1989
DOI: 10.1016/0379-6787(89)90032-x
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Intrinsic defect states in CuInSe2 single crystals

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Cited by 41 publications
(5 citation statements)
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“…An important characteristic of Cu chalcogenides is their high defect concentration, which plays a key role in determining most of their properties, including charge and heat transport, optoelectronic, optic, and plasmonic properties. Cu chalcogenide compounds tolerate a large range and density of nonstoichiometry and antisite defects, which may result in spatial compositional inhomogeneities and ordered defect compounds. Several reports have focused on a calculation of defects in Cu chalcogenides, including CuInSe 2 , ,, Cu 2 SnS 3 , CuGaS 2 , CuSbSe 2, and CZTS. ,,, While both anion and cation deficiencies are tolerated, inducing n- or p-type conductivities, Cu chalcogenides with p-type conductivity are the most common, where their p-type conductivity is associated with Cu vacancies. As an example, it takes much less energy to form a Cu vacancy in CuInSe 2 than to form cation vacancies in the II-VI compounds, and the low formation energy of the shallow defect Cu vacancies provides CuInSe 2 with p-type self-doping.…”
Section: Functional Propertiesmentioning
confidence: 99%
“…An important characteristic of Cu chalcogenides is their high defect concentration, which plays a key role in determining most of their properties, including charge and heat transport, optoelectronic, optic, and plasmonic properties. Cu chalcogenide compounds tolerate a large range and density of nonstoichiometry and antisite defects, which may result in spatial compositional inhomogeneities and ordered defect compounds. Several reports have focused on a calculation of defects in Cu chalcogenides, including CuInSe 2 , ,, Cu 2 SnS 3 , CuGaS 2 , CuSbSe 2, and CZTS. ,,, While both anion and cation deficiencies are tolerated, inducing n- or p-type conductivities, Cu chalcogenides with p-type conductivity are the most common, where their p-type conductivity is associated with Cu vacancies. As an example, it takes much less energy to form a Cu vacancy in CuInSe 2 than to form cation vacancies in the II-VI compounds, and the low formation energy of the shallow defect Cu vacancies provides CuInSe 2 with p-type self-doping.…”
Section: Functional Propertiesmentioning
confidence: 99%
“…In the low temperature domain, the activation energy could be attributed to activation of carriers from an energy level introduced in the band gap by some defects/or impurities. Such ionisation energy (80 meV) has already been measured in these ternary compounds [17,18].…”
Section: Discussionmentioning
confidence: 76%
“…It is rather likely that this defect is identical with the shallow acceptor with an ionisation energy of about 50 meV observed in CuInSe, crystals intentionally doped with oxygen (MATSUSHITA et al). Probably, a specific additional structure detected in the near-edge photoluminescence spectra of CuInSe, single crystals after annealing in air (ABOU-ELFOTOUH et al 1989) or implantation of oxygen (ABOU-ELFOTOUH et al 1990) and of air-annealed CuInSe, thin films (KUSHIYA et al) is caused by the same defect.…”
Section: Discussionmentioning
confidence: 99%