From 15cd12e43218d63b874022ae13e87b9a6d98aa31 Mon Sep 17 00:00:00 2001 From: Zheyuan Wu <60459821+Trance-0@users.noreply.github.com> Date: Thu, 27 Mar 2025 12:58:15 -0500 Subject: [PATCH] Update Math416_L19.md --- pages/Math416/Math416_L19.md | 67 +++++++++++++++++++++++++++++++++++- 1 file changed, 66 insertions(+), 1 deletion(-) diff --git a/pages/Math416/Math416_L19.md b/pages/Math416/Math416_L19.md index fa5ad16..2cc76f3 100644 --- a/pages/Math416/Math416_L19.md +++ b/pages/Math416/Math416_L19.md @@ -72,6 +72,8 @@ the singularity at $z=3$ is a simple pole with order 1 $f(z)=\frac{z+1}{z-3}=\fr there are three poles at $z=1,5,8$, the order of the poles are 2, 6, 1 respectively. +#### Corollary: order of poles and zeros + If $f$ has a pole of order $m$ at $z_0$, $$ @@ -83,8 +85,71 @@ then $(z-z_0)^m f(z)$ has a removable singularity at $z_0$. Value of holomorphic - $f$ is given by a power series in $A(z_0;0,R)$ - $f=(z-z_0)^{-m} g(z)$ where $g$ is holomorphic and $g(z_0)\neq 0$, $\frac{1}{f}=(z-z_0)^m \frac{1}{g(z)}$ has a pole of order $m$ at $z_0$. So $f$ has a pole of order $m$ at $z_0$ if and only if $\frac{1}{f}$ has a zero of order $m$ at $z_0$ -$e^{1/z}=1+\frac{1}{z}+\frac{1}{2!z^2}+\frac{1}{3!z^3}+\cdots$ has an essential singularity at $z=0$ since it has infinitely many terms with negative powers of $z$. +> $e^{1/z}=1+\frac{1}{z}+\frac{1}{2!z^2}+\frac{1}{3!z^3}+\cdots$ has an essential singularity at $z=0$ since it has infinitely many terms with negative powers of $z$. +Suppose $f$ is a holomorphic in a neighborhood of $\infty$: $\exists R>0$ s.t. $f$ is holomorphic on $\{z:|z|>R\}$ +We defined $g(z)=f(1/z)$ where $g$ is holomorphic on punctured disk center $0$ radius $1/R$ +Say $f(z)$ has a zero of order $\infty$ if any only if $g(z)=f(1/z)$ has a zero of order $m$ at $z=0$ +Say $f$ has a pole of order $m$ at $\infty$ if and only if $g(z)=f(1/z)$ has a pole of order $m$ at $z=0$ + +Example: + +1. $f(z)=z^2$, $g(z)=f(1/z)=1/z^2$ has a pole of order 2 at $z=0$ +2. $f(z)=\frac{1}{z^3}$ (vanishes to order 3 at $\infty$), $g(z)=f(1/z)=z^3$ has a zero of order 3 at $z=0$ + +We say $f$ has an isolated singularity at $\infty$ if and only if $g(z)=f(1/z)$ has an isolated singularity at $z=0$. + +$f$ has $\begin{cases} + \text{removable}\\ + \text{pole of order } m\\ + \text{essential} +\end{cases}$ singularity at $\infty$ if and only if $g(z)=f(1/z)$ has $\begin{cases} + \text{removable}\\ + \text{pole of order } m\\ + \text{essential} +\end{cases}$ singularity at $z=0$ + +#### Theorem: Criterion for a removable singularity (Riemann removable singularity theorem) + +Suppose $f$ has an isolated singularity at $z_0$. Then it is removable if and only if $f$ is bounded on a punctured disk centered at $z_0$. + +Proof: + +($\Leftarrow$) Suppose $z_0$ is a removable singularity. Then $\exists r>0$ such that $B_r(z_0)\setminus\{z_0\}=A(z_0;0,r)$ and $f(z)=\sum_{n=0}^{\infty} a_n (z-z_0)^n$ for $z\in A(z_0;0,r)$. Then $f$ is bounded in $A(z_0;0,r/2)$ + +($\Rightarrow$) Suppose $|f(z)|\leq M$ for $z\in A(z_0;0,r/2)$. So $f(z)=\sum_{n=-\infty}^{\infty} a_n (z-z_0)^{n-k-1}=\int_{C_r}f(z)(z-z_0)^{-k-1}dz=a_{k}2\pi i$ + +$a_k=\frac{1}{2\pi i}\int_{C_r}f(z)(z-z_0)^{-k-1}dz$ + +And $|a_k|\leq \max_{z\in C_r}\left|2\pi|f(z)|z-z_0|^{-k-1}\right|\leq 2\pi M r^{-k-1}2\pi r$ + +So $|a_k|\leq (4\pi^2M)r^{-k}$ for all $r