Temperature dependence of the dynamic electrical properties of Cu1+xMn1-xO2 (x=0 and 0.06) crednerite materials
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Malaescu, I
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Lungu, A.
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Marin, C. N.
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West Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, RomaniaWest Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
Marin, C. N.
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Sfirloaga, P.
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Natl Inst Res & Dev Electrochem & Condensed Matte, P Andronescu St 1, Timisoara 300224, RomaniaWest Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
Sfirloaga, P.
[2
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Vlazan, P.
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Natl Inst Res & Dev Electrochem & Condensed Matte, P Andronescu St 1, Timisoara 300224, RomaniaWest Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
Vlazan, P.
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Brindusoiu, S.
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West Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, RomaniaWest Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
Brindusoiu, S.
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Poienar, M.
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Natl Inst Res & Dev Electrochem & Condensed Matte, P Andronescu St 1, Timisoara 300224, RomaniaWest Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
Poienar, M.
[2
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[1] West Univ Timisoara, Fac Phys, Bd V Parvan 4, Timisoara 300223, Romania
[2] Natl Inst Res & Dev Electrochem & Condensed Matte, P Andronescu St 1, Timisoara 300224, Romania
Polycrystalline samples of Cu1+xMn1-xO2 (x = 0 and 0.06) have been obtained by solid state reaction in silica tubes. Measurements of complex impedance (Z = Z' + iZ") at various temperatures T, between 30 degrees C and 120 degrees C and over the frequency range 100 Hz-2 MHz were performed. The frequency dependence of Z"(f) exhibits a maximum which moves towards higher frequencies by increasing the temperature, proving thus the hopping of the charge carriers between the localized states is the dominant mechanism for the electrical conduction in the investigated samples. The barrier energy values were: 0.287 eV for CuMnO2 and 0.208 eV for Cu1.06Mn0.94O2. The conductivity spectrum, o(f) follows the Jonscher universal law at each constant temperature. Based on the temperature and frequency dependencies of the electrical conductivity and using the variable-range-hopping (VRH) model, the frequency and temperature dependencies of the density of localized states near the Fermi level, N(E-F), the hopping distance, R and the hopping energy, W were computed. The results show that at constant frequency, N(E-F) does not depend on temperature for both samples. At constant temperature and frequencies up to 30 kHz, increasing the concentration of Cu ions leads to the decrease of R and W, whilst at high frequencies (over 100 kHz), R and W increase with the increase in the concentration of Cu ions.
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Inst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, RomaniaInst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, Romania
Poienar, M.
Sfirloaga, P.
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Inst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, RomaniaInst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, Romania
Sfirloaga, P.
Martin, C.
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UMR 6508 CNRS ENSICAEN UCBN, Lab CRISMAT, 6 Blvd Marechal Juin, F-14050 Caen 4, FranceInst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, Romania
Martin, C.
Ursu, D.
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Inst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, RomaniaInst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, Romania
Ursu, D.
Vlazan, P.
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Inst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, RomaniaInst Res & Dev Electrochem & Condensed Matter, P Andronescu St 1, Timisoara 300224, Romania