Singularities: removable, pole, essential

At a Glance

Why This Chapter Matters

Singularity classification is a gateway concept for the entire residue theory. Questions appear in two flavours: (1) abstract proofs using Liouville’s theorem that exploit the connection between singularity type and growth, and (2) explicit classification of a given function together with its Laurent principal part. The 2017 question is a 4-step Liouville argument (easy once the pattern is seen); the 2021 question is a direct Laurent series argument (very fast); the harder 2023 question requires a careful power-series inversion to find the principal part of ez/(z−sin⁡z)e^z/(z-\sin z).

Minimum Theory

Three types of isolated singularity. Let ff be analytic on a punctured disc 0<∣z−z0∣<R0 < |z - z_0| < R with Laurent series ∑n=−∞∞an(z−z0)n\sum_{n=-\infty}^{\infty} a_n (z-z_0)^n. The singularity at z0z_0 is:

Riemann removable singularity theorem. An isolated singularity z0z_0 of ff is removable if and only if ff is bounded on some punctured neighbourhood of z0z_0.

Liouville’s theorem. A bounded entire function is constant.

Key pattern: ff entire ↔\leftrightarrow f(1/z)f(1/z) at 00. If f(z)=∑n≥0anznf(z) = \sum_{n \ge 0} a_n z^n is entire, then f(1/z)=∑n≥0anz−nf(1/z) = \sum_{n \ge 0} a_n z^{-n}, so the singularity of f(1/z)f(1/z) at z=0z=0 is removable if all an=0a_n = 0 for n≥1n \ge 1 (i.e. ff is constant), a pole of order mm if ff is a polynomial of degree mm, and essential if ff is a transcendental entire function (infinitely many nonzero Taylor coefficients).

Three singularity types on the complex plane: removable (no principal part), pole of order m (finite principal part), essential (infinite principal part)

Question Archetypes

ArchetypeRecognition
singularity-classification”classify the singularity”, “find the principal part”, or “Laurent series of f(1/z)f(1/z)“
liouville-application”entire ff such that 00 is a removable singularity of f(1/z)f(1/z)”; answer is that ff must be constant

singularity-classification (2 question(s); 2021, 2023)

Recognition Cues — The problem asks to classify an isolated singularity (removable / pole / essential) and/or to find the principal part of the Laurent series. The function is given explicitly. If it involves f(1/z)f(1/z) where ff is entire, use the Taylor ↔\leftrightarrow Laurent correspondence directly. If it is a ratio like ez/(z−sin⁡z)e^z/(z - \sin z), expand the denominator in a Maclaurin series to find the order of its zero.

Solution Template

  1. Find the order of the zero of the denominator (or the number of nonzero negative-power terms) at the singular point.
  2. Classify: zero of order mm in denominator ⇒\Rightarrow pole of order mm; infinitely many negative powers ⇒\Rightarrow essential; none ⇒\Rightarrow removable.
  3. To find the principal part: expand numerator and denominator as power series, invert using 1/(1−u)=1+u+u2+⋯1/(1-u) = 1 + u + u^2 + \cdots, multiply, and collect all terms with negative powers.

Worked Example — 2021 (abstract)

2021 Paper 2, 2021-P2-Q3a (15 marks)

Let ff be entire with Taylor series at z=0z=0 having infinitely many nonzero terms. Show that z=0z=0 is an essential singularity of f(1/z)f(1/z).

Setup. ff entire means f(z)=∑n=0∞anznf(z) = \sum_{n=0}^{\infty} a_n z^n converges everywhere, with infinitely many an≠0a_n \ne 0.

Step 1 — Substitute. Let g(z)=f(1/z)g(z) = f(1/z). Substituting z→1/zz \to 1/z in the Taylor series:

g(z)=f(1/z)=∑n=0∞anz−n=a0+a1z+a2z2+⋯g(z) = f(1/z) = \sum_{n=0}^{\infty} a_n z^{-n} = a_0 + \frac{a_1}{z} + \frac{a_2}{z^2} + \cdots

This is the Laurent series of gg centred at z=0z = 0, valid for z≠0z \ne 0.

