{k\to\infty} f_n(x_k) . \end{equation*}

Proof.

First we show that \(\{ a_n \}_{n=1}^\infty\) converges. As \(\{ f_n \}_{n=1}^\infty\) converges uniformly it is uniformly Cauchy. Let \(\epsilon > 0\) be given. There is an \(M\) such that for all \(m,n \geq M\text{,}\) we have
\begin{equation*} d_Y\bigl(f_n(x_k),f_m(x_k)\bigr) < \epsilon \qquad \text{for all } k . \end{equation*}
Note that \(d_Y(a_n,a_m) \leq d_Y\bigl(a_n,f_n(x_k)\bigr) + d_Y\bigl(f_n(x_k),f_m(x_k)\bigr) + d_Y\bigl(f_m(x_k),a_m\bigr)\) and take the limit as \(k \to \infty\) to find
\begin{equation*} d_Y(a_n,a_m) \leq \epsilon . \end{equation*}
Hence \(\{a_n\}_{n=1}^\infty\) is Cauchy and converges since \(Y\) is complete. Write \(a \coloneqq \lim_{k \to \infty} a_n\text{.}\)
Find a \(k \in \N\) such that
\begin{equation*} d_Y\bigl(f_k(p),f(p)\bigr) < \nicefrac{\epsilon}{3} \end{equation*}
for all \(p \in X\text{.}\) Assume \(k\) is large enough so that
\begin{equation*} d_Y(a_k,a) < \nicefrac{\epsilon}{3} . \end{equation*}
Find an \(N \in \N\) such that for \(m \geq N\text{,}\)
\begin{equation*} d_Y\bigl(f_k(x_m),a_k\bigr) < \nicefrac{\epsilon}{3} . \end{equation*}
Then for \(m \geq N\text{,}\)
\begin{equation*} d_Y\bigl(f(x_m),a\bigr) \leq d_Y\bigl(f(x_m),f_k(x_m)\bigr) + d_Y\bigl(f_k(x_m),a_k\bigr) + d_Y\bigl(a_k,a\bigr) < \nicefrac{\epsilon}{3} + \nicefrac{\epsilon}{3} + \nicefrac{\epsilon}{3} = \epsilon . \qedhere \end{equation*}
We obtain an immediate corollary about continuity. If \(f_n\) are all continuous then \(a_n = f_n(x)\) and so \(\{ a_n \}_{n=1}^\infty\) converges automatically to \(f(x)\) and so we do not require completeness of \(Y\text{.}\)
The converse is not true. Just because the limit is continuous does not mean that the convergence is uniform. For example: \(f_n \colon (0,1) \to \R\) defined by \(f_n(x) \coloneqq x^n\) converge to the zero function, but not uniformly. However, if we add extra conditions on the sequence, we can obtain a partial converse such as Dini’s theorem, see Exercise 6.2.10.
In Exercise 11.2.3 the reader is asked to prove that for a compact \(X\text{,}\) \(C(X,\C)\) is a normed vector space with the uniform norm, and hence a metric space. We have just shown that \(C(X,\C)\) is Cauchy-complete: Proposition 11.2.3 says that a Cauchy sequence in \(C(X,\C)\) converges uniformly to some function, and Corollary 11.2.8 shows that the limit is continuous and hence in \(C(X,\C)\text{.}\)

Example 11.2.10.

By Example 11.2.5 the Fourier series
\begin{equation*} \sum_{n=1}^\infty \frac{\sin(nx)}{n^2} \end{equation*}
converges uniformly and hence is continuous by Corollary 11.2.8 (as is visible in Figure 11.2).

Subsection 11.2.2 Integration

Since the integral of a complex-valued function is just the integral of the real and imaginary parts separately, the proof follows directly by the results of Chapter 6. We leave the details as an exercise.

Example 11.2.13.

