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5.3 Laurent Series
You may have noticed a certain interest in functions which are reciprocals
of polynomials. The reason of course is that they are easy to compute,
just as polynomials are. It is worth looking at functions which are ratios of
polynomials also, and indeed functions which are ratios of other functions we
already know. We shall come back to this later, but for the moment consider
a function such as
ez
z2
This is a ratio of analytic functions and is hence analytic except at the zeros
of the denominator. There are two roots, both the same, so we have a
singularity at z = 0. We can divide out the power series to get
ez
z2 _
1
z2
+
1
z
+
1
2!
+
z
3!
+ _ _ _
I haven't wanted to say these are equal: this would beg the question. But
the question more or less raises itself, are these equal? Or to put it another
way, does the expression on the right converge if jzj > 0, and if so, does it
converge to ez=z2?
The answer is 'yes' to both parts.
More generally, suppose we have a function which is analytic in the annulus
r < jzcj < R, for some point c, the centre of the annulus. Then it will in
general have an expansion in terms of integral powers, some or all of which
may be negative. This is called a Laurent Series for the function.
More formally:
De_nition 5.3.1 (Laurent Series)
5.3. LAURENT SERIES 139
For any w, the integer power series
1 X
1
ak(z c)k; k 2 Z
is de_ned to be
1 X
0
ak(z c)k +
1 X
1
a
k(
1
z c
)k
when both of these series converge.
Theorem 5.3 (Laurent's Theorem)
If f is analytic on the annulus r < jz cj < R, for some point c, then f is
equal to the Laurent series
f(z) =
1 X
1
ak(z c)k
where the coe_cients ak can be computed from:
ak =
1
2_i IC
f(z)
(z c)1+k dz
if k is positive or zero, and
ak =
1
2_i IC
f(z)
(z c)1k dz
when k is negative. C is any simple closed loop around the centre c which is
contained in the annulus and goes in the positive sense.
No Proof: See Mathews and Howell or any standard text. 2
Exercise 5.3.1 Try showing a similar result for the Taylor series for an analytic
function; i.e. try to get an expression for the Taylor series coe_cients
in terms of path integrals.
It is the case that Laurent series about any point, like Power series, are
unique when they converge.
The following result is extremely useful:
140 CHAPTER 5. TAYLOR AND LAURENT SERIES
Theorem 5.4 (Di_erentiability of Laurent Series)
The Laurent series for a function analytic in an annulus if di_erentiated
termwise gives the derivative of the function.
No Proof: 2
Since the case where all the negative coe_cients are zero reduces to the case
of the Taylor series, this is also true for Taylor Series. It is not generally
true that if a function is given by a sequence of approximating functions, the
derivative is given by the sequence of derivatives. After all,
1
n
sin nx
gets closer and closer to the zero function as n increases. But the derivatives
cos nx certainly do not get closer to anything.
This tells us yet again that the analytic functions are very special and that
they behave in particularly pleasant ways, all things considered.
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