Abstract

The linear symmetric systems associated with the modified Cherednik operators and applications

Highlights

  • Let a be a real Euclidean vector space of dimension d and let R be a root system in a

  • The original motivation for the study of these operators came from the theory of invariant differential operators: if the triplet (a, R, k) arises from the structure theory of a Riemannian symmetric space of the non-compact type G/K, it is possible to explicitly construct all radial components of the W −invariant differential operators on G/K using the Cherednik operators

  • The joint spectral theory of Cherednik operators is naturally related to the harmonic analysis on Reimannian symmetric spaces

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Summary

Introduction

Let a be a real Euclidean vector space of dimension d and let R be a root system in a. D, are the modified Cherednik operators, I be an interval of R, (Ap )0≤p≤d a family of functions from I × Rd into the space of m×m matrices with real coefficients ap,i,j (t, x) which are W -invariant with respect to x, symmetric (i.e. ap,i,j (t, x) = ap,j,i (t, x)) and whose all derivatives in x ∈ Rd are bounded and continuous functions of (t, x), the initial data belongs to generalized Sobolev spaces [Hks (Rd )]m and f is a continuous function on an interval I with value in [Hks (Rd )]m. Throughout this paper by C we always represent a positive constant not necessarily the same in each occurrence

Preliminaries
The eigenfunctions of the modified Cherednik operators
The generalized Fourier transform
Generalized convolution operator
The generalized Sobolev spaces
Cherednik linear symmetric systems
The Cherednik-wave equations with variable coefficients
Finite speed of propagation
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