Impurity–defect emission from undoped Cd1–xZnxTe single crystals near the fundamental absorption edge
- Authors: Krivobok V.S.1,2, Denisov I.A.3, Mozhevitina E.N.3, Nikolaev S.N.1, Onishchenko E.E.1, Pruchkina A.A.1, Silina A.A.3, Smirnova N.A.3, Chernopitsskii M.A.1, Shmatov N.I.3
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Affiliations:
- Lebedev Physical Institute
- National Research Nuclear University “MEPhI,”
- Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
- Issue: Vol 58, No 5 (2016)
- Pages: 981-991
- Section: Impurity Centers
- URL: https://journal-vniispk.ru/1063-7834/article/view/197515
- DOI: https://doi.org/10.1134/S1063783416050127
- ID: 197515
Cite item
Abstract
Shallow impurity–defect states in undoped Cd1–xZnxTe (x ∼ 3–6%) single crystals have been studied using low-temperature photoluminescence measurements. It has been found that the effect exerted by zinc is mainly reduced to a rigid shift of all the specific features associated with the exciton radiation, which made it possible, with a high (∼0.3 meV) accuracy, to measure the band gap and the zinc concentration in solid solutions. Hydrogen-like donors with the ground-state energy of ∼14 meV and four types of acceptors with average activation energies of 59.3 ± 0.6 meV, 69.6 ± 1.5 meV, 155.8 ± 2.0 meV, and 52.3 ± 0.6 meV have been identified in all the crystals studied. Based on a comparison with the results of the analysis of the impurity background and the data available in the literature on impurity–defect emission in undoped CdTe, the first three acceptors can be assigned to the substitutional impurities NaCd, PTe, and CuCd, respectively. The most shallow acceptor (52.3 ± 0.6 meV) is a complex defect in which there is a nonstandard excited level separated by only 7 meV from the ground level. This level is formed apparently due to the removal of degeneracy, which is characteristic of TD acceptors, by the low-symmetry potential of the complex defect.
About the authors
V. S. Krivobok
Lebedev Physical Institute; National Research Nuclear University “MEPhI,”
Author for correspondence.
Email: krivobok@lebedev.ru
Russian Federation, Leninskii pr. 53, Moscow, 119991; Kashirskoe sh. 31, Moscow, 115409
I. A. Denisov
Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
Email: krivobok@lebedev.ru
Russian Federation, Bolshoi Tolmachevskii per. 5-1, Moscow, 119017
E. N. Mozhevitina
Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
Email: krivobok@lebedev.ru
Russian Federation, Bolshoi Tolmachevskii per. 5-1, Moscow, 119017
S. N. Nikolaev
Lebedev Physical Institute
Email: krivobok@lebedev.ru
Russian Federation, Leninskii pr. 53, Moscow, 119991
E. E. Onishchenko
Lebedev Physical Institute
Email: krivobok@lebedev.ru
Russian Federation, Leninskii pr. 53, Moscow, 119991
A. A. Pruchkina
Lebedev Physical Institute
Email: krivobok@lebedev.ru
Russian Federation, Leninskii pr. 53, Moscow, 119991
A. A. Silina
Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
Email: krivobok@lebedev.ru
Russian Federation, Bolshoi Tolmachevskii per. 5-1, Moscow, 119017
N. A. Smirnova
Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
Email: krivobok@lebedev.ru
Russian Federation, Bolshoi Tolmachevskii per. 5-1, Moscow, 119017
M. A. Chernopitsskii
Lebedev Physical Institute
Email: krivobok@lebedev.ru
Russian Federation, Leninskii pr. 53, Moscow, 119991
N. I. Shmatov
Federal State Research and Design Institute of Rare Metal Industry “Giredmet,”
Email: krivobok@lebedev.ru
Russian Federation, Bolshoi Tolmachevskii per. 5-1, Moscow, 119017
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