Let us show how to integrate a Fourier series.
\begin{equation*} \int_{0}^x \sum_{n=1}^\infty \frac{\cos(nt)}{n^2} \,dt = \sum_{n=1}^\infty \int_{0}^x \frac{\cos(nt)}{n^2}\,dt = \sum_{n=1}^\infty \frac{\sin(nx)}{n^3} \end{equation*}
The swapping of integral and sum is possible because of uniform convergence, which we have proved before using the Weierstrass \(M\)-test (Theorem 11.2.4).
We remark that we can swap integrals and limits under far less stringent hypotheses, but for that we would need a stronger integral than the Riemann integral. E.g. the Lebesgue integral.

Subsection 11.2.3 Differentiation

Recall that a complex-valued function \(f \colon [a,b] \to \C\text{,}\) where \(f(x) = u(x)+i\,v(x)\text{,}\) is differentiable, if \(u\) and \(v\) are differentiable and the derivative is
\begin{equation*} f'(x) = u'(x)+i\,v'(x) . \end{equation*}
The proof of the following theorem is to apply the corresponding theorem for real functions to \(u\) and \(v\text{,}\) and is left as an exercise.
Uniform limits of the functions themselves are not enough, and can make matters even worse. In Section 11.7 we will prove that continuous functions are uniform limits of polynomials, yet as the following example demonstrates, a continuous function need not be differentiable anywhere.

Example 11.2.15.

There exist continuous nowhere differentiable functions. Such functions are often called Weierstrass functions, although this particular one, essentially due to Takagi
 1 
Teiji Takagi (1875–1960) was a Japanese mathematician.
, is a different example than what Weierstrass gave. Define
\begin{equation*} \varphi(x) \coloneqq \sabs{x} \qquad \text{for } x \in [-1,1] . \end{equation*}
Extend \(\varphi\) to all of \(\R\) by making it 2-periodic: Decree that \(\varphi(x) = \varphi(x+2)\text{.}\) The function \(\varphi \colon \R \to \R\) is continuous, in fact, \(\sabs{\varphi(x)-\varphi(y)} \leq \sabs{x-y}\) (why?). See Figure 11.3.

Figure 11.3. The 2-periodic function \(\varphi\text{.}\)

As \(\sum_{n=0}^\infty {\left(\frac{3}{4}\right)}^n\) converges and \(\sabs{\varphi(x)} \leq 1\) for all \(x\text{,}\) by the \(M\)-test (Theorem 11.2.4),
\begin{equation*} f(x) \coloneqq \sum_{n=0}^\infty {\left(\frac{3}{4}\right)}^n \varphi(4^n x) \end{equation*}
converges uniformly and hence is continuous. See Figure 11.4.

Figure 11.4. Plot of the nowhere differentiable function \(f\text{.}\)

