“…Although the non-relativistic Schrödinger equation with this potential has been solved for -states [41][42][43] and the single-particle motion in atomic nuclei has been explained quite well, the relativistic effects for a particle in this potential are more important, especially for a strongly coupled system. Solutions have been found and investigated for various cases including the 1D Schrödinger equation with the generalized WS potential using the NU method [44][45][46], the 1D KG equation with real and complex forms of the generalized WS potential [16], the one-dimensional Dirac equation with a WS potential [47], the ( )-wave Dirac equation ( = 0 i.e., κ = −1 for spin and κ = 1 for pseudospin symmetry) for a single particle with spin and pseudospin symmetry moving in a central WS potential [48], the three-dimensional Dirac equation for spherically symmetric potentials, specifically shape-invariant Morse, Rosen-Morse, Eckart, Pöschl-Teller, Scarf, WS and Hulthén potentials [49][50][51][52][53][54][55][56].…”