Quantum Many--Body Problems and Perturbation Theory
Abstract
We show that the existence of algebraic forms of exactly-solvable A-B-C-D and G2, F4 Olshanetsky-Perelomov Hamiltonians allow to develop the algebraic perturbation theory, where corrections are computed by pure algebraic means. A classification of perturbations leading to such a perturbation theory based on representation theory of Lie algebras is given. In particular, this scheme admits an explicit study of anharmonic many-body problems. Some examples are presented.
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