ConceptComplete

Residues and the Residue Theorem

The residue theorem converts contour integrals into algebraic computations involving the singularities of the integrand. It is the central tool for evaluating integrals in complex analysis.


Definition of Residue

Definition6.1Residue

Let ff have an isolated singularity at z0z_0 with Laurent expansion f(z)=n=an(zz0)nf(z) = \sum_{n=-\infty}^\infty a_n(z-z_0)^n in 0<zz0<R0 < |z-z_0| < R. The residue of ff at z0z_0 is

Res(f,z0)=a1=12πiγf(z)dz\text{Res}(f, z_0) = a_{-1} = \frac{1}{2\pi i}\oint_\gamma f(z)\,dz

where γ\gamma is any small positively oriented circle around z0z_0.

RemarkComputing residues

For practical computation:

  • Simple pole (m=1m = 1): Res(f,z0)=limzz0(zz0)f(z)\text{Res}(f, z_0) = \lim_{z \to z_0}(z - z_0)f(z).
  • If f=p/qf = p/q with simple zero of qq: Res(f,z0)=p(z0)/q(z0)\text{Res}(f, z_0) = p(z_0)/q'(z_0).
  • Pole of order mm: Res(f,z0)=1(m1)!limzz0dm1dzm1[(zz0)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)].
  • Essential singularity: Extract a1a_{-1} from the Laurent series directly.
ExampleResidue calculations
  1. f(z)=ezz2f(z) = \frac{e^z}{z^2} at z=0z=0 (pole of order 2): Res=ddzezz=0=1\text{Res} = \frac{d}{dz}e^z\big|_{z=0} = 1.

  2. f(z)=zz2+1f(z) = \frac{z}{z^2+1} at z=iz=i (simple pole): Res=i2i=12\text{Res} = \frac{i}{2i} = \frac{1}{2}.

  3. f(z)=coszzf(z) = \frac{\cos z}{z} at z=0z=0: Since cosz/z=1/zz/2+\cos z/z = 1/z - z/2 + \cdots, Res=1\text{Res} = 1.


The Residue Theorem

Theorem6.1Residue theorem

Let ff be holomorphic on a domain DD except for isolated singularities z1,,znz_1, \ldots, z_n. If γ\gamma is a positively oriented simple closed contour in DD with z1,,znz_1, \ldots, z_n in its interior, then

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

ExampleApplication of the residue theorem

Evaluate z=2z2(z1)(z2+1)dz\oint_{|z|=2} \frac{z^2}{(z-1)(z^2+1)}\,dz.

The singularities inside z=2|z|=2 are z=1,i,iz = 1, i, -i. Computing residues:

Res(f,1)=11+1=12,Res(f,i)=1(i1)(2i)=1+i4\text{Res}(f, 1) = \frac{1}{1+1} = \frac{1}{2}, \quad \text{Res}(f, i) = \frac{-1}{(i-1)(2i)} = \frac{1+i}{4} Res(f,i)=1(i1)(2i)=1i4.\text{Res}(f, -i) = \frac{-1}{(-i-1)(-2i)} = \frac{1-i}{4}.

Sum: 12+1+i4+1i4=12+12=1\frac{1}{2} + \frac{1+i}{4} + \frac{1-i}{4} = \frac{1}{2} + \frac{1}{2} = 1. Therefore the integral is 2πi2\pi i.


Residue at Infinity

Definition6.2Residue at infinity

For ff holomorphic in z>R|z| > R, the residue at infinity is

Res(f,)=12πiz=ρf(z)dz=a1\text{Res}(f, \infty) = -\frac{1}{2\pi i}\oint_{|z|=\rho} f(z)\,dz = -a_{-1}

where the integral is over a large circle (positively oriented) and a1a_{-1} is the coefficient of z1z^{-1} in the Laurent expansion at \infty. Equivalently, Res(f,)=Res(1z2f(1/z),0)\text{Res}(f, \infty) = -\text{Res}\left(\frac{1}{z^2}f(1/z), 0\right).

RemarkGlobal residue theorem

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

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

The sum of all residues on the Riemann sphere is always zero.