“…where λ 1 = −λ 2 = 1/2. The study of physical systems described by the Hamiltonian operator (2) have been a focus of attention for decades [11,15,16,17,18]. The generalizations of this Hamiltonian to particles interacting with electromagnetic fields, spin 1/2 particles, particles with position-dependent and anisotropic effective masses, and thin layers with small but finite thickness have been considered in [7,19,20,21,22,23].…”