laurent.htm Laurent Series
Laurent Series

Theorem. Let f(z) be analytic in the closed region
DR1, R2 = {0 < R1 ≤ |z| ≤ R2 }.
Then for R1 < |z| < R2,
f(z) = 1

2πi

(⎜)



CR2 
f(ζ)

ζ− z
 dζ− 1

2πi

(⎜)



CR1 
f(ζ)

ζ− z
 dζ.
Proof: The proof is similar in spirit to the proof of the Cauchy Integral Formula.
Fix z. For ϵ small, let Cz,ϵ = {ζ| |ζ− z| = ϵ} is in between CR1 and CR2. Define gz(ζ) = [(f(ζ))/(ζ− z)]. Then gz(ζ) is an analytic function of ζ in the region between the two circles CR1 and CR2 and outside Cz,ϵ.

laupic1.gif


2πi  f(z)
=
(⎜)



Cz,ϵ 
gz(ζ)  dζ
=
(⎜)



CR2 
gz(ζ)  dζ −
(⎜)



CR1 
gz(ζ)  dζ
=
(⎜)



CR2 
f(ζ)

ζ− z
 dζ−
(⎜)



CR1 
f(ζ)

ζ− z
 dζ.

Next we write
f(z)
= 1

2πi

(⎜)



CR2 
f(ζ)

ζ− z
 dζ− 1

2πi

(⎜)



CR1 
f(ζ)

ζ− z
 dζ
=f1(z) + f2(z).
Proceeding as before
f1(z)
= 1

2πi

(⎜)



CR2 
f(ζ)

ζ− z
 dζ.
= 1

2πi

(⎜)



CR2 
f(ζ) 1

ζ


n = 0 

z

ζ

n

 
 dζ
= 1

2πi

(⎜)



CR2 
f(ζ) 1

ζ
N

n = 0 

z

ζ

n

 
  dζ
+ 1

2πi

(⎜)



CR2 
f(ζ) 1

ζ

z

ζ

N+1

 

1 − z

ζ
 dζ
=

n = 0 
an zn ,
where
an
= 1

2πi

(⎜)



CR2 
f(ζ) 1

ζn+1
  dζ.
Note that f1(z) is analytic in the region {z ||z| ≤ R2}.
In the same spirit,
f2(z)
= − 1

2πi

(⎜)



CR1 
f(ζ)

ζ− z
 dζ
= 1

2πi

(⎜)



CR1 
f(ζ) 1

z
1

1− ζ

z
 dζ
= 1

2πi

(⎜)



CR1 
f(ζ) 1

z


m = 0 

ζ

z

m

 
 dζ
= 1

2πi

(⎜)



CR1 
f(ζ) 1

z
M

m = 0 

ζ

z

m

 
  dζ
+ 1

2πi

(⎜)



CR1 
f(ζ) 1

z

ζ

z

M+1

 

1 − ζ

z
 dζ
=

m = 0 
1

zm+1

1

2πi

(⎜)



CR2 
f(ζ) ζm  dζ
.
Note that f2(z) is analytic in the region {z ||z| ≥ R1}.

The Laurent Expansion

Theorem. Let f(z) be analytic in the region {z |R1 < |z| < R2 }. Then for R1 < |z| < R2,
f(z)
=

n = −∞ 
an zn,
an
= 1

2πi

(⎜)



Cr 
f(ζ) ζ−n − 1  dζ.
Here r is any number such that R1 < r < R2.
The series
f1(z) =

n = 0 
an zn
is analytic in {z | |z| < R2 },
The series
f2(z) = −1

n = −∞ 
an zn
is analytic in {z | R1 < |z| }.


Consequences and Notes

If f(z) be analytic in the region {z ||z| < R2 }, then
an = 1

2πi

(⎜)



Cr 
f(ζ) ζ−n − 1   dζ = 0, n = −1,−2, ….
If f(z) be analytic in the region {z |0 < |z| < R2 }, then
a−1 = 1

2πi

(⎜)



Cr 
f(ζ)   dζ
is called the residue of f(z) at z=0.


Zeroes, Poles, and Essential Singularities
For the moment, we shall consider a function f(z) analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Then
f(z)
=

n = −∞ 
an zn,
an
= 1

2πi

(⎜)



Cr 
f(ζ) ζ−n − 1  dζ.
If f(z) = ∑n = 0 an zn, f(z) may be extended by defining f(0) = a0, and the resulting function is analytic in |z| ≤ R.

If f(z) = ∑n = N an zn, N ≥ 0, aN ≠ 0, f(z) is said to have a zero of order N at z=0. Near z=0,
f(z) = zN ·g(z)
, where g(z) is analytic in |z| ≤ R, g(0) ≠ 0.

If f(z) = ∑n = − M an zn, M ≥ 0, a−M ≠ 0, f(z) is said to have a pole of order M at z=0. Near z=0,
f(z) = z−M ·g(z)
, where g(z) is analytic in |z| ≤ R, g(0) ≠ 0.

If f(z) = ∑n = − ∞ an zn, an ≠ 0 for infinitely many negative n, then f(z) is said to have an essential singularity at z=0.

The coefficient of z−1 is called the residue of f(z) at z=0, and is written
Res(f,z=0) = Resf(z)|z=0 = 1

2πi

(⎜)



Cr 
f(ζ)  dζ.
Exercises

1.
Let f(z) be analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Then for r small and positive,

(⎜)



Cr 
f(ζ)  dζ = 2 πi Resf(z)|z=0.

2.
Let f(z) be analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Suppose that f(z) has a zero of order N > 0, at z=0.
Then for r small and positive,

(⎜)



Cr 
f(ζ)

f(ζ)
 dζ = 2 πi ·N.

3.
Let f(z) be analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Suppose that f(z) has a pole of order M > 0, at z=0.
Then for r small and positive,

(⎜)



Cr 
f(ζ)

f(ζ)
 dζ = − 2 πi ·M.

4.
Let f(z) be analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Suppose that f(z) is bounded as z → 0. Show that
limz → 0 f(z) exists.
f(z) may be extended to be an analytic function in
DR = {z | |z| ≤ R}.
As a consequence, the singularity of f(z) at z=0 is removable .

5.
Let f(z) be analytic in the punctured disk

D
 

R 
= {z |0 < |z| ≤ R}.
Suppose that
f(z) = O(|z|M)  as   z → 0.
Show that for n < M, an = 0.



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On 02 Mar 2012, 09:45.