Laurent Series

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Introduction

The Laurent series (named after Pierre Alphonse Laurent) is an infinite series similar to a power series but additionally includes negative exponents. In general, a Laurent series in x with development point c has the following form:

f(x)=n=cn(xa)n
  • cn coefficients
  • a development point of series

Main Part and Regular Part

The series of terms with negative exponents is called the main part of the Laurent series, and the series of terms with non-negative exponents is called the regular part or the residual part.

Connection to Power Series

A Laurent series with a vanishing main part is a power series; if it also has only finitely many terms, then it is a polynomial. If a Laurent series has only finitely many terms in total (with negative or positive exponents), it is called a Laurent polynomial.

History

The Laurent series was introduced in 1843 by the French mathematician Pierre Alphonse Laurent. However, notes in the legacy of the German mathematician Karl Weierstrass suggest that he discovered it as early as 1841.

Laurent Decomposition

The principle of developing a holomorphic function into a Laurent series is based on the Laurent decomposition. To do this, consider an annular region =z;|;r<|z|<R. Now define two holomorphic functions g and h:

g:UR(0)
h:U1r(0).

Representation of Laurent Series by Two Holomorphic Functions

Let g:G and h:G be two holomorphic functions with a development point z0G,

f(z):=g(zz0)+h^(zz0) with h^(z):=h(1/z).

g and h are holomorphic functions on G0:=zz0 | zG, which can be developed into a power series around 0 in G0.

Convergence Set of Laurent Series

The functions g and h can be locally represented as a power series on a disk in Go:=zzo | zG (holomorphy criterion). Then h^ with h^(z):=h(1/z) converges on the complement of a disk.

Intersection of Convergence Domains

If f(z)'s principal part g(z) and h^(z) are convergent, then z lies in the intersection of the convergence sets. If r>R, the convergence set is empty because z would simultaneously have to lie on a disk of radius R and on the complement of a disk with radius r.

Convergence Radii

Let Rg>0 and Rh>0 be the convergence radii for the functions g and h. Calculate the radius Rh^>0 of the convergence set of h^(z):=h(1/z) for all zGo with |z|>Rh^>0.

Geometry of the Convergence Set

h converges holomorphically around the center on the disk with radius 1/r. Since the argument of the function h must lie within the defined circular region, it quickly becomes evident that the function h(1/z) is defined for values |z|>r. Thus, the sum of the two functions

f(z)=g(z)+h(1z)

is analytic on the annulus .

Uniqueness of Decomposition

It can be shown that any holomorphic function on an annular domain can be decomposed in this way. If one also assumes h(0)=0, the decomposition is unique.

By expanding this function in the form of power series, the following representation arises:

f(z)=g(z)+h(1z)=n=0anzn+n=1bnzn=n=anzn.

Here, bnan is defined. Additionally, b0=0 follows from the condition h(0)=0.

Decomposition with Expansion Point

If these considerations are extended to an expansion around a point c, rather than the origin, the initially stated definition of the Laurent series for a holomorphic function f around the expansion point c results:

f(z)=n=an(zc)n

Example

In the following, 𝕂 refers to either the real numbers or the complex numbers.

f:𝕂𝕂:x{exp(1x2),x0 0,otherwise.

The function is infinitely often differentiable in the real sense, but it is not holomorphic at x=0, where it has an essential singularity.

Substituting into the Taylor Series

By substituting z=1x2 into the power series expansion of the exponential function,

ez=n=0znn!=n=0(1x2)nn!

the Laurent series of f with the expansion point 0 is obtained:

f(x)=n=0(1)nx2nn!=n=1(1)n(n)!x2nPrincipal part+1

Convergence Domain of the Laurent Series

The secondary part g(x)=1 converges throughout , and the principal part (and therefore the entire Laurent series) converges for every complex number x0.

Approximation of the Function by Partial Sums

Approximation of Laurent series by partial sums

The image shows how the partial sum sequence

fn(x)=j=0n(1)jx2jj!

approaches the function.

Comparison of Graphs of Partial Sums with the Function

Approximation of Laurent series by partial sums.

Since graphs in are subsets of 4-dimensional -vector spaces, the graph is plotted here for values x0. The Laurent expansion can be continuously extended at 0.

Convergence of Laurent Series

Laurent series are important tools in Complex Analysis, especially for studying functions with isolated singularities.

Annuli and Disks

Laurent series describe complex functions that are holomorphic on an annulus, just as power series describe functions holomorphic on a disk.

Let

n=an(zc)n

be a Laurent series in z with complex coefficients an and expansion point c.

Convergence Radii - Interior of the Annulus

There are two uniquely determined numbers r and R such that:

The Laurent series converges Normal convergence and Absolute convergence on the open annulus A:=z:r<|zc|<R.

It converges normally, meaning the principal and secondary parts converge normally. This defines a holomorphic function f on A.

Outside the Annulus

Outside the annulus, the Laurent series diverges. For every point in

A:=z:r>|zc||zc|>R,

either the terms with positive (secondary part) or negative exponents (principal part) diverge.

Convergence Radii and Cauchy-Hadamard

The two radii can be calculated using the Cauchy-Hadamard formula:

r=lim supn|an|1/n
R=1lim supn|an|1/n

We set 10= and 1=0 in the second formula.

Functions Defined on Annuli

Conversely, one can start with an annulus A:=z:r<|zc|<R and a function f that is holomorphic on A. Then, there always exists a uniquely determined Laurent series with expansion point c that converges (at least) on A and coincides with f there. The coefficients satisfy:

an=12πiUϱ(c)f(ζ)(ζc)n+1dζ

for all n and a ϱ(r,R). Due to the Cauchy integral theorem, the choice of ϱ does not matter.

Punctured Disk

The case r=0, i.e., a holomorphic function f on a punctured disk around c, is particularly important. The coefficient a1 in the Laurent series expansion of f is called the residue of f at the isolated singularity c. It plays a significant role in the residue theorem.

Formal Laurent Series

Formal Laurent series are Laurent series in the indeterminate X, used without consideration of convergence.

Laurent Series on Commutative Rings

The coefficients ak can then belong to any Commutative Ring. In this context, it only makes sense to consider Laurent series with finitely many negative exponents, known as a "finite principal part," and to omit the expansion point by setting c=0.

Equality of Formal Laurent Series

Two such formal Laurent series are defined as equal if and only if all their coefficients agree. Laurent series are added by summing their respective coefficients. Since there are only finitely many terms with negative exponents, they can be multiplied by Convolution of their coefficient sequences, similar to power series. With these operations, the set of all Laurent series over a commutative ring R forms a commutative ring, denoted by R(!(X)!).

Laurent Series and Integral Domains

If K is a field, the formal power series in the indeterminate X over K form an integral domain, denoted by K[![X]!]. Its field of fractions is isomorphic to the field K(!(X)!) of Laurent series over K.

Exercises

Let Kr1,r2:=z,|,r1<|z|<r2. Construct a Laurent series with this annulus as its domain of convergence, which does not converge on Kr1,r2. Use geometric series as an idea with n=0+qn converging for q when |q|<1.

Exercises on Laurent Series and b-adic Number Systems

Analyze the relationship between Laurent series and the p-adic number system (e.g., binary system, hexadecimal system)! What are the similarities and differences?

Represent the number 17 as a value of a Laurent series in the 4-based number system x=4, where cn0,1,2,3. Calculate the coefficients cn:

f(x):=n=+cnznz

Literature

Eberhard Freitag & Rolf Busam: Complex Analysis 1, Springer-Verlag, Berlin, ISBN 3-540-67641-4

See Also

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