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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 Li-7 and B-11 NMR in xLi(2)S-(1-x)B2S3
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Further tests of the coupling model of ionic motions in glassy fast ionic conductors: conductivity relaxation and Li-7 and B-11 NMR in xLi(2)S-(1-x)B2S3

机译:玻态快速离子导体中离子运动耦合模型的进一步测试:xLi(2)S-(1-x)B2S3中的电导率弛豫以及Li-7和B-11 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 BS4 unit. For the long-range diffusion motion of Li ions in the lithium thioborate glasses both effects mentioned above were observed experimentally by Li-7 and B-11 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 BS4 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 Li-7 and B-11 spin lattice relaxation rate from this localized motion. This prediction for a localized Li ion around a BS4 unit, constituting a further test of the Coupling model, was indeed found experimentally and is pointed out for the first time in this work. [References: 24]
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。还不太了解的是,电导率弛豫时间与结合到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,讨论了在硫代硼酸锂玻璃上获得的展示两个独立锂离子运动的最新公开实验结果。 Li离子在BS3单元之间存在远距离扩散以及BS4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Li-7和B-11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,并且其细节可以通过耦合模型再次解释。另一方面,对于仅在硫代硼酸锂玻璃中出现的新功能的局部Li离子在BS4单元周围跳变,与其他Li离子的相互作用和相关性的缺失将立即产生耦合模型所期望的结果。从这种局部运动中,Li-7和B-11的自旋晶格弛豫率完全相同。确实通过实验找到了对BS4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,并在本研究中首次指出。 [参考:24]

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