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@@ -113,6 +113,8 @@ \section*{Math 202A - Final Exam - Dan Davison - \texttt{[email protected]}} | |
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I think that's not possible and therefore a contradiction proving that $f_n \to f$ almost everywhere. | ||
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(No, this is wrong -- see above) | ||
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One might think that the sequences $f_n(x)$ for $x \in E$ could contrive to, at every generation $n$, almost | ||
all be exactly equal to $f(x)$, except for a negligible set, with membership of this negligible set changing | ||
over time such that every $x \in E$ will at some point in the future be a member of the error set again, in | ||
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@@ -149,43 +151,79 @@ \section*{Math 202A - Final Exam - Dan Davison - \texttt{[email protected]}} | |
% But bringing the limit inside is justified by neither MCT nor DCT. So let's look for a counter-example based | ||
% on not satisfying DCT conditions. | ||
% \end{proof} | ||
I think my proof is put on a slightly firmer basis if I say at the outset that the syntax $e^{-x}$ | ||
is defined to mean the Maclaurin expansion: $e^{-x} := \sum_{j=0}^\infty (-1)^j ~ \frac{x^j}{j!}$. | ||
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\begin{mdframed} | ||
\includegraphics[width=400pt]{img/analysis--berkeley-202a-final-5921.png} | ||
\end{mdframed} | ||
\begin{lemma}\label{gamma-function} | ||
Define Euler's gamma function $\Gamma: \R \to \R$ | ||
by $\Gamma(y + 1) = \int_0^\infty x^y e^{-x} \dx$ and note that integration by parts | ||
(with $u = x^n$, $\dvdx = e^{-x}$) yields | ||
\begin{align*} | ||
\Gamma(y + 1) | ||
&= \big[-x^ye^{-x}\big]_0^\infty + y\int_0^\infty x^{y-1}e^{-x} \dx \\ | ||
&= y\Gamma(y), | ||
\end{align*} | ||
since $x^ye^{-x} \to 0$ as $x \to \infty$. | ||
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Note that $\Gamma(1) = \int_0^\infty e^{-x} \dx = 1$, and therefore $\Gamma(n + 1) = n!$ | ||
for $n \in \N$. (Since these are continuous functions, Lebesgue and Riemann integrals coincide | ||
and we freely use standard results for antiderivatives and derivatives from introductory | ||
calculus). | ||
\end{lemma} | ||
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\begin{lemma}\label{exponential-limit} | ||
$(1 - x/k)^k < e^{-x}$ for all $k \in \N$ and all $x \in \R$ | ||
and $\lim_{k \to \infty} \(1 - \frac{x}{k}\)^k = e^{-x}$. | ||
\end{lemma} | ||
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\begin{proof} | ||
Recall the Maclaurin expansion $e^{-x} = \sum_{j=0}^\infty (-1)^j ~ \frac{x^j}{j!}$ and observe that | ||
\begin{align*} | ||
\(1 - \frac{x}{k}\)^k | ||
&= \sum_{j=0}^k {k \choose j} \(\frac{-x}{k}\)^j \\ | ||
&= \sum_{j=0}^k (-1)^j \frac{x^j}{j!} \(\frac{k!/(k-j)!}{k^j} \) \\ | ||
& <\sum_{j=0}^k (-1)^j \frac{x^j}{j!}. | ||
\end{align*} | ||
Therefore $(1 - x/k)^k < e^{-x}$ for all $k \in \N$ and all $x \in \R$. | ||
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Furthermore we have | ||
\begin{align*} | ||
\lim_{k \to \infty} \(1 - \frac{x}{k}\)^k | ||
&= \sum_{j=0}^\infty (-1)^j \frac{x^j}{j!} \(\lim_{k \to \infty} \frac{k!/(k-j)!}{k^j} \). | ||
\end{align*} | ||
Note that | ||
\begin{align*} | ||
\lim_{k \to \infty} \frac{k!/(k-j)!}{k^j} | ||
&= \lim_{k \to \infty} \frac{k (k - 1) (k - 2) \cdots (k - (j - 1))}{k^j} \\ | ||
&= \lim_{k \to \infty} \frac{k^j (1 - k^{-1}) (k - 2k^{-1}) \cdots (1 - (j - 1)k^{-1})}{k^j} \\ | ||
&= 1, | ||
\end{align*} | ||
therefore $\lim_{k \to \infty} \(1 - \frac{x}{k}\)^k = e^{-x}$. | ||
\end{proof} | ||
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\begin{mdframed} | ||
\includegraphics[width=400pt]{img/analysis--berkeley-202a-final-96cc.png} | ||
\end{mdframed} | ||
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\begin{proof} | ||
\red{TODO} | ||
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Note that the integrand is non-negative. | ||
\green{DONE} | ||
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We want a dominating function. What about $x^ne^{-x/2}$? Is this integrable? It's continuous so we can use | ||
traditional Riemann / high-school integration techniques. I think it can be done by integration py parts and | ||
induction/recurrence. | ||
We may apply the dominated convergence theorem, since the integrand $x^n (1 - x/k)^k$ is | ||
non-negative and by lemma \ref{exponential-limit} is bounded above by $x^ne^{-x}$ which as shown | ||
