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Fizika i Tekhnika Poluprovodnikov, 2018 Volume 52, Issue 6, Pages 554–559 (Mi phts5800)

This article is cited in 4 papers

Electronic properties of semiconductors

Electrophysical properties of $p$-type undoped and arsenic-doped Hg$_{1-x}$Cd$_{x}$Te epitaxial layers with $x\approx$ 0.4 grown by the MOCVD method

V. S. Evstigneevab, V. S. Varavinc, A. V. Chilyasova, V. G. Remesnikc, A. N. Moiseevab, B. S. Stepanovda

a Institute of Chemistry of High-Purity Substances RAS, Nizhnii Novgorod
b Lobachevsky State University of Nizhny Novgorod
c Institute of Semiconductor Physics, Siberian Branch of Russian Academy of Sciences, Novosibirsk
d Devyatykh Institute of Chemistry of High-Purity Substances, Russian Academy of Sciences

Abstract: The temperature dependences of the charge-carrier concentration and lifetime of minority carriers in undoped and arsenic-doped $p$-type Hg$_{1-x}$Cd$_{x}$Te epitaxial layers with x $\approx$ 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$^{\circ}$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$^{\circ}$C, 2 h) of the doped layers makes it possible to attain the 100% activation of arsenic.

Received: 26.07.2017
Accepted: 05.09.2017

DOI: 10.21883/FTP.2018.06.45914.8696


 English version:
Semiconductors, 2018, 52:6, 702–707

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