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首页> 外文期刊>Solid state ionics >Further tests of the coupling model of ionic motions in glassy fast ionic conductors: conductivity relaxation and ~7Li and ~(11)B NMR in xLi_2S-(1-x)B_2S_3
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Further tests of the coupling model of ionic motions in glassy fast ionic conductors: conductivity relaxation and ~7Li and ~(11)B NMR in xLi_2S-(1-x)B_2S_3

机译:玻璃态快速离子导体中离子运动耦合模型的进一步测试:xLi_2S-(1-x)B_2S_3中的电导率弛豫和〜7Li和〜(11)B NMR

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The pronounced difference of the conductivity relaxation time and the nuclear spin lattice relaxation time of the diffusing ion in an ionic conductor has been established as a general property observed in various glassy ionic conductors. Not so well known is the near coincidence of the conductivity relaxation time and the nuclear spin lattice relaxation time of an immobile ion bound to the glassy matrix. These two effects combined have been explained by the Coupling model and the Coulomb lattice gas model. In this work, recent published experimental results obtained on lithium thioborate glasses which exhibit two separate lithium ion motions are discussed. There is the presence of long-range diffusion of Li ions among the BS3 units as well as a localized ionic hopping motion around a BS_4 unit. For the long-range diffusion motion of Li ions in the lithium thioborate glasses both effects mentioned above were observed experimentally by ~7Li and ~(11)B spin lattice relaxation, reaffirming that these effects are general and the details are again explainable by the Coupling model. On the other hand, for the hopping of a localized Li ion around a BS_4 unit which is a new feature occurring only in the lithium thioborate glasses, the absence of interaction and correlation with other Li ions has the immediate consequence that the Coupling model will expect exactly the same ~7Li and ~(11)B spin lattice relaxation rate from this localized motion. This prediction for a localized Li ion around a BS_4 unit, constituting a further test of the Coupling model, was indeed found experimentally and is pointed out for the first time in this work.
机译:已经建立了离子导体中扩散离子的电导率弛豫时间和核自旋晶格弛豫时间的明显差异,作为在各种玻璃态离子导体中观察到的一般特性。还不十分了解电导率弛豫时间与结合在玻璃状基质上的固定离子的核自旋晶格弛豫时间几乎一致。结合了这两种效应的耦合模型和库仑晶格气体模型已经对其进行了解释。在这项工作中,讨论了最近发表的在硫代硼酸锂玻璃上获得的实验结果,该玻璃表现出两个独立的锂离子运动。 Li离子在BS3单元之间存在远距离扩散以及BS_4单元周围的局部离子跳跃运动。对于锂离子在硫代硼酸锂玻璃中的远距离扩散运动,通过〜7Li和〜(11)B自旋晶格弛豫实验观察到了上述两种效应,重申了这些效应是普遍的,其细节可以再次通过耦合来解释模型。另一方面,对于仅在硫代硼酸锂玻璃中出现的新特征的局部锂离子在BS_4单元周围跳跃而言,与其他锂离子的相互作用和相关性的缺失会立即产生耦合模型所期望的结果。与该局部运动完全相同的〜7Li和〜(11)B自旋晶格弛豫速率。确实通过实验找到了对BS_4单元周围局部锂离子的预测,这构成了对耦合模型的进一步测试,并且在这项工作中首次指出了这一预测。

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