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Extended D.C. electrical transport measurements on the mixed conductor Cu_3CS_2

机译:混合导体Cu_3CS_2上扩展的直流电传输测量

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D.C. electrical transport measurements have been done over the temperautre range 200 K to 450 K on the mixed conductor Cu_(3.0)CS_2. This work extends the original work done on Cu_xCS_2 over the temperature range 260 K to 350 K. Above 220 K, the voltage versus time curves follow the Yokota model for mixed conductors. Below 220K, the voltage versus time curves were practically constant, suggesting very little ionic transport below this temperature, and an electronic conductivity of the order of 10~(-5) ( OMEGA cm)~(-1) at 200 K. At ambient temperatures, the ionic conductivity and electronic conductivity were both of the order of 10~(-3) ( OMEGA cm)~(-1), and the chemical diffusion coefficient found to be of the order of 10~(-6) cm~2s~(-1), in agreement with earlier work on Cu_3CS_2. Above 220 K, the ionic conductivity versus temperature plots were of the Arrhenius form with an activation energy of about 0.36 eV. The jump time and residence time were estimated to be of the order of 10~(-12)s and 10~(-6)s respectively, confirming hopping as the mode of ionic transport. The electronic conductivity versus temperature plot confirmed thermal activation as the mode of electronic transport. The results suggest Cu_xCS_2 to be very stable and the Yokota mode, with very little modification, to be very reliable for the analysis of these mixed conductors.
机译:在混合导体Cu_(3.0)CS_2上,在200 K至450 K的温度范围内进行了直流电传输测量。这项工作扩展了在260 K至350 K的温度范围内在Cu_xCS_2上完成的原始工作。在220 K以上,电压与时间的关系曲线遵循Yokota模型的混合导体。在220K以下,电压与时间的关系曲线实际上是恒定的,表明在该温度以下离子迁移非常小,在200 K下的电导率约为10〜(-5)(OMEGA cm)〜(-1)。温度,离子电导率和电子电导率均为10〜(-3)(OMEGA cm)〜(-1),化学扩散系数约为10〜(-6)cm〜。 2s〜(-1),与早期关于Cu_3CS_2的工作一致。高于220 K时,离子电导率与温度的关系曲线为阿伦尼乌斯形式,活化能约为0.36 eV。跳跃时间和停留时间估计分别为10〜(-12)s和10〜(-6)s的数量级,证实跳跃是离子迁移的方式。电子传导率与温度的关系图证实了热激活是电子传输的方式。结果表明,Cu_xCS_2非常稳定,而经过很少修改的横田模式对于分析这些混合导体非常可靠。

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