Abstract
We obtain, in exact closed form, the wave-function normalization constants for the Schrödinger equation with potential V=B0tanhzU0cosh2z. These constants are derived in terms of a variety of formulations and solutions of the equation. We give discussions of both mathematical aspects and physical motivations of the problem. The main results are gathered in two appendixes. Wave-function normalization constants for the related Pöschl-Teller potential are given in a third appendix.