Abstract
An Exactly-Solvable (ES) potential on the sphere is reviewed and the related Quasi-Exactly-Solvable (QES) potential is found and studied. Mapping the sphere to a simplex it is found that the metric (of constant curvature) is in polynomial form, and both the ES and the QES potentials are rational functions. Their hidden algebra is in a finite-dimensional representation realized by first order differential operators acting on . It is shown that variables in the Schrödinger eigenvalue equation can be separated in spherical coordinates and a number of the integrals of the second order exists assuring the complete integrability. The QES system is completely-integrable for and non-maximally superintegrable for . There is no separable coordinate system in which it is exactly solvable. We point out that by taking contractions of superintegrable systems, such as induced by Wigner-Inönü Lie algebra contractions, we can find other QES superintegrable systems, and we illustrate this by contracting our system to a QES non-maximal superintegrable system on Euclidean space , an extension of the Smorodinsky-Winternitz potential.
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