in lemma \ref{gamma-function} is integrable. | ||
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We may apply the DCT since the integrand is non-negative and bounded above by the integrable | ||
function $x^ne^{-x/2}$. Therefore | ||
Therefore | ||
\begin{align*} | ||
\lim_{k \to \infty} \int_0^k x^n (1 - x/k)^k \dx | ||
&= \int_0^k x^n \lim_{k \to \infty} (1 - x/k)^k \dx \\ | ||
&= \int_0^k x^n e^{-x} \dx \\ | ||
&= \lim_{k \to \infty} \int_0^\infty x^n (1 - x/k)^k\ind_{[0, k]} \dx \\ | ||
&= \int_0^\infty x^n \lim_{k \to \infty} (1 - x/k)^k\ind_{[0, k]} \dx & \text{by the dominated convergence theorem}\\ | ||
&= \int_0^\infty x^n e^{-x} \dx & \text{by lemma \ref{exponential-limit}}\\ | ||
&=: \Gamma(n + 1) \\ | ||
&= n! & \text{by lemma \ref{gamma-function}}.\\ | ||
\end{align*} | ||
\red{TODO} how am I dealing with the $k$ in the upper integral bound? This is reminiscent of HW8 7.13 (above) | ||
\end{proof} | ||
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% \begin{minted}{wolfram} :results latex | ||
% Integrate[x^n * Exp[-x/2], {x, 0, Infinity}] | ||
% \end{minted} | ||
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% \begin{align*} | ||
% \text{ConditionalExpression}\left[2^{n+1} \Gamma (n+1),\Re(n)>-1\right] | ||
% \end{align*} | ||
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\red{TODO: What did this have to do with part (a)?} | ||
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\begin{mdframed} | ||
\includegraphics[width=400pt]{img/analysis--berkeley-202a-final-c137.png} | ||
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@@ -522,8 +560,36 @@ \section*{Math 202A - Final Exam - Dan Davison - \texttt{[email protected]}} | |
\includegraphics[width=400pt]{img/analysis--berkeley-202a-final-8aed.png} | ||
\end{mdframed} | ||
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This question involves an averaging construction similar to that associated with Hardy-Littlewood maximal | ||
function theory and the Lebesgue differentiation theorem (Folland section 3.4). However, the theory in Folland | ||
3.4 concerns $\R^n$, whereas this question is about an abstract measure space. It doesn't look like extensions | ||
of that theory to abstract measure spaces are well-known, or at least not standard graduate-level material. | ||
Wikipedia (\url{https://en.wikipedia.org/wiki/Lebesgue_differentiation_theorem}) mentions that the Lebesgue differentiation theorem holds for a | ||
``finite Borel measure on a separable metric space'' obeying certain conditions and references Federer 1969, but | ||
we don't have that. | ||
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We are however given a finite measure space $\mu(X) < \infty$; that may be a clue. Also we have a measurable | ||
function to $\R \union \{\infty\}$. I wonder whether we can transfer some of the results over from $\R^n$ | ||
somehow. | ||
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\begin{proof} | ||
\red{TODO} (partial) | ||
\red{TODO} | ||
If $\mu(X) = 0$ then the result is trivially true so we assume $\mu(X) > 0$. | ||
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We would like to show that for almost every $x$ a sequence of sets $E_n$ exists, each of positive measure, | ||
such that $A_{E_n}(f) \to f(x)$. Then, since $S$ is closed, it contains the limit of every convergent | ||
sequence in $S$, and hence we would have $f(x) \in S$ for every $x \in X$. | ||
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\begin{itemize} | ||
\item We must use that $\mu(X) < \infty$. | ||
\item We must use that $\int |f| \dmu < \infty$. | ||
\item We are asked only for almost every $x \in X$ | ||
\end{itemize} | ||
\end{proof} | ||
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\begin{proof} | ||
\red{TODO} No, this is wrong. The measure space is not necessarily $\R^n$. | ||
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Since $f$ is integrable, it is locally integrable. So from Folland 3.18 we have | ||
that $\lim_{r \to 0} A_{B(x, r)}(f) = f(x)$ for a.e. $x \in \R$. Let $x$ be such a point and | ||
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@@ -537,4 +603,4 @@ \section*{Math 202A - Final Exam - Dan Davison - \texttt{[email protected]}} | |
\red{TODO} However, what we need to address is that $A_{\{x\}}(f)$ is not defined, since $\mu(\{x\}) = 0$. It | ||
certainly seems plausible that $A_{I^{(x)}_n} \to f(x)$, but we need to prove it. Perhaps this is related to | ||
Lebesgue density results. | ||
\end{proof} | ||
\end{proof} |