“…These states were first introduced by Schrödinger [34] since 1926 for the harmonic oscillator. Then followed decades of intensive works in order to extend the CS concept to other types of exactly solvable systems [5,6,17,20,28]. It was shown in 1980's that a large class of these solvable potentials are characterized by a single property, i.e., a discrete reparametrization invariance, called shape-invariance [11,14,16,23], introduced in the framework of the supersymmetric quantum mechanics (SUSY QM) [10,21].…”