Abstract

We construct the integrals of motion for the 5D deformed Kepler system with non-central potentials in su(2) Yang–Coulomb monopole field. We show that these integrals form a higher rank quadratic algebra Q(3;Lso(4),Tsu(2))⊕so(4), with structure constants involving the Casimir operators of so(4) and su(2) Lie algebras. We realize the quadratic algebra in terms of the deformed oscillator and construct its finite-dimensional unitary representations. This enable us to derive the energy spectrum of the system algebraically. Furthermore we show that the model is multiseparable and allows separation of variables in the hyperspherical and parabolic coordinates. We also show the separability of its 8D dual system (i.e. the 8D singular harmonic oscillator) in the Euler and cylindrical coordinates.

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