Abstract
Within the framework of the effective mass method a formula for the computation of the probability of the following non-radiative transition in a semiconductor- or insulator crystal was deduced: two holes and one electron or two electrons and one hole are trapped on a crystal lattice defect, one electron recombines with one hole and the energy released thereby is taken up by the remaining quasiparticle which is thus set free and a free carier is formed. The deduced formula is applied to a Cu2O-crystal with a copper-ion vacancy as the crystal lattice defect.
Similar content being viewed by others
References
Seitz F.: Rev. Mod. Phys.26 (1954), 7.
Wentzel G.: Z. Phys.43 (1927), 524. Handbuch der Physik XXIV/1, 734. Phys. Z.29 (1928), 321.
Fuchs R.: Phys. Rev.111 (1958), 387.
Bess L.: Phys. Rev.105 (1957), 1469.
Elliott R. J.: Phys. Rev.108 (1957), 1384.
Khás Z.: Czech. J. Phys.B 15 (1965), 346.
Pekar S. I.: Issledovanija po elektronnoj teoriji kristallov, Moskva, Gostechizdat (1951).
Tolstoj N. A.: Optika i spektroskopija2 (1957), 210.
Gross E. F.: J. Phys. Chem. Solids8 (1959), 172.
Pastrňák: Czech. J. Phys.B 11 (1961), 374.
Nikitine S., Grun J. B., Sieskind M.: J. Phys. Chem. Solids17 (1961), 292.
Author information
Authors and Affiliations
Additional information
The author wishes to express his gratitute to Dr. M. Trlifaj for pointing out this interesting problem and for his valuable comments.
Rights and permissions
About this article
Cite this article
Khás, Z. Spontaneous ionization of bound exciton complexes. Czech J Phys 15, 568–580 (1965). https://doi.org/10.1007/BF01688067
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01688067