We claim \(f \colon \R \to \R\) is nowhere differentiable. Fix \(x\text{,}\) and we will show \(f\) is not differentiable at \(x\text{.}\) Define
\begin{equation*} \delta_m \coloneqq \pm \frac{1}{2} 4^{-m} , \end{equation*}
where the sign is chosen so that there is no integer between \(4^m x\) and \(4^m(x+\delta_m) = 4^m x \pm \frac{1}{2}\text{.}\)
We want to look at the difference quotient
\begin{equation*} \frac{f(x+\delta_m)-f(x)}{\delta_m} = \sum_{n=0}^\infty {\left(\frac{3}{4}\right)}^n \frac{\varphi\bigl(4^n(x+\delta_m)\bigr)-\varphi(4^nx)}{\delta_m} . \end{equation*}
Fix \(m\) for a moment. Consider the expression inside the series:
\begin{equation*} \gamma_{n} \coloneqq \frac{\varphi\bigl(4^n(x+\delta_m)\bigr)-\varphi(4^nx)}{\delta_m} . \end{equation*}
If \(n > m\text{,}\) then \(4^n\delta_m\) is an even integer. As \(\varphi\) is 2-periodic we get that \(\gamma_n = 0\text{.}\)
As there is no integer between \(4^m(x+\delta_m) = 4^m x\pm\nicefrac{1}{2}\) and \(4^m x\text{,}\) then on this interval \(\varphi(t) = \pm t + \ell\) for some integer \(\ell\text{.}\) In particular, \(\abs{\varphi\bigl(4^m(x+ \delta_m)\bigr)-\varphi(4^mx)} = \abs{4^mx\pm\nicefrac{1}{2}-4^mx} = \nicefrac{1}{2}\text{.}\) Therefore,
\begin{equation*} \sabs{\gamma_m} = \abs{ \frac{\varphi\bigl(4^m(x+\delta_m)\bigr)-\varphi(4^mx)}{\pm (\nicefrac{1}{2}) 4^{-m}} } = 4^m . \end{equation*}
Similarly, suppose \(n < m\text{.}\) Since \(\sabs{\varphi(s) -\varphi(t)} \leq \sabs{s-t}\text{,}\)
\begin{equation*} \sabs{\gamma_n} = \abs{\frac{\varphi\bigl(4^nx\pm(\nicefrac{1}{2})4^{n-m}\bigr)-\varphi(4^nx)}{\pm (\nicefrac{1}{2}) 4^{-m}}} \leq \abs{\frac{\pm(\nicefrac{1}{2})4^{n-m}}{\pm (\nicefrac{1}{2}) 4^{-m}}} = 4^n . \end{equation*}
And so
\begin{equation*} \begin{split} \abs{ \frac{f(x+\delta_m)-f(x)}{\delta_m} } = \abs{ \sum_{n=0}^\infty {\left(\frac{3}{4}\right)}^n \gamma_n } & = \abs{ \sum_{n=0}^m {\left(\frac{3}{4}\right)}^n \gamma_n } \\ & \geq \abs{ {\left(\frac{3}{4}\right)}^m \gamma_m} - \abs{ \sum_{n=0}^{m-1} {\left(\frac{3}{4}\right)}^n \gamma_n } \\ & \geq 3^m - \sum_{n=0}^{m-1} 3^n = 3^m - \frac{3^{m}-1}{3-1} = \frac{3^m +1}{2} . \end{split} \end{equation*}
As \(m \to \infty\text{,}\) we have \(\delta_m \to 0\text{,}\) but \(\frac{3^m+1}{2}\) goes to infinity. So \(f\) cannot be differentiable at \(x\text{.}\)

Exercises 11.2.4 Exercises

11.2.3.

Suppose \((X,d)\) is a compact metric space. Prove that the uniform norm \(\snorm{\cdot}_X\) is a norm on the vector space of continuous complex-valued functions \(C(X,\C)\text{.}\)

11.2.4.

  1. Prove that \(f_n(x) \coloneqq 2^{-n} \sin(2^n x)\) converge uniformly to zero, but there exists a dense set \(D \subset \R\) such that \(\lim_{n\to\infty} f_n'(x) = 1\) for all \(x \in D\text{.}\)
  2. Prove that \(\sum_{n=1}^\infty 2^{-n} \sin(2^n x)\) converges uniformly to a continuous function, and there exists a dense set \(D \subset \R\) where the derivatives of the partial sums do not converge.

11.2.5.

Prove that \(\snorm{f}_{C^1} \coloneqq \snorm{f}_{[a,b]}+\snorm{f'}_{[a,b]}\) is a norm on the vector space of continuously differentiable complex-valued functions \(C^1\bigl([a,b],\C\bigr)\text{.}\)

11.2.8.

Work through the following counterexample to the converse of the Weierstrass \(M\)-test (Theorem 11.2.4). Define \(f_n \colon [0,1] \to \R\) by
\begin{equation*} f_n(x) \coloneqq \begin{cases} \frac{1}{n} & \text{if } \frac{1}{n+1} < x < \frac{1}{n},\\ 0 & \text{else.} \end{cases} \end{equation*}
Prove that \(\sum_{n=1}^\infty f_n\) converges uniformly, but \(\sum_{n=1}^\infty \snorm{f_n}_{[0,1]}\) does not converge.

11.2.9.

Suppose \(f_n \colon [0,1] \to \R\) are monotone increasing functions and suppose that \(\sum_{n=1}^\infty f_n\) converges pointwise. Prove that \(\sum_{n=1}^\infty f_n\) converges uniformly.

11.2.10.

Prove that
\begin{equation*} \sum_{n=1}^\infty e^{-nx} \end{equation*}
converges for all \(x > 0\) to a differentiable function.
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