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Chapter V. Singularities

This document defines and classifies different types of isolated singularities that a function can have at a point, including removable, pole, and essential singularities. A function has a removable singularity if it can be modified to be analytic at that point, a pole if the limit of the function values goes to infinity as the point is approached, and an essential singularity if it exhibits complex unpredictable behavior near that point. The Laurent series representation allows classifying a singularity based on the behavior of its coefficients. An essential singularity is characterized by having non-zero coefficients for infinitely many negative powers.

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0% found this document useful (0 votes)
179 views5 pages

Chapter V. Singularities

This document defines and classifies different types of isolated singularities that a function can have at a point, including removable, pole, and essential singularities. A function has a removable singularity if it can be modified to be analytic at that point, a pole if the limit of the function values goes to infinity as the point is approached, and an essential singularity if it exhibits complex unpredictable behavior near that point. The Laurent series representation allows classifying a singularity based on the behavior of its coefficients. An essential singularity is characterized by having non-zero coefficients for infinitely many negative powers.

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TOM DAVIS
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© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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V.1.

Classification of Singularities 1

Chapter V. Singularities
V.1. Classification of Singularities

Note. In this section, we define various types of singularities of a function and


develop the idea of a Laurent series.

Definition. A function f has an isolated singularity at z = a if there is an R > 0


such that f is defined and analytic in B(a; R) \ {a}, but not in B(a; R). Point a is
a removable singularity if there is an analytic function g : B(a; R) → C such that
g(z) = f (z) for 0 < |z − a| < R.

Example. Functions f1 (z) = 1/z and f2(z) = sin z/z, and f3 (z) = exp(1/z) each
have isolated singularities at z = 0. As shown in Exercise V.1.1, f2 (z) = sin z/z
has a removable singularity.

Theorem V.1.2. If f has an isolated singularity at a then z = a is a removable


singularity if and only if lim (z − a)f (z) = 0.
z→a

Definition. If z = a is an isolated singularity of f then a is a pole of f if lim |f (z)| =


z→a
∞. If an isolated singularity is neither a pole nor a removable singularity it is called
an essential singularity.
V.1. Classification of Singularities 2

1
Example. Function f (z) = for m ∈ N has a pole at z = a. Function
(z − a)m
g(z) = exp(z −1 ) has an essential singularity at z = 0. In fact, a function with a
pole at z = a has a well defined form, as given next.

Proposition V.1.4. If G is a region with a ∈ G, and if f is analytic in G \ {a}


with a pole at z = a, then there is a positive integer m and an analytic function
g(z)
g : G → C such that f (z) = .
(z − a)m

Definition. If f has a pole at z = a and m is the smallest positive integer such


that f (z)(z − a)m has a removable singularity at z = a, then f has a pole of order
m at z = a. A pole of order 1 is called a simple pole.

Note. If f has a pole of order m at z = a, then f (z) = g(z)/(z − a)m where g is


analytic in B(a; R) (for some R > 0), so
X

m−1 m
g(z) = Am + Am−1 (z − a) + · · · + A1 (z − a) + (z − a) ak (z − a)k
k=0

and
Am Am−1 A1
f (z) = + + · · · + + g1 (z)
(z − a)m (z − a)m−1 (z − a)
where g1 is analytic in B(a; R) and Am 6= 0.
V.1. Classification of Singularities 3

Definition. If f has a pole of order m at z = a and f satisfies

Am Am−1 A1
f (z) = + + · · · + + g1 (z)
(z − a)m (z − a)m−1 (z − a)

then
Am Am−1 A1
+ + · · · +
(z − a)m (z − a)m−1 (z − a)
is called the singular part of f at z = a.

Note. We will see that an essential singularity behaves rather like a pole of infinite
order. This then produces an infinite singular part. First, some definitions.

Definition V.1.10. If {zn | n ∈ Z} is a doubly infinite sequence of complex


P P∞ P∞
numbers, then ∞ a
n=−∞ n is absolutely convergent if both a
n=0 n and n=1 a−n

are absolutely convergent. If these series are absolutely convergent then define
X
∞ X
∞ X

zn = z−n + zn .
n=−∞ n=1 n=0
P∞
If un is a function on a set S for n ∈ Z and un (s) is absolutely convergent for
n=−∞
P P∞
every s ∈ S, then the convergence is uniform over S if both ∞ n=0 un and n=1 u−n

converge uniformly on S.

Definition. If 0 ≤ R1 < R2 ≤ ∞ and a is any complex number, define

ann(a; R1, R2) = {z | R1 < |z − a| < R2}.


V.1. Classification of Singularities 4

Note. We now deal with a series representation of a function analytic on an


annulus.

Theorem V.1.11. Laurent Series Development.


Let f be analytic in ann(a; R1, R2). Then
X

f (z) = an (z − a)n
n=−∞

where the convergence is absolute and uniform over the closure of ann(a; r1, r2 ) if
R1 < r1 < r2 < R2. The coefficients an are given by
Z
1 f (z)
an = dz (1.12)
2πi γ (z − a)n+1
where γ is the circle |z − a| = r for any r with R1 < r < R2. Moreover, this series
is unique.

Note. The proof of Theorem V.1.11 is in a, sort of, self contained supplement.
The Laurent series allows us to classify isolated singularities.

Corollary V.1.18. Let z = a be an isolated singularity of f and let f (z) =


X

an (z − a)n be its Laurent expansion in ann(a; 0, R). Then
−∞

(a) z = a is a removable singularity if and only if an = 0 for n ≤ −1,

(b) a = z is a pole of order m if and only if a−m 6= 0 and an = 0 for n ≤ −(m + 1),
and

(c) z = a is an essential singularity if and only if an 6= 0 for infinitely many negative


integers n.
V.1. Classification of Singularities 5

Note. If f has an essential singularity at z = a, then limz→a |f (z)| does not exist.
The text says: “This means that as z approaches a the values of f (z) must wander
through C.” The following result shows that this wandering is very intense.

Theorem V.1.21. Casorati-Weierstrass Theorem.


If f has an essential singularity at z = a then for every δ > 0, {f (ann(a; 0, δ)}− = C.

Note. A more general result concerning the behavior of f near an essential singu-
larity is in Chapter XII (the last chapter of the text, page 300):
Great Picard Theorem.
Suppose an analytic function has an essential singularity at z = a. Then in each
neighborhood of a, f assumes each complex number, with one possible exception,
an infinite number of times.

Note. Function f (z) = exp(1/z) is such a function, and it clearly does not take
on the value 0.

Note. For the record, from page 297 we have:


Little Picard Theorem.
If f is an entire function that omits two values, then f is a constant.

Note. Of course, f (z) = ez is an example of a function omitting one value.

Revised: 3/29/2018

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