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Mathematical Methods for Physicists: A concise introduction - Site Map

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FUNCTIONS OF A COMPLEX VARIABLE<br />

(b) ln‰…1 ‡ z†=…1 z†Š ˆ ln…1 ‡ z†ln…1 z†. Next, replacing z by z in<br />

Taylor's expansion <strong>for</strong> ln…1 ‡ z†, we have<br />

Then by subtraction, we obtain<br />

ln…1 z† ˆz z2<br />

2 z3<br />

3 z4<br />

4 :<br />

ln 1 ‡ z<br />

1 z ˆ 2 z ‡ z3<br />

3 ‡ z5<br />

5 ‡ !<br />

ˆ X1<br />

nˆ0<br />

2z 2n‡1<br />

2n ‡ 1 :<br />

Laurent series<br />

In many applications it is necessary to expand a function f …z† around points<br />

where or in the neighborhood of which the function is not analytic. The Taylor<br />

series is not applicable in such cases. A new type of series known as the Laurent<br />

series is required. The following is a representation which is valid in an annular<br />

ring bounded by two concentric circles of C 1 and C 2 such that f …z† is single-valued<br />

and analytic in the annulus and at each point of C 1 and C 2 , see Fig. 6.14. The<br />

function f …z† may have singular points outside C 1 and inside C 2 . Hermann<br />

Laurent (1841±1908, French mathematician) proved that, at any point in the<br />

annular ring bounded by the circles, f …z† can be represented by the series<br />

f …z† ˆ X1<br />

nˆ1<br />

a n …z a† n<br />

…6:34†<br />

where<br />

a n ˆ 1 I<br />

2i C<br />

f …w†dw<br />

…w a†<br />

n‡1;<br />

n ˆ 0; 1; 2; ...; …6:35†<br />

Figure 6.14.<br />

Laurent theorem.<br />

274

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