Abstract

Formation of the excitonic condensed phase in quantum wells with defects of macroscopic size is investigated in the case of a specific kind of defect arising in local areas of planar quantum wells where the wells are thicker or thinner by an atomic monolayer or two. The excitonic system in the wells is non-equilibrium as the excitons are constantly created by an irradiation and decay due to the finite lifetime. The condensation considered in the paper is not the Bose–Einstein condensation but rather the classical condensation due an interaction between excitons with additional peculiarities caused by non-equilibrium conditions. The main contribution to the exciton’s energy in the defect’s area comes from the energy of the exciton’s confinement along the growth axis and the respective quantization of the exciton’s levels. The condensation manifests itself by an enhancement the exciton accumulation in the defect’s area with increasing pumping and by an appearance of different types of structures in the exciton density distribution when the defect’s size is large. The condensed phase may appear in the form of islands or in the form of rings on the defect’s boundary. It is shown, that the value of the exciton’s lifetime plays an important role in the spatial distribution of the exciton density. The similarity and the difference of density structures for wells with the extra or lacking atomic monolayer in the defect’s area are investigated. The specific features of the manifestation of the exciton luminescence at the condensation in the defect’s region is analyzed.

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