Period functions for Maass wave forms. I.

By John S. Lewis, Don Zagier. 2001

211 citations recorded by the source corpus.

Recall that a Maass wave form on the full modular group Gamma=PSL(2,Z) is a smooth gamma-invariant function u from the upper half-plane H = {x+iy | y>0} to C which is small as y \to \infty and satisfies Delta u = lambda u for some lambda \in C, where Delta = y^2(d^2/dx^2 + d^2/dy^2) is the hyperbolic Laplacian. These functions give a basis for L_2 on the modular surface Gamma\H, with the usual trigonometric waveforms on the torus R^2/Z^2, which are also (for this surface) both the Fourier building blocks for L_2 and eigenfunctions of the Laplacian. Although therefore very basic objects, Maass forms nevertheless still remain mysteriously elusive fifty years after their discovery; in particular, no explicit construction exists for any of these functions for the full modular group. The basic information about them (e.g. their existence and the density of the eigenvalues) comes mostly from the Selberg trace formula: the rest is conjectural with support from extensive numerical computations.

Subfields: Algebra and Number Theory, Mathematical Physics, Statistical and Nonlinear Physics

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In Algebra and Number Theory

  1. Tudor Dimofte
  2. Don Zagier
  3. Yuri I. Manin
  4. S. Bettin
  5. Masanobu Kaneko
  6. Brianna L. Conrey
  7. Herbert Gangl
  8. F. Brown

In Mathematical Physics

  1. Tudor Dimofte
  2. Brianna L. Conrey
  3. S. Bettin
  4. Yuri I. Manin
  5. Don Zagier
  6. Masanobu Kaneko
  7. Herbert Gangl
  8. Sergei Gukov

In Statistical and Nonlinear Physics

  1. Tudor Dimofte
  2. Yuri I. Manin
  3. S. Bettin
  4. Brianna L. Conrey
  5. Don Zagier

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