We classify in this lecture singularities of complex functions. Let us recall that a point z0z_0 where the function f(z)f(z) is not analytic is called a singular point of f(z)f(z).

Definition 1. Let z0z_0 be a singular point of f(z)f(z). If ff is analytic in 0<|z−z0|<R0<|z-z_0|<R, for some R>0R>0, we say z0z_0 is an isolated singular point of f(z)f(z).

Example 2. Let f(z)=11−zf(z)=\dfrac{1}{1-z}, then z=1z=1 is an isolated singular point of f(z)f(z) since f(z)f(z) is analytic besides at the point z=1z=1.

Example 3. Let f(z)=ez(z−i)2f(z)=\dfrac{e^z}{(z-i)^2}, then z=iz=i is an isolated singular point of f(z)f(z) since f(z)f(z) is analytic besides at the point z=iz=i.

Example 4. Let f(z)=1sinzf(z)=\dfrac{1}{\sin z}, then z=kπz=k\pi (k∈ℤk\in\mathbb Z) are all isolated singular points of f(z)f(z).

Example 5. Let f(z)=e1/zf(z)=e^{1/z}, then z=0z=0 is an isolated singular points of f(z)f(z).

Removable singularities

Definition 6. Let z0z_0 be an isolated singular point of f(z)f(z). We say that z0z_0 is a removable singular point of f(z)f(z) if limz→z0f(z)=c0\displaystyle\lim_{z\to z_0} f(z) = c_0 for some c0∈ℂc_0\in\mathbb C.

Here are two classical examples of removable singular points.

Example 7. Let f(z)=sinzzf(z)=\dfrac{\sin z}{z}, then z=0z=0 is an isolated singular points of f(z)f(z) (this is easy to check since f′(z)=zcosz−sinzz2f'(z)=\dfrac{z\cos z-\sin z}{z^2} which blows up at z=0z=0). Moreover, z=0z=0 is a removable singular point since limz→0f(z)=1\displaystyle\lim_{z\to 0}f(z)=1.

Example 8. Let f(z)=ez−1zf(z)=\dfrac{e^z-1}{z}, then z=0z=0 is an isolated singular points of f(z)f(z) (since f′(z)=(z−1)ezz2f'(z)=\dfrac{(z-1)e^z}{z^2} which blows up at z=0z=0). Moreover, z=0z=0 is a removable singular point since limz→0f(z)=1\displaystyle\lim_{z\to 0} f(z)=1.

Poles of different orders

Definition 9. Let z0z_0 be an isolated singular point of f(z)f(z). We say that z0z_0 is an nn-th order pole of f(z)f(z) if there exists a positive integer nn and an analytic function g(z)g(z) (in a neighborhood of z0z_0) such that f(z)=g(z)(z−z0)nandg(z0)≠0.f(z)=\dfrac{g(z)}{(z-z_0)^n} \qquad \mbox{and} \qquad g(z_0)\neq 0. If n=1n=1, we say z0z_0 is a simple pole.

Example 10. Let f(z)=1(z−1)(z−2)f(z)=\dfrac{1}{(z-1)(z-2)}. Then z=1z=1 and z=2z=2 are both isolated singular points. Let g(z)=1(z−1)g(z)= \dfrac{1}{(z-1)}. Then g(z)g(z) is analytic when |z−2|≤0.5|z-2|\le 0.5 and f(z)=g(z)z−2f(z)=\dfrac{g(z)}{z-2}. Therefore, z=2z=2 is a simple pole. For the same reason, z=1z=1 is also a simple pole.

Example 11. Let f(z)=3z+1(z−1)3(z−2)(z−5)2f(z)=\dfrac{3z+1}{(z-1)^3(z-2)(z-5)^2}. Then z=1z=1 is a 3rd order pole, z=5z=5 is a second order pole and z=1z=1 is a simple pole.

