Temperature dependent spectroscopic ellipsometry of Ag 2 Se and Ag 2 S with phase transitions from ionic to superionic conductivity state

Temperature dependent infrared (IR) and optical spectroscopic ellipsometry methods are used to investigate peculiarities of the transitions from the ionic conductivity to the superionic conductivity states in Ag 2 S and Ag 2 Se compounds. The structural phase transitions (SPTs), known as β→α transit...

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Veröffentlicht in:Physica status solidi. C 2015-06, Vol.12 (6), p.605-609
Hauptverfasser: Alekperov, O., Gasimov, N., Khalilova, Kh, Shim, Y., Paucar, R., Abdulzade, N., Samedov, O., Jahangirli, Z., Nakhmedov, E., Wakita, K., Mamedov, N.
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Sprache:eng
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Zusammenfassung:Temperature dependent infrared (IR) and optical spectroscopic ellipsometry methods are used to investigate peculiarities of the transitions from the ionic conductivity to the superionic conductivity states in Ag 2 S and Ag 2 Se compounds. The structural phase transitions (SPTs), known as β→α transition in these semiconductors, are investigated also with spectroscopic ellipsometry methods. The electronic band structure of Ag 2 S at the SPT changes sharply from the monoclinic to the bcc phase, which occurs at T = 453 K in the super ionic conductivity state, where all the interband transitions in optic region, corresponding to the monoclinic structure of β‐phase, disappear. The α‐phase of Ag 2 S is characterised with new lines in the dielectric functions ε 1 and ε 2 , which arise at 5‐6.5 eV. The interband transitions do not change in the SPT from the orthorhombic to the bcc in Ag 2 Se, which occurs at T > 406 K. In IR ellipsometry for the degenerated Ag 2 Se, the free carriers' plasma energy is displaced abruptly from ħω=0.075 eV at T=300 K to ħω=0.125 eV at T=338 K. The same effect is seen in the IR ellipsometry for Ag 2 S, where negative ε 1 appears at T=434‐440 K. These facts indicate a drastic increase of the free carriers concentrations in both of the semiconductors at temperatures before the β→α SPT. In Ag 2 S the second abrupt shift of the free carriers plasma energy from 0.035eV to 0.1 eV occurs at T=453 K, corresponding to β→ α SPT. The second shift is due to the electronic band structure change of Ag 2 S. (© 2015 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
ISSN:1862-6351
1610-1642
DOI:10.1002/pssc.201400367