Residue (complex analysis)

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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.

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[edit] Definition

The residue of a meromorphic function f at an isolated singularity a, often denoted Res(f,a) is the unique value R such that f(z)-{R \over (z-a)} has an analytic antiderivative in a punctured disk 0 < | za | < δ. Alternatively, residues can be calculated by finding Laurent series expansions, and are sometimes defined in terms of them.

[edit] Motivation

As an example, consider the contour integral

\oint_C {e^z \over z^5}\,dz

where C is some Jordan curve about 0.

Let us evaluate this integral without using standard integral theorems that may be available to us. Now, the Taylor series for ez is well-known, and we substitute this series into the integrand. The integral then becomes

\oint_C {1 \over z^5}\left(1+z+{z^2 \over 2!} + {z^3\over 3!} + {z^4 \over 4!} + {z^5 \over 5!} + {z^6 \over 6!} + \cdots\right)\,dz.

Let us bring the 1/z5 term into the series, and so, we obtain

\oint_C \left({1 \over z^5}+{z \over z^5}+{z^2 \over 2!\;z^5} + {z^3\over 3!\;z^5} + {z^4 \over 4!\;z^5} + {z^5 \over 5!\;z^5} + {z^6 \over 6!\;z^5} + \cdots\right)\,dz =
\oint_C \left({1 \over\;z^5}+{1 \over\;z^4}+{1 \over 2!\;z^3} + {1\over 3!\;z^2} + {1 \over 4!\;z} + {1\over\;5!} + {z \over 6!} + \cdots\right)\,dz.

The integral now collapses to a much simpler form. Recall that

\oint_C {1 \over z^a} \,dz=0,\quad a \in \mathbb{Z},\mbox{ for }a \ne 1.

So now the integral around C of every other term not in the form cz−1 becomes zero, and the integral is reduced to

\oint_C {1 \over 4!\;z} \,dz={1 \over 4!}\oint_C{1 \over z}\,dz={1 \over 4!}(2\pi i) = {\pi i \over 12}.

The value 1/4! is the residue of ez/z5 at z = 0, and is notated as

\mathrm{Res}_0 {e^z \over z^5},\ \mathrm{or}\ \mathrm{Res}_{z=0} {e^z \over z^5},\ \mathrm{or}\ \mathrm{Res}(f,0).

[edit] Calculating residues

Suppose a punctured disk D = {z : 0 < |zc| < R} in the complex plane is given and f is a holomorphic function defined (at least) on D. The residue Res(f, c) of f at c is the coefficient a−1 of (zc)−1 in the Laurent series expansion of f around c. At a simple pole, the residue is given by:

\operatorname{Res}(f,c)=\lim_{z\to c}(z-c)f(z).

According to Cauchy's integral formula, we have:

\operatorname{Res}(f,c) = 
{1 \over 2\pi i} \int_\gamma f(z)\,dz

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 : |zc| < R }, then Res(f, c) = 0. The converse is not generally true.

Due to its simplicity, the latter formula is more than useful in the computation of residues at first order poles.

[edit] 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 + \sin1\right) + \cdots.

So the residue of f(z) at z = 1 is sin 1.

[edit] See also

[edit] External links

[edit] References

  • Ahlfors, Lars (1979). Complex Analysis. McGraw Hill. 
  • Marsden & Hoffman, Basic complex analysis (Freeman, 1999).