Quantum mechanical potentials exactly solvable in terms of higher hypergeometric functions. I: The third-order case

TL;DR

This paper introduces a new family of exactly solvable quantum potentials expressed through higher hypergeometric functions, expanding the class of potentials with explicitly known solutions and analyzing their spectral properties.

Contribution

It presents a six-parameter family of potentials derived from third-order hypergeometric equations, generalizing known potentials and discussing reduction techniques for higher-order eigenvalue problems.

Findings

Explicit solutions for scattering and bound states are computed.

The phase diagram illustrates the discrete spectrum properties.

Reduction of higher-order equations to Schrödinger form is systematically discussed.

Abstract

We present a new six-parameter family of potentials whose solutions are expressed in terms of the hypergeometric functions 3F2, 2F2 and 1F2. Both the scattering data and the bound states of these potentials are explicitly computed and the peculiar properties of the discrete spectrum are depicted in a suitable phase diagram. Our starting point is a third-order formal eigenvalue equation of the hypergeometric type (with a suitable solution known) which is transformed to the Schr\"odinger equation by applying the reduction of order technique as the crucial first step. The general preconditions allowing for the reduction to Schr\"odinger form of an arbitrary eigenvalue equation of higher order, are discussed at the end of the article, and two universal features of the potentials arising this way are also stated and discussed. In this general scheme the Natanzon potentials are the simplest special case, those presented here the next ones, and so on for potentials arising from equations of fourth or higher order.