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# Math416 Lecture 19
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## Continue on the Laurent series
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### Laurent series
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If $f$ is holomorphic in $A(z_0;R_1,R_2)$ then $f=\sum_{n=-\infty}^{\infty} a_n (z-z_0)^n$ where the Laurent series converges on the annulus $A(z_0;R_1,R_2)$
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$$
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\int_{C(z_0,r)} f(z)(z-z_0)^{-k-1} dz = \sum_{n=-\infty}^{\infty} a_n \int_{C(z_0,r)} (z-z_0)^{n-k-1} dz=a_k 2\pi i
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$$
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> $C(z_0,r)$ is a circle centered at $z_0$ with radius $r$
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### Isolated singularities
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A punctured disk at $z_0$ is $A(z_0;0,R)=\{z:0<|z-z_0|<R\}$
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Say a function $f$ has an isolated singularity at $z_0$ if it is holomorphic in a punctured disk $A(z_0;0,R)$
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$f$ has a Laurent series in $A(z_0;0,R)$
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$$
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f(z) = \sum_{n=-\infty}^{\infty} a_n (z-z_0)^n
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$$
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that converges in $A(z_0;0,R)$
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#### Principal part of a Laurent series
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The principal part of a Laurent series is the sum of the terms with negative powers of $(z-z_0)$
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$$
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\sum_{n=-\infty}^{-1} a_n (z-z_0)^n
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$$
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Say the isolated singularity is
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- removable if $a_n=0$ for all $n<0$
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- If $f(z)$ has a removable singularity at $z_0$, then extend $f$ to $\mathbb{D}_{z_0,R}$ by defining $f(z_0)=a_0$. This extended $f$ is holomorphic on $\mathbb{D}_{z_0,R}$ and $f(z)=\sum_{n=0}^{\infty} a_n (z-z_0)^n$ for $z\in \mathbb{D}_{z_0,R}$
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- pole if $a_{-k}\neq 0$ and $a_n=0$ for all $n<-k$
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- A pole with order $1$ is a simple pole
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- essential if the cases above are not true
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Example:
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1. $f(z)=\frac{\sin z}{z}$ has a removable singularity at $z=0$.
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the power series is
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$$
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\sin z = z - \frac{z^3}{3!} + \frac{z^5}{5!} - \cdots
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$$
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So the Laurent series is
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$$
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\frac{\sin z}{z} = 1 - \frac{z^2}{3!} + \frac{z^4}{5!} - \cdots
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$$
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The singularity is removable by defining $f(0)=1$
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2. $f(z)=\frac{z^2-1}{(z-1)(z-3)}=\frac{(z-1)(z+1)}{(z-1)(z-3)}$
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There are two poles at $z=1$ and $z=3$
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the singularity at $z=1$ is removable by defining $f(1)=1$
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the singularity at $z=3$ is a simple pole with order 1 $f(z)=\frac{z+1}{z-3}=\frac{(z-3)+4}{z-3}=4(z-3)^{-1}+1$
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3. $f(z)=\frac{(z+1)^2(z+2)^3}{(z-1)^2(z-5)^6(z-8)}$
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there are three poles at $z=1,5,8$, the order of the poles are 2, 6, 1 respectively.
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@@ -22,4 +22,5 @@ export default {
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Math416_L16: "Complex Variables (Lecture 16)",
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Math416_L16: "Complex Variables (Lecture 16)",
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Math416_L17: "Complex Variables (Lecture 17)",
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Math416_L17: "Complex Variables (Lecture 17)",
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Math416_L18: "Complex Variables (Lecture 18)",
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Math416_L18: "Complex Variables (Lecture 18)",
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Math416_L19: "Complex Variables (Lecture 19)",
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}
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}
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Complex variables. This is a course that explores the theory and applications of complex analysis as extension of Real analysis.
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Complex variables. This is a course that explores the theory and applications of complex analysis as extension of Real analysis.
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The course is taught by Professor.
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The course is taught by Professor.
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John E. McCarthy <mccarthy@math.wustl.edu>
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John E. McCarthy <mailto:mccarthy@math.wustl.edu>
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Some interesting fact is that he cover the lecture terribly quick. At least for me. I need to preview and review the lecture after the course ended. The only thing that I can take granted of is that many theorem in real analysis still holds in the complex. By elegant definition designing, we build a wonderful math with complex variables and extended theorems, which is more helpful when solving questions that cannot be solved in real numbers.
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Some interesting fact is that he cover the lecture terribly quick. At least for me. I need to preview and review the lecture after the course ended. The only thing that I can take granted of is that many theorem in real analysis still holds in the complex. By elegant definition designing, we build a wonderful math with complex variables and extended theorems, which is more helpful when solving questions that cannot be solved in real numbers.
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McCarthy like to write $\zeta$ for $z$ and his writing for $\zeta$ is almost identical with $z$, I decided to use the traditional notation system I've learned to avoid confusion in my notes.
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McCarthy like to write $\zeta$ for $z$ and his writing for $\zeta$ is almost identical with $z$, I decided to use the traditional notation system I've learned to avoid confusion in my notes.
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I will use $B_r(z_0)$ to denote a disk in $\mathbb{C}$ such that $B_r(z_0) = \{ z \in \mathbb{C} : |z - z_0| < r \}$
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I will use $B_r(z_0)$ to denote a disk in $\mathbb{C}$ such that $B_r(z_0) = \{ z \in \mathbb{C} : |z - z_0| < r \}$. In the lecture, he use $\mathbb{D}(z_0,r)$ to denote the disk centered at $z_0$ with radius $r$. If $\mathbb{D}$ is used, then it means the unit disk $\mathbb{D}=\{z:|z|<1\}$. You may also see the closure of the disk $\overline{B_r(z_0)}$ and $\overline{\mathbb{D}}$, these are equivalent definition.
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I will use $z$ to replace the strange notation of $\zeta$. If that makes sense.
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I will use $z$ to replace the strange notation of $\zeta$. If that makes sense.
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