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Ion and Polaron Conducting Glasses

机译:离子和极化子导电玻璃

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摘要

Conductivity spectra, σ(ω), covering wide frequency ranges up to the mid infrared, have been taken of various glasses at different temperatures. The systems studied include the ion-conducting glasses 0.30 Na_2O · 0.70 B_2O_3, 0.30 Li_2O · 0.70 B_2O_3 and B_2O_3 · 0.56 Li_2O · 0.45 LiBr as well as the polaron conducting glass 0.2 P_2O_5 · 0.8 (0.89 V_2O_5 · 0.11 V_2O_4). In the case of the ion-conducting glasses it is possible to separate vibrational and hopping spectra from each other. The resulting hopping spectra display high-frequency plateaus; in the dispersive regime, two power-law exponents are observed, one being smaller, the other larger than unity. In contrast, the dispersive conductivity of the polaron conducting glass shows a simple single-power-law behavior with an exponent smaller than one. The interpretation of the spectra includes the idea of different "target" sites for the mobile species. A model concept for ion and polaron transport in glasses is proposed.
机译:已经在不同温度下拍摄了各种玻璃的电导率谱σ(ω),涵盖了高达中红外的宽频率范围。研究的系统包括离子导电玻璃0.30 Na_2O·0.70 B_2O_3、0.30 Li_2O·0.70 B_2O_3和B_2O_3·0.56 Li_2O·0.45 LiBr以及极化子导电玻璃0.2 P_2O_5·0.8(0.89 V_2O_5·0.11 V_2O_4)。在离子传导玻璃的情况下,可以将振动光谱和跳跃光谱彼此分开。产生的跳跃频谱显示出高频平稳状态;在色散状态下,观察到两个幂律指数,一个较小,另一个大于一。相反,极化子导电玻璃的分散导电性表现出简单的单幂律特性,其指数小于一个。光谱的解释包括对流动物种使用不同“目标”位点的想法。提出了玻璃中离子和极化子传输的模型概念。

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