  The intrinsic orbital magnetization of a TMD monolayer is usually calculated
for a plane unbounded system without mentioning the geometrical shape of
samples and boundary conditions (BCs) for electron wave functions. The method
of calculations includes allowing for the Berry curvature contribution also in
the case when the system is described by the two-band minimal model [9]. In the
present paper, we show that the geometrical and topological properties of the
specimen, as well as the BCs, play an important role in the problem of
magnetization even for a macroscopic specimen.
