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19 April 2024
 
  » arxiv » 1905.4112

 Article overview


The Fourier transform on harmonic manifolds of purely exponential volume growth
Kingshook Biswas ; Gerhard Knieper ; Norbert Peyerimhoff ;
Date 8 May 2019
AbstractLet $X$ be a complete, simply connected harmonic manifold of purely exponential volume growth. This class contains all non-flat harmonic manifolds of non-positive curvature and, in particular all known examples of harmonic manifolds except for the flat spaces.
Denote by $h > 0$ the mean curvature of horospheres in $X$, and set $ ho = h/2$. Fixing a basepoint $o in X$, for $xi in partial X$, denote by $B_{xi}$ the Busemann function at $xi$ such that $B_{xi}(o) = 0$. then for $lambda in C$ the function $e^{(ilambda - ho)B_{xi}}$ is an eigenfunction of the Laplace-Beltrami operator with eigenvalue $-(lambda^2 + ho^2)$.
For a function $f$ on $X$, we define the Fourier transform of $f$ by $$ ilde{f}(lambda, xi) := int_X f(x) e^{(-ilambda - ho)B_{xi}(x)} dvol(x)$$ for all $lambda in C, xi in partial X$ for which the integral converges. We prove a Fourier inversion formula $$f(x) = C_0 int_{0}^{infty} int_{partial X} ilde{f}(lambda, xi) e^{(ilambda - ho)B_{xi}(x)} dlambda_o(xi) |c(lambda)|^{-2} dlambda$$ for $f in C^{infty}_c(X)$, where $c$ is a certain function on $mathbb{R} - {0}$, $lambda_o$ is the visibility measure on $partial X$ with respect to the basepoint $o in X$ and $C_0 > 0$ is a constant. We also prove a Plancherel theorem, and a version of the Kunze-Stein phenomenon.
Source arXiv, 1905.4112
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