On Two Superintegrable Nonlinear Oscillators in N Dimensions RID B-5702-2011

We consider the classical superintegrable Hamiltonian system given by H(lambda) = T + U = p(2)/2(1 + lambda q(2)) + omega(2)q(2)/2(1 + lambda q(2)), where U is known to be the "intrinsic" oscillator potential on the Darboux spaces of nonconstant curvature determined by the kinetic energy term T and parametrized by lambda. We show that H(lambda) is Stackel equivalent to the free Euclidean motion, a fact that directly provides a curved Fradkin tensor of constants of motion for H(lambda). Furthermore, we analyze in terms of. the three different underlying manifolds whose geodesic motion is provided by T. As a consequence, we find that H(lambda) comprises three different nonlinear physical models that, by constructing their radial effective potentials, are shown to be two different nonlinear oscillators and an infinite barrier potential. The quantization of these two oscillators and its connection with spherical confinement models is briefly discussed.