lacunary - Mathnotes

Residue Integration

Suppose f(z) has a singularity at z=z0 inside a simple closed curve C but is otherwise analytic on C and inside C.

Then, f(z) has a @laurent-series

f(z)=∑n=0∞an(z−z0)n+b1z−z0+b2(z−z0)2+⋯

that converges for all points near z=z0 (except at z=z0 itself,) in some domain of the form 0<|z−z0|<R.

The coefficient b1 of the first negative power 1/(z−z0) of this @laurent-series is given by the @Cauchy-integral-formula as

b1=12∗pi∗i∮Cf(z)dz.

Now, we can use this to find the value of the integral without using any of the integral formulas:

∮Cf(z)dz=2πib1.

This is a CCW integral around a simple closed path C that contains z=z0 in its interior (but no other singularities of f(z) on or inside C.)

Definition: Residue \@{residue}

Given a convergent @laurent-series

f(z)=∑n=0∞an(z−z0)n+b1z−z0+b2(z−z0)2+⋯,

the coefficient b1 of the first negative power of 1/(z−z0) is called the residue of f(z) at z=z0. It is denoted by

b1=Resz=z0f(z).

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Residue Formulas

Instead of finding the @laurent-series, we can use these handy formulas.

Simple pole at z0

Theorem: First Simple Pole Residue Formula \@{first-simple-pole-residue-formula}

Resz=z0f(z)=b1=limz→z0(z−z0)f(z).

Theorem: Second Simple Pole Residue Formula \@{second-simple-pole-residue-formula}

Resz=z0f(z)=Resz=z0p(z)q(z)=p(z0)q′(z0).

Poles of any Order at z0

Theorem \@{residue-at-mth-order-pole}

Resz=z0f(z)=1(m−1)!limz→z0{dm−1dzm−1[(z−z0)mf(z)]}.

Remark \@{remark-5}

For second order poles (m=2), this gives

Resz=z0f(z)=limz→z0{[(z−z0)2f(z)]′}.

Several Singularities Inside the Contour

Theorem: Residue Theorem \@{residue-theorem}

Let f(z) be analytic inside a simple closed path C and on C, except for finitely many @singular-points z1,z2,…,zk inside C. Then,

∮Cf(z)dz=2πi∑j=1kResz=zjf(z).

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