Example 12. Let f(z)=3z+1zsinzf(z)=\dfrac{3z+1}{z\sin z}. Then it is clear that z=0z=0 is an isolated singular point, but is not removable. Using Taylor series of sinz\sin z at z=0z=0, we have f(z)=3z+1zsinz=3z+1z(z−z33!+z55!−⋯)=3z+1z2(1−z23!+z45!−⋯)=3z+1z2(1+(z23!−z45!+⋯)+(z23!−z45!+⋯)2+⋯)\begin{gathered} f(z)=\dfrac{3z+1}{z\sin z} = \dfrac{3z+1}{z(z-\frac{z^3}{3!}+\frac{z^5}{5!}-\cdots)}=\dfrac{3z+1}{z^2(1-\frac{z^2}{3!}+\frac{z^4}{5!}-\cdots)} \\ =\dfrac{3z+1}{z^2}\left(1+(\frac{z^2}{3!}-\frac{z^4}{5!}+\cdots)+(\frac{z^2}{3!}-\frac{z^4}{5!}+\cdots)^2+\cdots\right) \end{gathered} Therefore, z=0z=0 is a second order pole.

Remark 13 ([Warning!]). The requirement that g(z0)≠0g(z_0)\neq 0 is essential in the definition of poles. For instance, let f(z)=sinzz−1f(z)=\dfrac{\sin z}{z-1}, then z=1z=1 is a simple pole. However, define the analytic function g(z)=sinz(z−1)3g(z)=\sin z(z-1)^3, we have f(z)=sinzz−1=sinz(z−1)3(z−1)4=g(z)(z−1)4.f(z)=\dfrac{\sin z}{z-1}=\dfrac{\sin z(z-1)^3}{(z-1)^4} =\dfrac{g(z)}{(z-1)^4}. Therefore, it looks like that z=1z=1 is a fourth order pole. This is NOT the case since g(1)=0g(1)=0.

Essential singular points

Definition 14. Let z0z_0 be an isolated singular point of f(z)f(z). We call z0z_0 an essential singular point of f(z)f(z) if it is neither a removable singular point nor a pole.

Example 15. Let f(z)=e1/zf(z)=e^{1/z}. Then z=0z=0 is an isolated singular point. However, z=0z=0 is not removable. To see why z=0z=0 is not a pole, we observe that we can not have a finite nn such that zne1/zz^n e^{1/z} is analytic.

Singularities at Infinity

Using the transform z→1/zz\to 1/z, we can study singularities of functions at z=∞z=\infty: the type of singularity of f(z)f(z) at z=∞z=\infty is the same as that of f(1/z)f(1/z) at z=0z=0.

Example 16. The function f(z)=z2f(z)=z^2 has a second order pole at z=∞z=\infty. This is because f(1/z)=1/z2f(1/z)=1/z^2 has a second order pole at z=0z=0.

Example 17. The function f(z)=ezf(z)=e^z has an essential singularity at z=∞z=\infty. This is because f(1/z)=e1/zf(1/z)=e^{1/z} has an essential singularity at z=0z=0.

Guided review and additional examples

Learning goals

  • Classify isolated singularities as removable, poles, or essential.
  • Use limits and Laurent coefficients to recognize each type.
  • Determine the order of a pole.
  • Extend a function across a removable singularity.

Classification checklist

Near an isolated singularity z0z_0, inspect the Laurent series. No negative powers means the singularity is removable. Finitely many negative powers means a pole, whose order is the largest negative exponent. Infinitely many negative powers means an essential singularity.

Worked example 1: remove a singularity

For f(z)=sinz/zf(z)=\sin z/z at z=0z=0,

sinzz=1−z23!+z45!−⋯. \frac{\sin z}{z}=1-\frac{z^2}{3!}+\frac{z^4}{5!}-\cdots.

There are no negative powers, and limz→0sinz/z=1\lim_{z\to0}\sin z/z=1. Defining f(0)=1f(0)=1 extends ff to an entire function.

Worked example 2: compare a pole and an essential singularity

The function 1/z31/z^3 has a pole of order 33 at zero because z3(1/z3)=1z^3(1/z^3)=1. By contrast,

e1/z=1+1z+12!z2+13!z3+⋯ e^{1/z}=1+\frac1z+\frac{1}{2!z^2}+\frac{1}{3!z^3}+\cdots

has infinitely many negative powers, so zero is an essential singularity. Multiplying by any fixed power of zz cannot make it analytic at zero.

Check your understanding

What kind of singularity does (1−cosz)/z2(1-\cos z)/z^2 have at 00, and what value removes it?

Show the answer

Since 1−cosz=z2/2−z4/4!+⋯1-\cos z=z^2/2-z^4/4!+\cdots, the quotient tends to 1/21/2. The singularity is removable, and defining the value at zero to be 1/21/2 gives an analytic extension.