We consider a real scalar field and a Majorana fermion field to construct a supersymmetric quantum theory of free fermion fields based on the deformed Heisenberg algebra [𝑥, 𝑝] = 𝑖ℏ(1−𝛽𝑝+2𝛽2𝑝2), where 𝛽 is a deformation parameter.We present a deformed supersymmetric algebra in the presence of minimal length and maximal momentum.
