A set of exactly solvable one-dimensional quantum-mechanical potentials is described. It is defined by a finite-difference-difTerential equation generating in the limiting cases the Rosen-Morse, harmonic, and Poschl-Teller potentials. A general solution includes Shabafs infinite number soliton system and leads to raising and lowering operators satisfying a ^-deformed harmonic-oscillator algebra. In the latter case the energy spectrum is purely exponential and physical states form a reducible representation of the quantum conformal algebra su (1,1).Lie algebras are among the cornerstones of modern physics. They have an enormous number of applications in quantum mechanics and, in particular, put an order in the classification of exactly solvable potentials. "Quantized, " or g-deformed, Lie algebras (also loosely called quantum groups) are now well-established objects in mathematics [1]. Their applications were found in twodimensional integrable models and systems on lattices. However, despite much effort quantum algebras do not yet penetrate into physics on a large scale. In this paper we add to this field and show that a ^-deformed harmonic-oscillator algebra [2] may have straightforward meaning as the spectrum-generating algebra of the specific one-dimensional potential with exponential spectrum. This result shows that group-theoretical content of exactly solvable models is not bounded by the standard Lie theory.Recently Shabat analyzed an infinite chain of reflectionless potentials and constructed an infinite number soliton system [3]. The limiting potential decreased slowly at space infinities and obeyed peculiar self-similar behavior. We will present corresponding results in slightly different notations. We denote the space variable by x and introduce N superpotentials W n (x) satisfying the following set of second-order differential equations:(W^ + W^ + l + wZ-W n 2