Difference between revisions of "Two-constants theorem"
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− | + | Let $ D $ | |
+ | be a finitely-connected Jordan domain in the $ z $- | ||
+ | plane and let $ w ( z) $ | ||
+ | be a regular analytic function in $ D $ | ||
+ | satisfying the inequality $ | w ( z) | \leq M $, | ||
+ | as well as the relation | ||
− | < | + | $$ |
+ | \lim\limits _ {z \rightarrow \zeta } \sup | w ( z) | \leq \ | ||
+ | m < M ,\ z \in D ,\ \zeta \in \alpha , | ||
+ | $$ | ||
− | + | on some arc $ \alpha $ | |
+ | of the boundary $ \partial D $. | ||
+ | Then, at each point $ z $ | ||
+ | of the set | ||
− | + | $$ | |
+ | \{ {z \in D } : {0 < \lambda \leq \omega ( z ; \alpha , D ) < 1 } \} | ||
+ | , | ||
+ | $$ | ||
− | + | where $ \omega ( z ; \alpha , D ) $ | |
+ | is the [[Harmonic measure|harmonic measure]] of the arc $ \alpha $ | ||
+ | with respect to $ D $ | ||
+ | at $ z $, | ||
+ | the inequality | ||
− | + | $$ | |
+ | | w ( z) | \leq m ^ \lambda \cdot M ^ {1- \lambda } | ||
+ | $$ | ||
− | + | is satisfied. If for some $ z $( | |
+ | satisfying the condition $ \omega ( z ; \alpha , D ) = \lambda $) | ||
+ | equality is attained, equality will hold for all $ z \in D $ | ||
+ | and for all $ \lambda $, | ||
+ | $ 0 \leq \lambda \leq 1 $, | ||
+ | while the function $ w ( z) $ | ||
+ | in this case has the form | ||
+ | |||
+ | $$ | ||
+ | w ( z) = e ^ {ia } m ^ {\phi ( z) } M ^ {1 - \phi ( z) } , | ||
+ | $$ | ||
+ | |||
+ | where $ a $ | ||
+ | is a real number and $ \phi ( z) $ | ||
+ | is an analytic function in $ D $ | ||
+ | for which $ \mathop{\rm Re} \phi ( z) = \omega ( z ; \alpha , D ) $[[#References|[1]]], [[#References|[2]]]. | ||
The two-constants theorem gives a quantitative expression of the unique determination of analytic functions by their boundary values and has important applications in the theory of functions [[#References|[3]]]. Hadamard's three-circles theorem (cf. [[Hadamard theorem|Hadamard theorem]]) is obtained from it as a special case. For possible analogues of the two-constants theorem for harmonic functions in space see [[#References|[4]]], [[#References|[5]]]. | The two-constants theorem gives a quantitative expression of the unique determination of analytic functions by their boundary values and has important applications in the theory of functions [[#References|[3]]]. Hadamard's three-circles theorem (cf. [[Hadamard theorem|Hadamard theorem]]) is obtained from it as a special case. For possible analogues of the two-constants theorem for harmonic functions in space see [[#References|[4]]], [[#References|[5]]]. | ||
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====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> F. Nevanlinna, R. Nevanlinna, "Über die Eigenschaften einer analytischen Funktion in der Umgebung einer singulären Stelle oder Linie" ''Acta Soc. Sci. Fennica'' , '''5''' : 5 (1922)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> A. Ostrowski, "Über allgemeine Konvergenzsätze der komplexen Funktionentheorie" ''Jahresber. Deutsch. Math.-Ver.'' , '''32''' : 9–12 (1923) pp. 185–194</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> R. Nevanilinna, "Analytic functions" , Springer (1970) (Translated from German)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> S.N. Mergelyan, "Harmonic approximation and approximate solution of the Cauchy problem for the Laplace equation" ''Uspekhi Mat. Nauk'' , '''11''' : 5 (1956) pp. 3–26 (In Russian)</TD></TR><TR><TD valign="top">[5]</TD> <TD valign="top"> E.D. Solomentsev, "Three-spheres theorem for harmonic functions" ''Dokl. Akad. Nauk ArmSSR'' , '''42''' : 5 (1966) pp. 274–278 (In Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> F. Nevanlinna, R. Nevanlinna, "Über die Eigenschaften einer analytischen Funktion in der Umgebung einer singulären Stelle oder Linie" ''Acta Soc. Sci. Fennica'' , '''5''' : 5 (1922)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> A. Ostrowski, "Über allgemeine Konvergenzsätze der komplexen Funktionentheorie" ''Jahresber. Deutsch. Math.-Ver.'' , '''32''' : 9–12 (1923) pp. 185–194</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> R. Nevanilinna, "Analytic functions" , Springer (1970) (Translated from German)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> S.N. Mergelyan, "Harmonic approximation and approximate solution of the Cauchy problem for the Laplace equation" ''Uspekhi Mat. Nauk'' , '''11''' : 5 (1956) pp. 3–26 (In Russian)</TD></TR><TR><TD valign="top">[5]</TD> <TD valign="top"> E.D. Solomentsev, "Three-spheres theorem for harmonic functions" ''Dokl. Akad. Nauk ArmSSR'' , '''42''' : 5 (1966) pp. 274–278 (In Russian)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | There is a more general | + | There is a more general $ n $- |
