Ionization equilibrium in an excited semiconductor: Mott transition versus Bose-Einstein condensation

D. Semkat, F. Richter, D. Kremp, G. Manzke, W.-D. Kraeft, and K. Henneberger
Phys. Rev. B 80, 155201 – Published 2 October 2009

Abstract

The ionization equilibrium of an electron-hole plasma in a highly excited semiconductor is investigated. Special attention is directed to the influence of many-particle effects such as screening and lowering of the ionization energy causing, in particular, the Mott effect (density ionization). This effect limits the region of existence of excitons and, therefore, of a possible Bose-Einstein condensate at low temperatures. Results for the chemical potential and the degree of ionization are presented for zinc selenide (ZnSe). A possible window for the occurrence of a Bose-Einstein condensate of excitons is shown, taking into account the Mott effect.

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  • Received 15 June 2009

DOI:https://doi.org/10.1103/PhysRevB.80.155201

©2009 American Physical Society

Authors & Affiliations

D. Semkat, F. Richter, D. Kremp, G. Manzke, W.-D. Kraeft, and K. Henneberger

  • Institut für Physik, Universität Rostock, 18051 Rostock, Germany

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Issue

Vol. 80, Iss. 15 — 15 October 2009

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