\sum_{n=1}^\infty \frac{n!}{n^n}x^n
\] diverges when $|x|$ is the radius of convergence $e$. In fact, we can show that \[
n!\brac{\frac{e}{n}}^n\to \infty
\] by Stirling's Formula (in the simplest form), which is the following asymptotic result:
Theorem. We have $\dis n!\sim \sqrt{2\pi n} \brac{\frac{n}{e}}^n$ as $n\to \infty$.
\limn \frac{n!}{n^{n+1/2}e^{-n}}=\sqrt{2\pi}.
\] We are going to prove this result with the help of the following simple exercises, each of them will be used exactly once.
\[\brac{\frac{n+1}{e}}^n<n!\]
f(x)=\brac{1+\frac{1}{x}}^{x+\alpha}
\] is decreasing on $(0,\infty)$ when $\alpha \ge1/2$.
Problem 3. If $f:(a,b)\to \R$ is convex, then show that for every $x_1,x_2\in (a,b)$ with $x_1<x_2$, one has \[
f\brac{\frac{x_1+x_2}{2}}\leq \frac{1}{x_2-x_1}\int_{x_1}^{x_2}f(t)\,dt\leq \frac{f(x_1)+f(x_2)}{2}.
\]
I_{2n}=\frac{(2n-1)!!}{(2n)!!}\cdot \frac{\pi}{2}\quad\text{and}\quad I_{2n+1}=\frac{(2n)!!}{(2n+1)!!}.
\] Hence by considering $I_{2n}/I_{2n+1}$, show that \[
\limn \frac{1}{2n+1}\brac{\frac{(2n)!!}{(2n-1)!!}}^2=\frac{\pi}{2}.
\]
Motivation:
By problem 1 we have\[\brac{1+\frac{1}{n}}^n<\frac{e^nn!}{n^n}.
\] We note that LHS increases to $e$, thus if $\dis b_n:=\frac{e^nn!}{n^n}$ also converges, we should get at least a nonzero limit. To study this, consider the quotient \[
\frac{b_{n+1}}{b_n}=e\brac{\frac{n}{n+1}}^n\iff \frac{b_{n}}{b_{n+1}}=\frac{1}{e}\brac{1+\frac{1}{n}}^n<1.
\] Therefore $\{b_n\}$ is increasing, however this limit is possibly unbounded. On the other hand, we observe that by problem 2 we can obtain a decreasing sequence by multiplying $b_n/b_{n+1}$ a factor $\dis \brac{1+\frac{1}{n}}^{1/2}=\frac{\sqrt{n+1}}{\sqrt{n}}$, namely, \[
\frac{b_n/\sqrt{n}}{b_{n+1}/\sqrt{n+1}}=\frac{1}{e}\brac{1+\frac{1}{n}}^{n+1/2}>1.
\] So instead we try to compute the limit of \[
\boxed{\dis a_n:=\frac{b_n}{\sqrt{n}}=\frac{e^nn!}{n^{n+1/2}}}
\] as at least this limit must not be unbounded.
Proof to Stirling Formula:
Now observe that \begin{align*}1&<\frac{a_n}{a_{n+1}}=e^{-1}\brac{1+\frac{1}{n}}^{n+1/2}=\exp\bigg(-1+\Big(n+\frac{1}{2}\Big) \int_{n}^{n+1}\frac{1}{x}\,dx\bigg),
\end{align*} by problem 3 we have $\dis \int_{n}^{n+1}\frac{1}{x}\,dx\leq\frac{1}{2}\brac{\frac{1}{n}+\frac{1}{n+1}}$, therefore a simple computation yields \[
1<\frac{a_n}{a_{n+1}}<e^{\frac{1}{4}\brac{\frac{1}{n}-\frac{1}{n+1}}}.
\] Thus the first inequality tells us $\{a_n\}$ converges to a nonnegative limit $\boxed{\alpha:=\limn a_n}$. On the other hand, the second inequality tell us $\{a_ne^{-\frac{1}{4n}}\}$ increases to $\alpha$, so $\alpha >0$. By using the following form of Walli's formula (modified from problem 4) \[
\frac{(n!)^2 2^{2n}}{(2n)!}\sim \sqrt{\pi n}
\] and using $n!=a_nn^{n+1/2}e^{-n}$ we get \[
\sqrt{\pi}\leftarrow \frac{(n!)^22^{2n}}{\sqrt{n}(2n)!}=\frac{1}{\sqrt{2}} \frac{a_n^2}{a_{2n}}\to \frac{\alpha}{\sqrt{2}}.
\] Therefore we conclude that \[
\limn \frac{n!}{n^{n+1/2} e^{-n}}=\limn a_n=\alpha =\sqrt{2\pi}.\qed
\] For the ease of memorization this result is usually written as \[
\boxed{\dis n!\sim \sqrt{2\pi n} \brac{\frac{n}{e}}^n.}
\]
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