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In this work we introduce two different generalizations of the Fokker–Planck equation in (1+1) dimensions by replacing the spatial derivatives in terms of generalized Dunkl-type derivatives involving reflection operators. As applications of these results, we solve exactly the generalized Fokker–Planck equations for the harmonic oscillator and the centrifugal-type potentials. • We generalize the Fokker–Planck equation through Dunkl-type derivatives. • We solve exactly the Dunkl–Fokker–Planck equation for the centrifugal-type potential. • We solve exactly the Dunkl–Fokker–Planck equation for the harmonic oscillator. • We compute the energy spectrum and eigenfunctions of these potentials. [ABSTRACT FROM AUTHOR]

We decouple the Dirac's radial equations in D + 1 dimensions with Coulomb-type scalar and vector potentials through appropriate transformations. We study each of these uncoupled second-order equations in an algebraic way by using an su ( 1 , 1 ) algebra realization. Based on the theory of irreducible representations, we find the energy spectrum and the radial eigenfunctions. We construct the Perelomov coherent states for the Sturmian basis, which is the basis for the unitary irreducible representation of the su ( 1 , 1 ) Lie algebra. The physical radial coherent states for our problem are obtained by applying the inverse original transformations to the Sturmian coherent states. [ABSTRACT FROM AUTHOR]