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Radiation fields, scattering and inverse scattering on asymptotically hyperbolic manifolds, preprint
"... The purpose of this article is to define the radiation fields on asymptotically hyperbolic manifolds and to use them to study scattering theory. The radiation fields on R n and on asymptotically Euclidean manifolds were introduced by F.G. Friedlander in a series of papers starting in the early 1960’ ..."
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The purpose of this article is to define the radiation fields on asymptotically hyperbolic manifolds and to use them to study scattering theory. The radiation fields on R n and on asymptotically Euclidean manifolds were introduced by F.G. Friedlander in a series of papers starting in the early 1960’s [10, 11, 12, 13, 14]. His program of using the radiation fields to obtain the scattering matrix in that general setting was
A Note On Some Positivity Conditions Related To Zeta And L-Functions
- IMRN
, 1998
"... Introduction The theory of Hilbert spaces of entire functions [1] was developed by Louis de Branges in the late 1950s and early 1960s with the help of his students including James Rovnyak and David Trutt. It is a generalization of the part of Fourier analysis involving Fourier transform and Plancher ..."
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Introduction The theory of Hilbert spaces of entire functions [1] was developed by Louis de Branges in the late 1950s and early 1960s with the help of his students including James Rovnyak and David Trutt. It is a generalization of the part of Fourier analysis involving Fourier transform and Plancherel formula. The de Branges-Rovnyak theory of square summable power series, whichplayed an important role in leading to de Branges' discovery of a proof of the Bieberbach conjecture, originated from the theory of Hilbert spaces of entire functions. In [2] de Branges proposed an approach to the generalized Riemann hypothesis, that is, the hypothesis that not only the Riemann zeta function i(s) but also all the Dirichlet L-functions L(s# ) with primitive have their nontrivial zeros lying on the critical line !s = 1=2 (See Davenport [5]). In [2] de Br

