TheoremComplete

The Residue Theorem

The residue theorem is the culmination of the theory of complex integration, providing a powerful method to evaluate contour integrals by reducing them to algebraic computations at isolated singularities.


Statement

Theorem6.6Residue theorem

Let DD be a simply connected domain and let ff be holomorphic on DD except at finitely many isolated singularities z1,…,zn∈Dz_1, \ldots, z_n \in D. If γ\gamma is a positively oriented simple closed contour in DD enclosing all singularities, then

∮γf(z) dz=2πi∑k=1nRes(f,zk).\oint_\gamma f(z)\,dz = 2\pi i \sum_{k=1}^n \text{Res}(f, z_k).


Proof

Proof

Surround each singularity zkz_k by a small circle CkC_k of radius εk\varepsilon_k (chosen small enough so the circles are disjoint and contained inside γ\gamma). By Cauchy's theorem for multiply connected domains, applied to the region between γ\gamma and the circles CkC_k:

∮γf dz=∑k=1n∮Ckf dz.\oint_\gamma f\,dz = \sum_{k=1}^n \oint_{C_k} f\,dz.

By definition of residue, ∮Ckf dz=2πi⋅Res(f,zk)\oint_{C_k} f\,dz = 2\pi i \cdot \text{Res}(f, z_k). Therefore:

∮γf dz=2πi∑k=1nRes(f,zk).■\oint_\gamma f\,dz = 2\pi i \sum_{k=1}^n \text{Res}(f, z_k). \qquad \blacksquare

■

Systematic Methods for Computing Residues

RemarkResidue formulas catalog

Let ff have an isolated singularity at z0z_0.

1. Simple pole (m=1m=1): Res(f,z0)=lim⁡z→z0(z−z0)f(z).\text{Res}(f, z_0) = \lim_{z \to z_0}(z-z_0)f(z).

2. Simple pole of p(z)/q(z)p(z)/q(z) where q(z0)=0q(z_0) = 0, q′(z0)≠0q'(z_0) \neq 0: Res(p/q,z0)=p(z0)q′(z0).\text{Res}(p/q, z_0) = \frac{p(z_0)}{q'(z_0)}.

3. Pole of order mm: Res(f,z0)=1(m−1)!lim⁡z→z0dm−1dzm−1[(z−z0)mf(z)].\text{Res}(f, z_0) = \frac{1}{(m-1)!}\lim_{z \to z_0}\frac{d^{m-1}}{dz^{m-1}}[(z-z_0)^m f(z)].

4. Essential singularity: Compute the Laurent series and read off a−1a_{-1}.

ExampleComplete evaluation example

Evaluate I=∮∣z∣=3z2ez(z−1)2(z+2) dzI = \oint_{|z|=3} \frac{z^2 e^z}{(z-1)^2(z+2)}\,dz.

Singularities inside ∣z∣=3|z|=3: z=1z=1 (pole of order 2) and z=−2z=-2 (simple pole).

At z=1z = 1: Res=ddz[z2ezz+2]z=1=ddz[z2ezz+2]z=1\text{Res} = \frac{d}{dz}\left[\frac{z^2 e^z}{z+2}\right]_{z=1} = \frac{d}{dz}\left[\frac{z^2 e^z}{z+2}\right]_{z=1}.

Computing: ddzz2ezz+2=(2z+z2)ez(z+2)−z2ez(z+2)2\frac{d}{dz}\frac{z^2 e^z}{z+2} = \frac{(2z+z^2)e^z(z+2) - z^2 e^z}{(z+2)^2}. At z=1z=1: 3e⋅3−e9=8e9\frac{3e \cdot 3 - e}{9} = \frac{8e}{9}.

At z=−2z = -2: Res=4e−2(−3)2=4e−29\text{Res} = \frac{4e^{-2}}{(-3)^2} = \frac{4e^{-2}}{9}.

Therefore I=2πi(8e9+4e−29)=2πi(8e+4e−2)9I = 2\pi i\left(\frac{8e}{9} + \frac{4e^{-2}}{9}\right) = \frac{2\pi i(8e + 4e^{-2})}{9}.


The Residue Theorem on the Riemann Sphere

Theorem6.7Global residue theorem

If ff is meromorphic on the Riemann sphere C^=C∪{∞}\hat{\mathbb{C}} = \mathbb{C} \cup \{\infty\} with singularities z1,…,znz_1, \ldots, z_n (possibly including ∞\infty), then

∑k=1nRes(f,zk)+Res(f,∞)=0.\sum_{k=1}^n \text{Res}(f, z_k) + \text{Res}(f, \infty) = 0.

ExampleVerification of global residue theorem

For f(z)=1z(z−1)f(z) = \frac{1}{z(z-1)}: residues at z=0z=0: −1-1; at z=1z=1: 11. At ∞\infty: Res(f,∞)=−Res(1w2⋅1(1/w)(1/w−1),0)=−Res(−1w(1−w),0)=−(−1)=1\text{Res}(f, \infty) = -\text{Res}(\frac{1}{w^2}\cdot\frac{1}{(1/w)(1/w-1)}, 0) = -\text{Res}(\frac{-1}{w(1-w)}, 0) = -(-1) = 1. Wait: sum should be 00. Rechecking: Res(f,∞)=0\text{Res}(f, \infty) = 0, and indeed −1+1+0=0-1 + 1 + 0 = 0.

RemarkPower of the residue theorem

The residue theorem unifies many seemingly different results: the Cauchy integral formula (residue of f(z)/(z−z0)f(z)/(z-z_0) at z0z_0 is f(z0)f(z_0)), the argument principle (residue of f′/ff'/f), and the evaluation of definite integrals. It is one of the most versatile tools in all of mathematics.