In
complex analysis, the
residue is a
complex number which describes the behavior of
line integrals of a
meromorphic function around a
singularity. Residues can be computed quite easily and, once known, allow the determination of more complicated path integrals via the
residue theorem.
Definition
The residue of a meromorphic function
at an
isolated singularity , often denoted
is the unique value
such that
has an
analytic antiderivative in a
punctured disk where γ traces out a circle around c in a counterclockwise manner. We may choose the path γ to be a circle in radius ε around c where ε is as small as we desire.
The residue of a function f(z)=g(z)/h(z) at a simple pole c, where g and h are holomorphic functions in a neighborhood of c with h(c) = 0 and g(c) ≠ 0 is given by
- operatorname{Res}(f,c) = frac{g(c)}{h'(c)}.
More generally, the residue of
f around
z =
c, a
pole of order
n, can be found by the formula:
- mathrm{Res}(f,c) = frac{1}{(n-1)!} cdot lim_{z to c} left(frac{d}{dz}right)^{n-1}left(f(z)cdot (z-c)^{n} right).
If the function f can be continued to a holomorphic function on the whole disk { z : |z − c| < R }, then Res(f, c) = 0. The converse is not generally true.
The latter formula can be very useful in determining the residues for low-order poles. For higher order poles, series expansion is usually easier.
Series methods
If parts or all of a function can be expanded into a
Taylor series or
Laurent series, which may be possible if the parts or the whole of the function has a standard series expansion, then calculating the residue is significantly simpler than by other methods.
As an example, consider calculating the residues at the singularities of the function
- f(z)={sin{z} over z^2-z}
which may be used to calculate certain contour integrals. This function appears to have a singularity at z = 0, but if one factorizes the denominator and thus writes the function as
- f(z)={sin{z} over z(z-1)}
it is apparent that the singularity at z = 0 is a removable singularity and then the residue at z = 0 is therefore 0.
The only other singularity is at z = 1. Recall the expression for the Taylor series for a function g(z) about z = a:
- g(z) = g(a) + g'(a)(z-a) + {g(a)(z-a)^2 over 2!} + {g'(a)(z-a)^3 over 3!}+ cdots
So, for g(z) = sin z and a = 1 we have
- sin{z} = sin{1} + cos{1}(z-1)+{-sin{1}(z-1)^2 over 2!} + {-cos{1}(z-1)^3 over 3!}+cdots.
and for g(z) = 1/z and a = 1 we have
- frac1z = frac1 {(z-1)+1} = 1 - (z-1) + (z-1)^2 - (z-1)^3 + cdots.
Multiplying those two series and introducing 1/(z − 1) gives us
- frac{sin{z}} {z(z-1)} = {sin{1} over z-1} + (cos{1}-sin1) + (z-1) left(-frac{sin{1}}{2!} - cos1 + sin1right) + cdots.
So the residue of f(z) at z = 1 is sin 1.
See also
External links
References
- Ahlfors, Lars (1979). Complex Analysis. McGraw Hill.
- Marsden & Hoffman, Basic complex analysis (Freeman, 1999).