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The Transfer Operator Approach to Selberg’s Zeta Function and Modular and Maass Wave Forms For P S L (2, ℤ)

Identifieur interne : 000387 ( Istex/Corpus ); précédent : 000386; suivant : 000388

The Transfer Operator Approach to Selberg’s Zeta Function and Modular and Maass Wave Forms For P S L (2, ℤ)

Auteurs : Cheng-Hung Chang ; Dieter H. Mayer

Source :

RBID : ISTEX:1273B34EC314C75A1F671BC13B8218FFBE44FE97

Abstract

Abstract: In this paper we discuss the transfer operator approach to Selberg’s zeta function for P S L(2, ℤ). Since this function can be expressed as the Fredholm determinant det(1 - L β ) of the transfer operator L β , β ∈ C for the geodesic flow on the modular surface, the zeros and poles of the Selberg function are closely related to those β-values, where L β has an eigenvalue λ = 1 respectively where L β has poles. It turns out that the corresponding eigenfunctions of L β for eigenvalues λ = 1 are closely related to both holomorphic and non-holomorphic modular forms respectively the Maass wave forms. Therefore these eigenfunctions, which by definition of L β are holomorphic functions, are by themselves interesting quantities for the group P S L (2, ℤ): indeed special cases are the period polynomials and functions of the Manin-Eichler and Shimura theory of periods for this group. Another special example of such an eigenfunction is the well known density of Gauss’s measure for the continued fraction expansion. The transfer operator approach hence in a surprising way combines several aspects of the theory of modular and Maass wave forms for the modular group, which up to now were not directly related.

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DOI: 10.1007/978-1-4612-1544-8_3

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ISTEX:1273B34EC314C75A1F671BC13B8218FFBE44FE97

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<ChapterTitle Language="En">The Transfer Operator Approach to Selberg’s Zeta Function and Modular and Maass Wave Forms For
<Emphasis Type="Italic">P S L</Emphasis>
(2, ℤ)</ChapterTitle>
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<AuthorName DisplayOrder="Western">
<GivenName>Cheng-Hung</GivenName>
<FamilyName>Chang</FamilyName>
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<AuthorName DisplayOrder="Western">
<GivenName>Dieter</GivenName>
<GivenName>H.</GivenName>
<FamilyName>Mayer</FamilyName>
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<OrgName>Institut für Theoretische Physik C, TU Clausthal</OrgName>
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<Country>Germany</Country>
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<Abstract ID="Abs1" Language="En" OutputMedium="All">
<Heading>Abstract</Heading>
<Para>In this paper we discuss the transfer operator approach to Selberg’s zeta function for
<Emphasis Type="Italic">P S L</Emphasis>
(2, ℤ). Since this function can be expressed as the Fredholm determinant
<Emphasis Type="Italic">det</Emphasis>
(1 -
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
) of the transfer operator
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
,
<Emphasis Type="Italic">β</Emphasis>
<Emphasis Type="Italic">C</Emphasis>
for the geodesic flow on the modular surface, the zeros and poles of the Selberg function are closely related to those
<Emphasis Type="Italic">β-</Emphasis>
values, where
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
has an eigenvalue λ = 1 respectively where
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
has poles. It turns out that the corresponding eigenfunctions of
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
for eigenvalues λ = 1 are closely related to both holomorphic and non-holomorphic modular forms respectively the Maass wave forms. Therefore these eigenfunctions, which by definition of
<Emphasis Type="Italic">L</Emphasis>
<Subscript>
<Emphasis Type="Italic">β</Emphasis>
</Subscript>
are holomorphic functions, are by themselves interesting quantities for the group
<Emphasis Type="Italic">P S L</Emphasis>
(2, ℤ): indeed special cases are the period polynomials and functions of the Manin-Eichler and Shimura theory of periods for this group. Another special example of such an eigenfunction is the well known density of Gauss’s measure for the continued fraction expansion. The transfer operator approach hence in a surprising way combines several aspects of the theory of modular and Maass wave forms for the modular group, which up to now were not directly related.</Para>
</Abstract>
<KeywordGroup Language="En">
<Heading>Key words</Heading>
<Keyword>quantum chaos</Keyword>
<Keyword>Selberg zeta function</Keyword>
<Keyword>dynamical zeta function</Keyword>
<Keyword>transfer operator</Keyword>
<Keyword>functional equation</Keyword>
<Keyword>modular forms</Keyword>
<Keyword>Maass wave forms</Keyword>
<Keyword>period polynomial</Keyword>
<Keyword>period function</Keyword>
</KeywordGroup>
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<SimplePara>The work is supported by DFG Schwerpunktprogramm “Ergodentheorie, Analysis und effiziente Simulation dynamischer Systeme”.</SimplePara>
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<abstract lang="en">Abstract: In this paper we discuss the transfer operator approach to Selberg’s zeta function for P S L(2, ℤ). Since this function can be expressed as the Fredholm determinant det(1 - L β ) of the transfer operator L β , β ∈ C for the geodesic flow on the modular surface, the zeros and poles of the Selberg function are closely related to those β-values, where L β has an eigenvalue λ = 1 respectively where L β has poles. It turns out that the corresponding eigenfunctions of L β for eigenvalues λ = 1 are closely related to both holomorphic and non-holomorphic modular forms respectively the Maass wave forms. Therefore these eigenfunctions, which by definition of L β are holomorphic functions, are by themselves interesting quantities for the group P S L (2, ℤ): indeed special cases are the period polynomials and functions of the Manin-Eichler and Shimura theory of periods for this group. Another special example of such an eigenfunction is the well known density of Gauss’s measure for the continued fraction expansion. The transfer operator approach hence in a surprising way combines several aspects of the theory of modular and Maass wave forms for the modular group, which up to now were not directly related.</abstract>
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