Abstract
This work deals with the physical system governed by a Hamiltonian operator, in two-dimensional space, of spinless charged particles subject to a perpendicular magnetic field B, coupled with a harmonic potential in the context of nonextensive statistical thermodynamics. The thermodynamics of such a quantum gas system is elaborated in the framework of Tsallis statistics by obtaining the q versions of the partition function, magnetization, and susceptibility after performing the Hilhorst integral transformation. The results are discussed in the q ↦ 1 limit.