+ | constants theorem, [[#References|[a2]]]: Let $ f( z) $ | ||
+ | be holomorphic in a domain $ D $ | ||
+ | whose boundary is the union of $ n $ | ||
+ | distinct rectifiable arcs $ \alpha _ {1} \dots \alpha _ {n} $; | ||
+ | suppose that for each $ j $ | ||
+ | there is a constant $ M _ {j} $ | ||
+ | such that if $ z $ | ||
+ | approaches any point of $ \alpha _ {j} $, | ||
+ | then the limits of $ f ( z) $ | ||
+ | do not exceed $ M _ {j} $ | ||
+ | in absolute value. Then for each $ z \in D $, | ||
− | + | $$ | |
+ | \mathop{\rm log} | f( z) | \leq \sum_{j=1} ^ { m } | ||
+ | \omega ( z, \alpha _ {j} ; D) \mathop{\rm log} M _ {j} . | ||
+ | $$ | ||
====References==== | ====References==== | ||
− | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> A.I. Markushevich, "Theory of functions of a complex variable" , '''2''' , Chelsea (1977) pp. 210–214 (Translated from Russian)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> E. Hille, "Analytic function theory" , '''2''' , Chelsea, reprint (1987) pp. 409–410</TD></TR></table> | + | <table> |
+ | <TR><TD valign="top">[a1]</TD> <TD valign="top"> A.I. Markushevich, "Theory of functions of a complex variable" , '''2''' , Chelsea (1977) pp. 210–214 (Translated from Russian)</TD></TR> | ||
+ | <TR><TD valign="top">[a2]</TD> <TD valign="top"> E. Hille, "Analytic function theory" , '''2''' , Chelsea, reprint (1987) pp. 409–410</TD></TR> | ||
+ | </table> |
Latest revision as of 19:15, 11 January 2024
Let $ D $
be a finitely-connected Jordan domain in the $ z $-
plane and let $ w ( z) $
be a regular analytic function in $ D $
satisfying the inequality $ | w ( z) | \leq M $,
as well as the relation
$$ \lim\limits _ {z \rightarrow \zeta } \sup | w ( z) | \leq \ m < M ,\ z \in D ,\ \zeta \in \alpha , $$
on some arc $ \alpha $ of the boundary $ \partial D $. Then, at each point $ z $ of the set
$$ \{ {z \in D } : {0 < \lambda \leq \omega ( z ; \alpha , D ) < 1 } \} , $$
where $ \omega ( z ; \alpha , D ) $ is the harmonic measure of the arc $ \alpha $ with respect to $ D $ at $ z $, the inequality
$$ | w ( z) | \leq m ^ \lambda \cdot M ^ {1- \lambda } $$
is satisfied. If for some $ z $( satisfying the condition $ \omega ( z ; \alpha , D ) = \lambda $) equality is attained, equality will hold for all $ z \in D $ and for all $ \lambda $, $ 0 \leq \lambda \leq 1 $, while the function $ w ( z) $ in this case has the form
$$ w ( z) = e ^ {ia } m ^ {\phi ( z) } M ^ {1 - \phi ( z) } , $$
where $ a $ is a real number and $ \phi ( z) $ is an analytic function in $ D $ for which $ \mathop{\rm Re} \phi ( z) = \omega ( z ; \alpha , D ) $[1], [2].
The two-constants theorem gives a quantitative expression of the unique determination of analytic functions by their boundary values and has important applications in the theory of functions [3]. Hadamard's three-circles theorem (cf. Hadamard theorem) is obtained from it as a special case. For possible analogues of the two-constants theorem for harmonic functions in space see [4], [5].
References
[1] | F. Nevanlinna, R. Nevanlinna, "Über die Eigenschaften einer analytischen Funktion in der Umgebung einer singulären Stelle oder Linie" Acta Soc. Sci. Fennica , 5 : 5 (1922) |
[2] | A. Ostrowski, "Über allgemeine Konvergenzsätze der komplexen Funktionentheorie" Jahresber. Deutsch. Math.-Ver. , 32 : 9–12 (1923) pp. 185–194 |
[3] | R. Nevanilinna, "Analytic functions" , Springer (1970) (Translated from German) |
[4] | S.N. Mergelyan, "Harmonic approximation and approximate solution of the Cauchy problem for the Laplace equation" Uspekhi Mat. Nauk , 11 : 5 (1956) pp. 3–26 (In Russian) |
[5] | E.D. Solomentsev, "Three-spheres theorem for harmonic functions" Dokl. Akad. Nauk ArmSSR , 42 : 5 (1966) pp. 274–278 (In Russian) |
Comments
There is a more general $ n $- constants theorem, [a2]: Let $ f( z) $ be holomorphic in a domain $ D $ whose boundary is the union of $ n $ distinct rectifiable arcs $ \alpha _ {1} \dots \alpha _ {n} $; suppose that for each $ j $ there is a constant $ M _ {j} $ such that if $ z $ approaches any point of $ \alpha _ {j} $, then the limits of $ f ( z) $ do not exceed $ M _ {j} $ in absolute value. Then for each $ z \in D $,
$$ \mathop{\rm log} | f( z) | \leq \sum_{j=1} ^ { m } \omega ( z, \alpha _ {j} ; D) \mathop{\rm log} M _ {j} . $$
References
[a1] | A.I. Markushevich, "Theory of functions of a complex variable" , 2 , Chelsea (1977) pp. 210–214 (Translated from Russian) |
[a2] | E. Hille, "Analytic function theory" , 2 , Chelsea, reprint (1987) pp. 409–410 |
Two-constants theorem. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Two-constants_theorem&oldid=12855