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Abstract In this paper, we extend the path integral formalism for the Klein–Gordon oscillator by replacing the standard derivative with the Dunkl derivative in 1 D , 2 D , and even in d − dimensions. Using space-time Cartesian coordinates, we derive the propagators and solve the problems exactly. We determine the energy eigenvalues and corresponding wave functions for the spinless particle. In limiting cases, where the Dunkl derivative parameters are set to zero, our results converge appropriately to those found in the literature for these problems.
Benzair et al. (Fri,) studied this question.