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首页> 外文期刊>International Journal of Quantum Chemistry >NONADIABATIC HOPPING CONDUCTION IN Sr1+xLa1-xFeO4 (0 less than or equal to x less than or equal to 0.20) BELOW 300 K
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NONADIABATIC HOPPING CONDUCTION IN Sr1+xLa1-xFeO4 (0 less than or equal to x less than or equal to 0.20) BELOW 300 K

机译:Sr1 + xLa1-xFeO4中的非绝热跃迁传导(0小于或等于x小于或等于0.20)300 K以下

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摘要

Authors measured bulk conductivities using complex-plane impedance analyses and frequency dependencies of dielectric properties in Sr1+xLa1-xFeO4 (0 less than or equal to x less than or equal to 0.20) with the four-probe dc conductivities. The temperature dependence of bulk conductivity in every specimen exhibits the nonadiabatic hopping conduction; i.e., sigma=A0 exp[-(WH+WO/2) /kBT]/T3/2, WH and WO being the hopping energy and the energy required to create a free hopping polaron. In every specimen, a dielectric relaxation process shows up with an activation energy nearly equal to that of the bulk conduction. The electron transfer integrals, J, estimated in the dielectric relaxations meet the nonadiabatic requirements. Speculation on the pre-exponential factor of the conductivity, A0, indicates that the holes in valence bands created by electron excitation predominantly contribute to electrical transport rather than the doped holes introduced by Sr-substitution for La. The experimental results are explained self-consistently by nonadiabatic hopping conduction. 38 refs.
机译:作者使用复平面阻抗分析和Sr1 + xLa1-xFeO4(0小于或等于x小于或等于0.20)和四探针直流电导率的介电特性频率相关性来测量整体电导率。每个样品中体电导率的温度依赖性都表现出非绝热跳跃传导。即sigma = A0 exp [-(WH + WO / 2)/ kBT] / T3 / 2,WH和WO是跳变能量和产生自由跳变极化子所需的能量。在每个样本中,都出现了介电弛豫过程,其激活能量几乎等于体导电的能量。介电弛豫中估计的电子转移积分J满足非绝热要求。对电导率的预指数因子A0的推测表明,由电子激发产生的价带中的空穴主要有助于电传输,而不是由Sr取代引入的La掺杂空穴。实验结果自洽地解释了通过非绝热跳跃传导。 38个参考

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