Electrophysical Properties of p-Type Undoped and Arsenic-Doped Hg1 – x Cd x Te Epitaxial Layers with x ≈ 0.4 Grown by the MOCVD Method
The temperature dependences of the charge-carrier concentration and lifetime of minority carriers in undoped and arsenic-doped p-type Hg1 – xCdxTe epitaxial layers with x ≈ 0.4 grown by the MOCVD-IMP (metalorganic chemical vapor deposition–interdiffusion multilayer process) method are studied. It is...
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Published in | Semiconductors (Woodbury, N.Y.) Vol. 52; no. 6; pp. 702 - 707 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
New York
Springer Nature B.V
01.01.2018
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Subjects | |
Online Access | Get full text |
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Summary: | The temperature dependences of the charge-carrier concentration and lifetime of minority carriers in undoped and arsenic-doped p-type Hg1 – xCdxTe epitaxial layers with x ≈ 0.4 grown by the MOCVD-IMP (metalorganic chemical vapor deposition–interdiffusion multilayer process) method are studied. It is shown that the temperature dependences of the charge-carrier concentration can be described by a model assuming the presence of one acceptor and one donor level. The ionization energies of acceptors in the undoped and arsenic-doped materials are 14 and 3.6 meV, respectively. It is established that the dominant recombination mechanism in the undoped layers is Shockley–Read–Hall recombination, and after low-temperature equilibrium annealing in mercury vapors (230°C, 24 h), the dominant mechanism is radiative recombination. The fundamental limitation of the lifetime in the arsenic-doped material is caused by the Auger-7 process. Activation annealing (360°C, 2 h) of the doped layers makes it possible to attain the 100% activation of arsenic. |
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ISSN: | 1063-7826 1090-6479 |
DOI: | 10.1134/S1063782618060052 |