ConceptComplete

Singularities and Their Behavior

The behavior of a holomorphic function near an isolated singularity is completely characterized by its Laurent expansion. The three types of singularities — removable, poles, and essential — exhibit dramatically different behavior.


Removable Singularities

Theorem5.5Riemann's removable singularity theorem

Let ff be holomorphic on 0<zz0<R0 < |z - z_0| < R. The following are equivalent:

  1. z0z_0 is a removable singularity (the principal part of the Laurent series vanishes).
  2. limzz0f(z)\lim_{z \to z_0} f(z) exists and is finite.
  3. ff is bounded in some punctured neighborhood of z0z_0.
  4. limzz0(zz0)f(z)=0\lim_{z \to z_0} (z-z_0)f(z) = 0.
ExampleDetecting removable singularities

The function f(z)=z31z1f(z) = \frac{z^3 - 1}{z - 1} has a removable singularity at z=1z = 1 since limz1f(z)=limz1(z2+z+1)=3\lim_{z \to 1} f(z) = \lim_{z \to 1} (z^2 + z + 1) = 3. After removal, ff extends to an entire function.

Similarly, ez1z\frac{e^z - 1}{z} has a removable singularity at z=0z = 0 with limit 11.


Poles

Definition5.4Pole

A function ff has a pole of order mm at z0z_0 if the Laurent series has the form

f(z)=am(zz0)m++a1zz0+a0+a1(zz0)+f(z) = \frac{a_{-m}}{(z-z_0)^m} + \cdots + \frac{a_{-1}}{z-z_0} + a_0 + a_1(z-z_0) + \cdots

with am0a_{-m} \neq 0. A pole of order 11 is called a simple pole. Equivalently, ff has a pole of order mm at z0z_0 if and only if g(z)=(zz0)mf(z)g(z) = (z-z_0)^m f(z) has a removable singularity at z0z_0 with g(z0)0g(z_0) \neq 0.

Theorem5.6Characterization of poles

The following are equivalent:

  1. ff has a pole at z0z_0.
  2. limzz0f(z)=\lim_{z \to z_0} |f(z)| = \infty.
  3. 1/f1/f has a zero at z0z_0 (after defining 1/f(z0)=01/f(z_0) = 0).
  4. ff has a pole of order mm if and only if 1/f1/f has a zero of order mm.
ExampleResidue at a pole

For a simple pole at z0z_0: Res(f,z0)=limzz0(zz0)f(z)\text{Res}(f, z_0) = \lim_{z \to z_0}(z-z_0)f(z).

For a 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)].

For f(z)=1(z1)2(z+1)f(z) = \frac{1}{(z-1)^2(z+1)}: at z=1z=1 (pole of order 2), Res(f,1)=ddz1z+1z=1=14\text{Res}(f, 1) = \frac{d}{dz}\frac{1}{z+1}\big|_{z=1} = -\frac{1}{4}.


Essential Singularities

Theorem5.7Casorati-Weierstrass theorem

If ff has an essential singularity at z0z_0, then for every ε>0\varepsilon > 0, the image f({0<zz0<ε})f(\{0 < |z-z_0| < \varepsilon\}) is dense in C\mathbb{C}.

Theorem5.8Picard's great theorem

If ff has an essential singularity at z0z_0, then in every punctured neighborhood of z0z_0, ff takes every complex value infinitely often with at most one exception.

ExampleEssential singularity of $e^{1/z}$

The function e1/ze^{1/z} has an essential singularity at z=0z = 0. To find zz near 00 with e1/z=we^{1/z} = w (for any w0w \neq 0), solve 1/z=logw+2πik1/z = \log w + 2\pi i k, giving zk=1/(logw+2πik)0z_k = 1/(\log w + 2\pi ik) \to 0 as kk \to \infty. The only omitted value is w=0w = 0 (since e1/z0e^{1/z} \neq 0), confirming Picard's theorem.


Behavior Summary

RemarkClassification summary

| Type | limzz0f(z)\lim_{z \to z_0} f(z) | Laurent principal part | Behavior near z0z_0 | |------|-------------------------|----------------------|---------------------| | Removable | Finite limit exists | None (empty) | ff extends holomorphically | | Pole of order mm | \infty | Finitely many terms | f(z)C/zz0m|f(z)| \sim C/|z-z_0|^m | | Essential | No limit exists | Infinitely many terms | ff takes almost all values |

The trichotomy is exhaustive: every isolated singularity falls into exactly one of these categories.