“…In recent years, a lot of effort has been put into solving these relativistic wave equations for various potentials by using different methods [4,5]. Some researchers have investigated the Dirac equation by using a variety of potentials and different methods, such as the spin symmetry in the antinucleon spectrum and tensor type Coulomb potential with spin-orbit number k in a state of spin symmetry and p-spin symmetry [6],bound states of the Dirac equation with positiondependent mass for the Eckart potential [7], the exact solution of Klein-Gordon with the Poschl-Teller double-ring-shaped Coulomb potential [8],the exact solution of the Dirac equation for the Coulomb potential plus NAD potential by using the Nikorov-Uvarov method [9], the potential Deng-Fan and the Coulomb potential tensor using the asymptotic iteration method (AIM) [10],the potential Poschl-Teller plus the Manning Rosen radial section with the hypergeometry method [11], the solution ofKlein-Gordon equation for Hulthen non-central potential inradial part with Romanovski polynomial [12],and the solution [13], the Scarf potential with the new tensor coupling potential for spin and pseudospin symmetries using Romanovski polynomials [14],for the q-deformed hyperbolic Poschl-Teller potential and the trigonometric Scarf II noncentral potential by using AIM [15],eigensolutions of the deformed Woods-Saxon potential via AIM [16],approximate solutions of the Klein Gordon equation with an improved Manning Rosen potential in D-dimensions using SUSYQM [17], and eigen spectra of the Dirac equation for a deformed Woods-Saxon potential via the similarity transformation [18].…”