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Ion Transport across Grain Boundaries in Fast Lithium Ion Conducting Glass Ceramics

机译:快速锂离子传导玻璃陶瓷中跨晶界的离子传输

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Li_(1.5)Al_(0.5)Ge_(1.5)(PO_4)_3 (LAGP) 1. Grain and grain boundary resistance exhibit the same activation energy. → Purely geometrical current constriction; fraction of contacted area: about 25% Ohara Glass Ceramic (Li_(1+x)Al_xTi_(2-x)(PO_4)_3 doped with other oxides) 2. Grain boundary resistance exhibits a slightly higher activation energy than the grain resistance. 3. Nonlinear impedance spectra provide strong indication that the grain boundary resistance is not caused by a single (space charge) barrier, but by several serial barriers 4. Fit of nonlinear impedance data suggests that the thickness of the grain boundaries is in the range 5-10 nm. 5. HR-TEM images reveal type-A (amorphous) and type-B (high degree of crystallinity) grain boundaries. 6. Thickness of type-B grain boundaries is, in fact, in the range 5-10 nm. Mechanical stresses may lead to slightly higher activation energy.
机译:Li_(1.5)Al_(0.5)Ge_(1.5)(PO_4)_3(LAGP)1.晶粒和晶界电阻表现出相同的活化能。 →纯几何电流收缩;接触面积的分数:约25%大原玻璃陶瓷(掺杂有其他氧化物的Li_(1 + x)Al_xTi_(2-x)(PO_4)_3)2.晶界电阻的活化能略高于晶粒电阻。 3.非线性阻抗谱提供了强有力的指示,表明晶界电阻不是由单个(空间电荷)势垒引起的,而是由多个串联势垒引起的。4.非线性阻抗数据的拟合表明,晶界厚度在5范围内-10 nm。 5. HR-TEM图像显示了A型(非晶态)和B型(高结晶度)晶界。 6. B型晶界的厚度实际上在5-10 nm范围内。机械应力可能会导致更高的活化能。

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