Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(lu) #1

COMPLEX VARIABLES


x

y

R


z 0

C 1


C 2


Figure 24.12 The region of convergenceRfor a Laurent series off(z) about
a pointz=z 0 wheref(z) has a singularity.

classify the nature of that point. Iff(z) is actually analytic atz=z 0 ,thenin


(24.55) allanforn<0 must be zero. It may happen that not only are allan


zero forn<0 buta 0 ,a 1 ,...,am− 1 are all zero as well. In this case, the first


non-vanishing term in (24.55) isam(z−z 0 )m, withm>0, andf(z)isthensaidto


have azero of ordermatz=z 0.


Iff(z) is not analytic atz=z 0 , then two cases arise, as discussed above (pis

here taken as positive):


(i) it is possible to find an integerpsuch thata−p= 0 buta−p−k= 0 for all
integersk>0;

(ii) it is not possible to find such a lowest value of−p.

In case (i),f(z) is of the form (24.54) and is described as having apole of order


patz=z 0 ; the value ofa− 1 (nota−p) is called theresidueoff(z) at the pole


z=z 0 , and will play an important part in later applications.


For case (ii), in which the negatively decreasing powers ofz−z 0 do not

terminate,f(z) is said to have anessential singularity. These definitions should be


compared with those given in section 24.6.


Find the Laurent series of

f(z)=

1


z(z−2)^3
about the singularitiesz=0andz=2(separately). Hence verify thatz=0is a pole of
order 1 andz=2is a pole of order 3 , and find the residue off(z)at each pole.

To obtain the Laurent series aboutz= 0, we make the factor in parentheses in the

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