Step 2 — Classify. A singularity is essential when the principal part (negative-power terms) has infinitely many nonzero terms. Here the coefficient of z−nz^{-n} is ana_n. Since infinitely many an≠0a_n \ne 0, the principal part contains infinitely many nonzero terms.

Therefore z=0z = 0 is an essential singularity of g(z)=f(1/z)g(z) = f(1/z). ■\blacksquare

z=0 is an essential singularity of f(1/z).\boxed{z=0 \text{ is an essential singularity of } f(1/z).}

Example: f(z)=ezf(z) = e^z has an=1/n!a_n = 1/n! for all n≥0n \ge 0, so e1/ze^{1/z} has essential singularity at 00 — the textbook illustration of Picard’s theorem.

Worked Example — 2023 (explicit principal part)

2023 Paper 2, 2023-P2-Q4b (15 marks)

Classify the singular point z=0z=0 of f(z)=ezz−sin⁡zf(z) = \dfrac{e^z}{z - \sin z} and obtain the principal part of its Laurent series expansion.

Step 1 — Order of the zero of z−sin⁡zz - \sin z at 00. Using sin⁡z=z−z3/6+z5/120−⋯\sin z = z - z^3/6 + z^5/120 - \cdots:

z−sin⁡z=z36−z5120+⋯=z36 ⁣(1−z220+⋯ ).z - \sin z = \frac{z^3}{6} - \frac{z^5}{120} + \cdots = \frac{z^3}{6}\!\left(1 - \frac{z^2}{20} + \cdots\right).

The leading term is z3/6z^3/6, so z−sin⁡zz - \sin z has a zero of order 3 at z=0z = 0.

Step 2 — Classify the singularity. Since e0=1≠0e^0 = 1 \ne 0, the function f(z)=ez/(z−sin⁡z)f(z) = e^z/(z - \sin z) has a pole of order 3 at z=0z = 0.

Step 3 — Expand 1/(z−sin⁡z)1/(z - \sin z). Write u(z)=z2/20−z4/840+⋯u(z) = z^2/20 - z^4/840 + \cdots so that

1z−sin⁡z=6z3⋅11−u(z)=6z3 ⁣(1+u+u2+O(u3)).\frac{1}{z - \sin z} = \frac{6}{z^3} \cdot \frac{1}{1 - u(z)} = \frac{6}{z^3}\!\left(1 + u + u^2 + O(u^3)\right).

Retaining terms up to z4z^4:

1+u+u2=1+z220+(−1840+1400)z4+O(z6)=1+z220+11z48400+O(z6).1 + u + u^2 = 1 + \frac{z^2}{20} + \left(-\frac{1}{840} + \frac{1}{400}\right)z^4 + O(z^6) = 1 + \frac{z^2}{20} + \frac{11z^4}{8400} + O(z^6).

Therefore:

1z−sin⁡z=6z3+310z+11z1400+O(z3).\frac{1}{z - \sin z} = \frac{6}{z^3} + \frac{3}{10z} + \frac{11z}{1400} + O(z^3).

Step 4 — Multiply by ez=1+z+z2/2+z3/6+⋯e^z = 1 + z + z^2/2 + z^3/6 + \cdots and collect negative powers.

Principal part=6z3+6z2+3310z.\boxed{\text{Principal part} = \frac{6}{z^3} + \frac{6}{z^2} + \frac{33}{10z}.}

The singularity is a pole of order 3, with residue 33/1033/10.

Common Traps

liouville-application (1 question(s); 2017)

Recognition Cues — The problem says ff is entire and asks to characterise all such ff satisfying some singularity condition on f(1/z)f(1/z). The condition “removable singularity at 00 of f(1/z)f(1/z)” translates to ”ff is bounded at infinity”, which combined with entirety and Liouville forces ff to be constant.

