A.1 The Basics

The key word linked to contour integration is “analyticity” or the absense thereof:

A function is called analytic in a region R in the complex plane iff all the derivatives of the function (1st, 2nd, ....) exist for every point inside R.
This means that the Taylor series
f(z) ={ \mathop{∑ }}_{n=0}^{∞}{f}^{(n)}(c){{(z − c)}^{n}\over n!}
(A.1)

exists for every point c inside R.
In most cases we are actually interested in functions that are not analytic; if this only happens at isolated points (i.e., we don’t consider a ”line of singularities”, usually called a ”cut” or ”branch-cut”) we can still expand the function in a Laurent series

f(z) ={ \mathop{∑ }}_{n=−∞}^{∞}{f}^{(n)}(c){{(z − c)}^{n}\over n!}
(A.2)

How we obtain the coefficients {f}^{(n)}(c) from the function is closely linked to the problem of contour integration.