Abstract
For an integrable Hamiltonian system we construct a representation of the phase space symmetry algebra over the space of functions on a Lagrangian manifold. The representation is a result of the canonical quantization of the integrable system using separating variables. The variables are chosen in such way that half of them parameterizes the Lagrangian manifold, which coincides with the Liouville torus of the integrable system. The obtained representation is indecomposable and non-exponentiated.
Information
Published: 1 January 2013
First available in Project Euclid: 13 July 2015
zbMATH: 1351.37218
MathSciNet: MR3183930
Digital Object Identifier: 10.7546/giq-14-2013-61-73
Rights: Copyright © 2013 Institute of Biophysics and Biomedical Engineering, Bulgarian Academy of Sciences