Jump to content

Polar set (potential theory)

From Wikipedia, the free encyclopedia

This is an old revision of this page, as edited by Spectral sequence (talk | contribs) at 18:26, 22 July 2013 (Nearly everywhere: cite Ransford (1995)). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

In mathematics, in the area of classical potential theory, polar sets are the "negligible sets", similar to the way in which sets of measure zero are the negligible sets in measure theory.

Definition

A set in (where ) is a polar set if there is a non-constant subharmonic function

on

such that

Note that there are other (equivalent) ways in which polar sets may be defined, such as by replacing "subharmonic" by "superharmonic", and by in the definition above.

Properties

The most important properties of polar sets are:

  • A singleton set in is polar.
  • A countable set in is polar.
  • The union of a countable collection of polar sets is polar.
  • A polar set has Lebesgue measure zero in

Nearly everywhere

A property holds nearly everywhere in a set S if it holds on SE where E is a Borel polar set. If P holds nearly everywhere then it holds almost everywhere.[1]

See also

References

  1. ^ Ransford (1995) p.56
  • Doob, Joseph L. (1984). Classical Potential Theory and Its Probabilistic Counterpart. Grundlehren der Mathematischen Wissenschaften. Vol. 262. Berlin Heidelberg New York: Springer-Verlag. ISBN 3-540-41206-9. Zbl 0549.31001.
  • Helms, L. L. (1975). Introduction to potential theory. R. E. Krieger. ISBN 0-88275-224-3.
  • Ransford, Thomas (1995). Potential theory in the complex plane. London Mathematical Society Student Texts. Vol. 28. Cambridge: Cambridge University Press. ISBN 0-521-46654-7. Zbl 0828.31001.