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Separating bulk from grain boundary Li ion conductivity in the sol–gel prepared solid electrolyte Li1.5Al0.5Ti1.5(PO4)3

机译:在溶胶-凝胶法制备的固体电解质Li1.5Al0.5Ti1.5(PO4)3中从晶界锂离子电导率中分离体积

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摘要

Lithium aluminium titanium phosphate (LATP) belongs to one of the most promising solid electrolytes. Besides sufficiently high electrochemical stability, its use in lithium-based all-solid-state batteries crucially depends on the ionic transport properties. While many impedance studies can be found in literature that report on overall ion conductivities, a discrimination of bulk and grain boundary electrical responses via conductivity spectroscopy has rarely been reported so far. Here, we took advantage of impedance measurements that were carried out at low temperatures to separate bulk contributions from the grain boundary responses. It turned out that bulk ion conductivity is by at least three orders of magnitude higher than ion transport across the grain boundary regions. At temperatures well below ambient long-range Li ion dynamics is governed by activation energies ranging from 0.26 to 0.29 eV depending on the sintering conditions. As an example, at temperatures as low as 173 K, the bulk ion conductivity, measured in N2 inert gas atmosphere, is in the order of 8.1 × 10−6 S cm−1. Extrapolating this value to room temperature yields ca. 3.4 × 10−3 S cm−1 at 293 K. Interestingly, exposing the dense pellets to air atmosphere over a long period of time causes a significant decrease of bulk ion transport. This process can be reversed if the phosphate is calcined at elevated temperatures again.
机译:磷酸锂铝钛(LATP)属于最有前途的固体电解质之一。除了足够高的电化学稳定性外,其在锂基全固态电池中的使用还关键取决于离子传输性能。尽管在报告整体离子电导率的文献中可以找到许多阻抗研究,但迄今为止,很少有报道通过电导率光谱法来区分体和晶界电响应。在这里,我们利用了在低温下进行的阻抗测量,将晶界​​响应的整体贡献区分开来。结果表明,体离子电导率比跨晶界区域的离子传输高至少三个数量级。在远低于环境温度的情况下,取决于烧结条件,锂离子的动态动力学受活化能的控制,该活化能的范围为0.26至0.29 eV。例如,在低至173 K的温度下,在N2惰性气体气氛中测得的整体离子电导率约为8.1×10-6 S cm-1。将该值外推至室温可得出约。在293 K时为3.4×10-3 S cm-1。有趣的是,将致密的颗粒长时间暴露在空气中会导致大量离子传输的显着减少。如果将磷酸盐再次在高温下煅烧,则该过程可以逆转。

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