Quantum equivalent of the Bertrand's theorem
arXiv:quant-ph/9905011 · doi:10.1142/S0217732300002255
Abstract
A procedure for constructing bound state potentials is given. We show that, under the natural conditions imposed on a radial eigenvalue problem, the only special cases of the general central potential, which are exactly solvable and have infinite number of energy eigenvalues, are the Coulomb and harmonic oscillator potentials.
11 pages, REVTeX