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DC and AC conductivities of (As 2S 3) 100− x (AsSe 0.5Te 0.5I) x chalcogenide glasses
The DC and AC conductivities of samples from the system (As 2S 3) 100− x (AsSe 0.5Te 0.5I) x , where x=0, 5, 10, 15, 20, 25, 30, 35, 50, 70 and 90 mol%, were measured as a function of temperature. Besides, the AC conductivities of the samples with x=10 and 30 were measured as a function of frequency...
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Published in: | Physica. B, Condensed matter Condensed matter, 2008-08, Vol.403 (17), p.2578-2583 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The DC and AC conductivities of samples from the system (As
2S
3)
100−
x
(AsSe
0.5Te
0.5I)
x
, where
x=0, 5, 10, 15, 20, 25, 30, 35, 50, 70 and 90
mol%, were measured as a function of temperature. Besides, the AC conductivities of the samples with
x=10 and 30 were measured as a function of frequency from room temperature to the glass transition temperature. The DC conductivity dependence on temperature is of the Arrhenius type, whereas the value of the pre-exponential factor suggests the electrical conduction by localized states in the band tails and by localized states near the Fermi level. The small values of the conduction activation energy (10
−2–10
−1
eV) obtained at higher frequencies suggest that the conduction in these materials is due to hopping of charge carriers between close defect states near the Fermi level. |
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ISSN: | 0921-4526 1873-2135 |
DOI: | 10.1016/j.physb.2008.01.038 |