We investigate the one-dimensional nonrelativistic Schrödinger equation within the Jacobi–Dunkl framework. Although the Jacobi–Dunkl operator is well established in harmonic analysis and special-function theory, its systematic use in quantum-mechanical spectral and scattering problems remains comparatively limited. In this work, we develop an explicit parity-resolved formulation in which the reflection-induced deformation is incorporated directly at the operator level. The Jacobi–Dunkl momentum operator, Hamiltonian, weighted scalar product, and parity decomposition are constructed consistently in the associated weighted Hilbert space. For reflection-invariant potentials, the stationary Schrödinger equation is naturally separated into even and odd sectors. The odd sector acquires an additional effective hyperbolic contribution generated by the reflection part of the operator, whereas the even sector is governed by a different reduced equation. The formalism is first applied to the one-dimensional infinite quantum well, for which exact eigenfunctions and parity-dependent quantization conditions are obtained in terms of Jacobi-type hypergeometric functions. We then treat the hyperbolic Pöschl–Teller potential. In the bound-state sector, finite parity-dependent discrete spectra and normalized eigenfunctions expressed through Jacobi polynomials are derived. The corresponding scattering sector is also analyzed by reconstructing the full-line reflection and transmission amplitudes from the even- and odd parity channels. The results show that the Jacobi–Dunkl parameters restructure the spectrum, split the parity branches, modify the bound-state localization, and affect the scattering behavior. The ordinary Schrödinger results are recovered as a formal limiting benchmark, confirming the consistency of the construction.
In this paper, we investigate the Dunkl-Schrödinger equation in the presence of energy-dependent potentials. A consistent formulation is developed by deriving modified expressions for the probability density, normalization condition, and scalar product, thereby ensuring the conservation of probability. Exact analytical...
R. Boudjouraf, B. Hamil, A. Benchikha et al.· Modern Physics Letters A· 0 citations
This work investigates a class of exactly solvable quantum systems described by a generalized Dunkl--Schr\"odinger equation with energy-dependent interactions. A two-parameter extension of the Dunkl differential operator is introduced, incorporating both the conventional reflection contribution and an additional deriva...
B. Hamil, R. Boudjouraf, A. Benchikha et al.· 0 citations
We introduce a microlocal formulation of the Schr{\"o}dinger-Klein-Gordon system describing the interaction between a non-relativistic quantum particle and a Klein-Gordon field through Yukawa coupling. Instead of working directly with the Schr{\"o}dinger wave function, we represent the quantum component by its Fourier-...
The inverse spectral theory for a self-adjoint one-dimensional Dirac operator associated periodic potentials is formulated via a Riemann–Hilbert problem (RHP) approach. The resulting formalism is also used to solve the initial value problem for the non-linear Schrödinger (NLS) equation. A uniqueness theorem for the s...
G. Biondini, Ze-Chuan Zhang· Journal of Nonlinear Waves· 0 citations