首页> 外文期刊>International Journal of Quantum Chemistry >Li-6 and Li-7 MAS NMR studies on fast ionic conducting spinel-type Li2MgCl4, Li2-xCuxMgCl4, Li2-xNaxMgCl4, and Li2ZnCl4
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Li-6 and Li-7 MAS NMR studies on fast ionic conducting spinel-type Li2MgCl4, Li2-xCuxMgCl4, Li2-xNaxMgCl4, and Li2ZnCl4

机译:快速离子导电尖晶石型Li2MgCl4,Li2-xCuxMgCl4,Li2-xNaxMgCl4和Li2ZnCl4的Li-6和Li-7 MAS NMR研究

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Li-6 and Li-7 MAS NMR spectra including 1D-EXSY (exchange spectroscopy) and inversion recovery experiments of fast ionic conducting Li2MgCl4, Li2-xCuxMgCl4, Li2-xNaxMgCl4, and Li2ZnCl4 have been recorded and discussed with respect to the dynamics and local structure of the lithium ions. The chemical shifts, intensities, and half-widths of the Li MAS NMR signals of the inverse spinel-type solid solutions (Li2-xXxMgCl4)-Mg-1 (M-1 = Cu, Na) with the copper ions solely at tetrahedral sites and sodium ions at octahedral sites and the normal spinel-type zinc compound, respectively, confirm the assignment of the low-field signal to Li-tet of inverse spinel-type Li2MgCl4 and the high-field signal to Li-oct as proposed by Nagel et al. (2000). In contrast to spinel-type Li2-2xMg1+xCl4 solid solutions with clustering of the vacancies and Mg2+ ions, the Cu+ and Na+ ions are randomly distributed on the tetrahedral and octahedral sites, respectively. The activation energies due to the various dynamic processes of the lithium ions in inverse spinel-type chlorides obtained by the NMR experiments are E-a = 6.6-6.9 and DeltaG* > 79 kJ mol(-1) (in addition to 23, 29, and 75 kJ mol(-1) obtained by other techniques), respectively. The largest activation energy of >79 kJ mol(-1) corresponds to hopping exchange processes of Li ions between the tetrahedral 8a sites and the octahedral 16d sites. The smallest value of 6.6-6.9 kJ mol(-1), which was derived from the temperature dependence of both the spin-lattice relaxation times T-1 and the correlation times tau(C) of Li-tet, reveals a dynamic process for the Li-tet ions inside the tetrahedral voids of the structure, probably between fourfold 32e split sites around the tetrahedral 8a site. (C) 2002 Elsevier Science (USA). [References: 27]
机译:记录并讨论了关于Li-6和Li-7的MAS NMR光谱,包括一维EXSY(交换光谱)和快速离子导电Li2MgCl4,Li2-xCuxMgCl4,Li2-xNaxMgCl4和Li2ZnCl4的反转恢复实验。锂离子的结构。反尖晶石型固溶体(Li2-xXxMgCl4)-Mg-1(M-1 = Cu,Na)与铜离子仅在四面体位点处的Li MAS NMR信号的化学位移,强度和半峰宽Nagel提出,在八面体位点的钠离子和钠离子以及正常的尖晶石型锌化合物分别证实了反向尖晶石型Li2MgCl4的Li-tet的低场信号和Li-oct的高场信号的分配等。 (2000)。与具有空位和Mg2 +离子聚集的尖晶石型Li2-2xMg1 + xCl4固溶体相反,Cu +和Na +离子分别随机分布在四面体和八面体位置。通过NMR实验获得的反尖晶石型氯化物中锂离子的各种动态过程导致的活化能为Ea = 6.6-6.9和DeltaG *> 79 kJ mol(-1)(除23、29和75 kJ mol(-1)通过其他技术获得)。最大活化能> 79 kJ mol(-1)对应于四面体8a位和八面体16d位之间锂离子的跳跃交换过程。从自旋晶格弛豫时间T-1和Li-tet的相关时间tau(C)的温度相关性得出的最小值6.6-6.9 kJ mol(-1)揭示了一个动态过程在结构的四面体空隙内的Li-tet离子,可能在四面体8a部位周围的四个32e分裂部位之间。 (C)2002 Elsevier Science(美国)。 [参考:27]

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