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Mathematical Methods for Physicists: A concise introduction - Site Map

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FUNCTIONS OF A COMPLEX VARIABLE<br />

Thus on letting z ! a<br />

that is,<br />

d m1<br />

lim<br />

z!a dz m1 ‰…z a†m f …z†Š ˆ …m 1†!a 1 ;<br />

( )<br />

Res f …z† ˆ 1<br />

zˆa …m 1†! lim d m1<br />

z!a dz m1 ‰ …z a†m f …z† Š : …6:40†<br />

Of course, in the case of a rational function f …z† the residues can also be<br />

determined from the representation of f …z† in terms of partial fractions.<br />

The residue theorem<br />

So far we have employed the residue method to evaluate contour integrals whose<br />

integrands have only a single singularity inside the contour of integration. Now<br />

consider a simple closed curve C containing in its interior a number of isolated<br />

singularities of a function f …z†. If around each singular point we draw a circle so<br />

small that it encloses no other singular points (Fig. 6.15), these small circles,<br />

together with the curve C, <strong>for</strong>m the boundary of a multiply-connected region in<br />

which f …z† is everywhere analytic and to which Cauchy's theorem can there<strong>for</strong>e be<br />

applied. This gives<br />

1<br />

2i<br />

I<br />

C<br />

I<br />

I<br />

f …z†dz ‡ f …z†dz ‡‡<br />

C 1<br />

f …z†dz<br />

C m<br />

<br />

ˆ 0:<br />

If we reverse the direction of integration around each of the circles and change the<br />

sign of each integral to compensate, this can be written<br />

I<br />

1<br />

f …z†dz ˆ 1 I<br />

f …z†dz ‡ 1 I<br />

f …z†dz ‡‡ 1 I<br />

f …z†dz;<br />

2i C 2i C 1<br />

2i C 2<br />

2i C m<br />

Figure 6.15.<br />

Residue theorem.<br />

282

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