Math 2.0

Functions of a complex variable Theorem

Bürmann–Lagrange series

Builds on Holomorphic functionTaylor seriesLagrange inversion theorem

Statement

Let gg be a holomorphic function on a neighbourhood of a point a∈ℂa \in \C with g′(a)≠0g'(a) \ne 0, and let b=g(a)b = g(a). Let HH be holomorphic on a neighbourhood of aa. Put φ(z)=z−ag(z)−b\varphi(z) = \dfrac{z - a}{g(z) - b} for z≠az \ne a and φ(a)=1/g′(a)\varphi(a) = 1/g'(a), which is holomorphic near aa. Then there is a neighbourhood UU of aa such that for all z∈Uz \in U H(z)=H(a)+∑n=1∞cnn!(g(z)−b)n,cn=d n−1dz n−1[H′(z) φ(z)n]z=a,H(z) = H(a) + \sum_{n=1}^{\infty} \frac{c_n}{n!} \big( g(z) - b \big)^n, \qquad c_n = \frac{d^{\,n-1}}{dz^{\,n-1}} \Big[ H'(z)\, \varphi(z)^n \Big]_{z = a}, and the series converges absolutely on UU.

Remarks

Proof idea: since g′(a)≠0g'(a) \ne 0, the function gg has a holomorphic inverse g−1g^{-1} near bb. The series is the Taylor series of w↦H(g−1(w))w \mapsto H(g^{-1}(w)) at w=bw = b, evaluated at w=g(z)w = g(z). Its coefficients are found by Cauchy's integral formula for derivatives, followed by the change of variable w=g(z)w = g(z). An integration by parts then turns the integral into a residue at z=az = a.

With H(z)=zH(z) = z the series is the classical Lagrange inversion formula for g−1g^{-1}. Example: g(z)=ze−zg(z) = z e^{-z} and a=0a = 0, so φ(z)=ez\varphi(z) = e^{z} and cn=d n−1dz n−1enz∣z=0=nn−1c_n = \frac{d^{\,n-1}}{dz^{\,n-1}} e^{nz} \big|_{z=0} = n^{n-1}. So the inverse of ze−zz e^{-z} near 00 is ∑n≥1nn−1n!wn\sum_{n \ge 1} \frac{n^{n-1}}{n!} w^n, which is −W(−w)-W(-w) for the Lambert W function.

The hypothesis g′(a)≠0g'(a) \ne 0 is needed: for g(z)=z2g(z) = z^2 and a=0a = 0 the function H(z)=zH(z) = z is not a power series in g(z)=z2g(z) = z^2, since zz is odd. The formal version for power series over a field of characteristic 00 is the Lagrange inversion theorem.

Going deeper

For a student

The series is the analytic form of Lagrange inversion. It gives the Taylor coefficients of an inverse function, for example of the solution w(z)w(z) of Kepler's equation or of the Lambert WW function. In asymptotic analysis it is used to change variables near a critical point. For instance, it reduces an integral in Laplace's method to a Gaussian form with an explicit series of corrections. The combinatorial version, for formal power series, is the Lagrange inversion theorem, which counts trees.

Reading path

To understand this page from the ground up, read these 7 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
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  1. Coefficient of a power series concept
  2. Formal power series concept
  3. Generating function concept
  4. Holomorphic function concept
  5. Taylor series concept
  6. Lagrange inversion theorem statement
  7. Bürmann–Lagrange series statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Lagrange_inversion_theorem, Lagrange–Bürmann formula
About this page
TagTPB4F1VY4Z
URIm2://TPB4F1VY4Z
Kindstatement, theorem
WritingW0 stub
MSC30B10, 41A58
StatusThis copy of the site has no build data. Run m2 status TPB4F1VY4Z.
AboutHolomorphic function
UsesHolomorphic function, Taylor series, Lagrange inversion theorem

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