Solution Template

  1. Apply Riemann’s removable singularity theorem: removable ⇔\Leftrightarrow f(1/z)f(1/z) bounded near 00 ⇔\Leftrightarrow f(w)f(w) bounded for ∣w∣>R|w| > R.
  2. On the compact disc ∣w∣≤R|w| \le R, ff is continuous hence bounded.
  3. Combine: ff bounded on all of C\mathbb{C}.
  4. Invoke Liouville: bounded entire ⇒\Rightarrow constant.
  5. Verify the converse: constant functions trivially satisfy the condition.

Worked Example

2017 Paper 2, 2017-P2-Q1d (10 marks)

Determine all entire functions f(z)f(z) such that 00 is a removable singularity of f ⁣(1z)f\!\left(\dfrac{1}{z}\right).

Setup. Let g(z)=f(1/z)g(z) = f(1/z), which is analytic on 0<∣z∣<∞0 < |z| < \infty since ff is entire and 1/z1/z is analytic for z≠0z \ne 0. We want z=0z = 0 to be a removable singularity of gg.

Step 1 — Removable ⇔\Leftrightarrow bounded. By Riemann’s removable singularity theorem, z=0z=0 is removable for gg if and only if gg is bounded on some punctured neighbourhood 0<∣z∣<δ0 < |z| < \delta:

∃ δ,M>0 such that ∣f(1/z)∣≤M for 0<∣z∣<δ.\exists\, \delta, M > 0 \text{ such that } |f(1/z)| \le M \text{ for } 0 < |z| < \delta.

Step 2 — Translate to behaviour at ∞\infty. Substituting w=1/zw = 1/z, as zz ranges over 0<∣z∣<δ0 < |z| < \delta the variable ww ranges over ∣w∣>1/δ=:R|w| > 1/\delta =: R. So the condition becomes

∣f(w)∣≤Mfor all ∣w∣>R.|f(w)| \le M \quad \text{for all } |w| > R.

Step 3 — ff is bounded on all of C\mathbb{C}. Since ff is entire, it is continuous on the closed disc {∣w∣≤R}\{|w| \le R\}, which is compact. Continuous functions on compact sets are bounded, so ∣f(w)∣≤M′|f(w)| \le M' for ∣w∣≤R|w| \le R. Combining:

∣f(w)∣≤max⁡{M,M′}for all w∈C.|f(w)| \le \max\{M, M'\} \quad \text{for all } w \in \mathbb{C}.

Step 4 — Liouville’s theorem. A bounded entire function is constant. Therefore f(z)=cf(z) = c for some constant c∈Cc \in \mathbb{C}.

Converse. If f≡cf \equiv c, then f(1/z)=cf(1/z) = c is constant on the punctured plane, so z=0z=0 is trivially a removable singularity. Every constant satisfies the condition.

f is entire with 0 removable for f(1/z)  ⟺  f is constant.\boxed{f \text{ is entire with } 0 \text{ removable for } f(1/z) \iff f \text{ is constant.}}

■\blacksquare

Laurent verification: Write f(w)=∑n≥0anwnf(w) = \sum_{n \ge 0} a_n w^n. Then f(1/z)=∑n≥0anz−nf(1/z) = \sum_{n \ge 0} a_n z^{-n}. Singularity at 00 is removable iff all an=0a_n = 0 for n≥1n \ge 1, i.e. f(w)=a0f(w) = a_0 is constant. Agrees exactly with the boxed answer.

Common Traps

Marks-Aware Writing

For a 10-mark question (2017 type): state Riemann’s theorem, translate boundedness to ∞\infty, invoke compactness, invoke Liouville — four steps clearly labelled, 2–3 marks each. For a 15-mark question (2021, 2023): the 2021 proof needs explicit Laurent series setup and classification by definition; the 2023 question needs the full power-series computation with the denominator expansion shown step by step and the principal-part terms identified term by term. Writing the principal part in any form not broken into z−3,z−2,z−1z^{-3}, z^{-2}, z^{-1} terms will lose marks.

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