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In mathematics, a '''Maass wave form''' is a function on the [[upper half plane]] that transforms like a [[modular form]] but need not be [[Holomorphic function|holomorphic]]. They were first studied by [[Hans Maass]] in {{harvtxt|Maass|1949}}.
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==Definition==
A '''Maass wave form''' is defined to be a continuous complex-valued function ''f'' of &tau; = ''x'' + ''iy'' in the upper half plane satisfying the following conditions:
*''f'' is invariant under the action of the group [[Modular group|SL<sub>2</sub>('''Z''')]] on the upper half plane.
*''f'' is an [[eigenvector]] of the [[Laplacian operator]] <math>-y^2\left(\frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2}\right).</math>
*''f'' is of at most polynomial growth at [[Cusp form|cusps]] of SL<sub>2</sub>('''Z''').
 
A '''weak Maass wave form''' is defined similarly but without the growth condition at cusps.
 
==See also==
*[[Mock modular form]]
*[[Real analytic Eisenstein series]]
 
==References==
*{{Citation | last1=Bump | first1=Daniel | title=Automorphic forms and representations | publisher=[[Cambridge University Press]] | series=Cambridge Studies in Advanced Mathematics | isbn=978-0-521-55098-7 | id={{MathSciNet | id = 1431508}} | year=1997 | volume=55}}
*{{Citation | last1=Maass | first1=Hans | authorlink=Hans Maass|title=Über eine neue Art von nichtanalytischen automorphen Funktionen und die Bestimmung Dirichletscher Reihen durch Funktionalgleichungen | doi=10.1007/BF01329622 | id={{MathSciNet | id = 0031519}} | year=1949 | journal=[[Mathematische Annalen]] | volume=121 | pages=141–183}}
 
[[Category:Modular forms]]

Latest revision as of 00:27, 29 July 2014

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