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Mathematical Methods for Physicists: A concise introduction - Site Map

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FUNCTIONS OF A COMPLEX VARIABLE<br />

Notice that the Eq. (6.31) is just a Taylor series at the origin of a function with<br />

f n …0† ˆa n n!. Every choice we make <strong>for</strong> the in®nite variables a n de®nes a new<br />

function with its own set of derivatives at the origin. Of course we can go beyond<br />

the origin, and expand a function in a Taylor series centered at z ˆ z 0 . Thus in the<br />

complex analysis there is a Taylor expansion <strong>for</strong> every analytic function. This is<br />

the question addressed by Taylor's theorem (named after the English mathematician<br />

Brook Taylor, 1685±1731):<br />

If f(z) is analytic throughout a region R bounded by a simple<br />

closed curve C, and if z and a are both interior to C, then f(z)<br />

can be expanded in a Taylor series centered at z ˆ a <strong>for</strong><br />

jz aj < R:<br />

f …z† ˆf …a†‡f 0 …a†…z a†‡f 00 …z a†2<br />

…a† ‡ <br />

2!<br />

‡ f n …z a†n1<br />

…a† ‡ R<br />

n!<br />

n ; …6:32†<br />

where the remainder R n is given by<br />

I<br />

R n …z† ˆ…z a† n 1<br />

2i C<br />

f …w†dw<br />

…w a† n …w z† :<br />

Proof:<br />

To prove this, we ®rst rewrite Cauchy's integral <strong>for</strong>mula as<br />

f …z† ˆ 1 I<br />

f …w†dw<br />

2i C w z ˆ 1 I<br />

2i C<br />

f …w†<br />

w a<br />

<br />

1<br />

<br />

1 …z a†=…w a†<br />

dw:<br />

…6:33†<br />

For later use we note that since w is on C while z is inside C,<br />

z a<br />

< 1:<br />

w a<br />

From the geometric progression<br />

we obtain the relation<br />

1 ‡ q ‡ q 2 ‡ ‡q n ˆ 1 qn‡1<br />

1 q ˆ 1<br />

1 q qn‡1<br />

1 q<br />

1<br />

1 q ˆ 1 ‡ q ‡‡qn ‡ qn‡1<br />

1 q :<br />

270

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