Namespaces
Variants
Actions

Harmonic measure, principle of

From Encyclopedia of Mathematics
Jump to: navigation, search
The printable version is no longer supported and may have rendering errors. Please update your browser bookmarks and please use the default browser print function instead.


The harmonic measure does not decrease under mappings realized by single-valued analytic functions. If $ \omega ( z; \alpha , D) $ is the harmonic measure of a boundary set $ \alpha $ with respect to a domain $ D $ in the complex $ z $- plane, one specific formulation of the principle of harmonic measure is as follows. In a domain $ D _ {z} $ with boundary $ \Gamma _ {z} $ consisting of a finite number of Jordan arcs let there be given a single-valued analytic function $ w = w( z) $ which satisfies the following conditions: the values $ w = w( z) $, $ z \in D _ {z} $, form part of the domain $ D _ {w} $ with boundary $ \Gamma _ {w} $ consisting of a finite number of Jordan arcs; the function $ w( z) $ can be continuously extended onto some set $ \alpha _ {z} \subset \Gamma _ {z} $ consisting of a finite number of arcs; and the values of $ w( z) $ on $ \alpha _ {z} $ form part of a set $ E \subset \overline{D}\; _ {w} $ with boundary $ \partial E $ consisting of a finite number of Jordan arcs. Under these conditions one has, at any point $ z \in D _ {z} $ at which $ w( z) \notin E $,

$$ \tag{1 } \omega ( z; \alpha _ {z} , D _ {z} ) \leq \ \omega ( w ( z); \partial E, D _ {w} ^ {*} ), $$

where $ D _ {w} ^ {*} $ denotes the subdomain of $ D _ {w} $ such that $ w( z) \in D _ {w} ^ {*} $ and $ \partial D _ {w} ^ {*} \subset \Gamma _ {w} \cup \partial E $. If (1) becomes an equality at any point $ z $, then equality will be valid everywhere in $ D _ {z} $. In particular, for a one-to-one conformal mapping from $ D _ {z} $ onto $ D _ {w} $ one has the identity

$$ \omega ( z; \alpha _ {z} , D _ {z} ) \equiv \ \omega ( w ( z); \alpha _ {w} , D _ {w} ). $$

The principle of harmonic measure, including its numerous applications [1], [2], was established by R. Nevanlinna. In particular, a corollary of the principle is the two-constants theorem, which implies, in turn, that for a function $ w( z) $ that is holomorphic in a domain $ D _ {z} $, the maximum value of $ \mathop{\rm ln} w( z) $ on the level line $ \{ {z } : {\omega ( z ; \alpha _ {z} , D _ {z} ) = t } \} $ is a convex function of the parameter $ t \in ( 0, 1) $.

The principle of harmonic measure has been generalized to holomorphic functions $ w = w( z) $, $ z = ( z _ {1} \dots z _ {n} ) $, of several complex variables, $ n \geq 1 $.

References

[1] F. Nevanlinna, R. Nevanlinna, "Ueber die Eigenschaften einer analytischen Funktion in der Umgebung einer singulären Stelle oder Linie" Acta Soc. Sci. Fennica , 50 : 5 (1922) pp. 1–46
[2] R. Nevanilinna, "Analytic functions" , Springer (1970) (Translated from German)
How to Cite This Entry:
Harmonic measure, principle of. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Harmonic_measure,_principle_of&oldid=47183
This article was adapted from an original article by P.M. Tamrazov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article