2016
DOI: 10.1134/s1087659616030081
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Origin of the electrical activity of iron atoms in vitreous arsenic selenide

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Cited by 3 publications
(4 citation statements)
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“…Figure 7 presents the dependence of the shift of the Fermi level from the middle of the band gap δE = (E opt )/2 -E σ on the iron concentration. As can be seen from the figure, when the iron concentration increases, the Fermi level smoothly approaches its limiting position, which is distant from the middle of the band gap by a value of 0.57 ± 0.03 eV (Marchenko, Rabchanova, Seregin et al 2016). .…”
Section: Electrical Activity Of Iron Atomsmentioning
confidence: 82%
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“…Figure 7 presents the dependence of the shift of the Fermi level from the middle of the band gap δE = (E opt )/2 -E σ on the iron concentration. As can be seen from the figure, when the iron concentration increases, the Fermi level smoothly approaches its limiting position, which is distant from the middle of the band gap by a value of 0.57 ± 0.03 eV (Marchenko, Rabchanova, Seregin et al 2016). .…”
Section: Electrical Activity Of Iron Atomsmentioning
confidence: 82%
“…For undoped glass E opt ≈ 2E σ and the current transfer, according to the sign of Seebeck coefficient, is realised by holes. The introduction of iron into glass leads to a change in the sign of the current carriers (the current transfer, according to the sign of the Seebeck coefficient, is realised by electrons) and to a decrease in the electro conductance activation energy (Marchenko, Rabchanova, Seregin et al 2016). Figure 7 presents the dependence of the shift of the Fermi level from the middle of the band gap δE = (E opt )/2 -E σ on the iron concentration.…”
Section: Electrical Activity Of Iron Atomsmentioning
confidence: 99%
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