Poisson transformation

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In mathematics , the Poisson transformation is a method for constructing harmonic functions on the unit disk . The integral that appears in this construction is called the Poisson integral and the integral kernel of this is called the Poisson kernel . The transformation, the integral and the integral kernel are named after the mathematician and physicist Siméon Denis Poisson .

Problem

A (limited) function is given on the unit circle , a (limited) harmonic function is sought on the unit disk whose values ​​on the edge match the given function .

In other words: it is supposed to be the Dirichlet problem for the Laplace equation

be solved on the circular disc.

construction

The Poisson core is the through

given function.

The Poisson transformation is the integral transformation with integral kernel : a function becomes the function defined on

assigned, wherein the uniform probability to designated.

One can show that is a bounded harmonic function.

Bijection

The Poisson transform creates a bijection between the set of bounded functions on and the set of bounded harmonic functions on .

In other words: for every function there is a unique harmonic function with boundary values .

The bijection receives the norm.

Generalizations

The Poisson transformation can be generalized to the n-dimensional unit sphere , in this case the Poisson kernel is for .

literature

  • Helgason, Sigurdur: Topics in harmonic analysis on homogeneous spaces. Progress in Mathematics, 13. Birkhauser, Boston, Mass., 1981. ISBN 3-7643-3051-1
  • Quint, J.-F .: An overview of Patterson-Sullivan theory , Workshop "The barycenter method", FIM, Zurich, May 2006 (Online)

Individual evidence

  1. Poisson integral . In: Guido Walz (Ed.): Lexicon of Mathematics . 1st edition. Spectrum Academic Publishing House, Mannheim / Heidelberg 2000, ISBN 3-8274-0439-8 .
  2. ^ Poisson core . In: Guido Walz (Ed.): Lexicon of Mathematics . 1st edition. Spectrum Academic Publishing House, Mannheim / Heidelberg 2000, ISBN 3-8274-0439-8 .