Abstract
The quantum integrable system is a 3D system with rational potential related to the non-crystallographic root system . It is shown that the gauge-rotated Hamiltonian as well as one of the integrals, when written in terms of the invariants of the Coxeter group , is in algebraic form: it has polynomial coefficients in front of derivatives. The Hamiltonian has infinitely-many finite-dimensional invariant subspaces in polynomials, they form the infinite flag with the characteristic vector $\vec \al\ =\ (1,2,3)$. One among possible integrals is found (of the second order) as well as its algebraic form. A hidden algebra of the Hamiltonian is determined. It is an infinite-dimensional, finitely-generated algebra of differential operators possessing finite-dimensional representations characterized by a generalized Gauss decomposition property. A quasi-exactly-solvable integrable generalization of the model is obtained. A discrete integrable model on the uniform lattice in a space of -invariants "polynomially"-isospectral to the quantum model is defined.
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