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NASICON型LiTiSc(PO)(0 ≤ x ≤ 0.5)系列中的阳离子混溶性和锂迁移率:核磁共振与阻抗联合研究

Cation Miscibility and Lithium Mobility in NASICON LiTiSc(PO) (0 ≤ x ≤ 0.5) Series: A Combined NMR and Impedance Study.

作者信息

Kahlaoui Radhouene, Arbi Kamel, Sobrados Isabel, Jimenez Ricardo, Sanz Jesus, Ternane Riadh

机构信息

Laboratoire d'Application de la Chimie aux Ressources et Substances Naturelles et à l'Environnement (LACReSNE), Université de Carthage, Faculté des Sciences de Bizerte , 7021 Zarzouna, Bizerte, Tunisia.

Instituto de Ciencia de Materiales de Madrid (ICMM), Consejo Superior de Investigaciónes Científicas (CSIC) , Cantoblanco, 28049 Madrid, Spain.

出版信息

Inorg Chem. 2017 Feb 6;56(3):1216-1224. doi: 10.1021/acs.inorgchem.6b02274. Epub 2017 Jan 9.

Abstract

Rhombohedral NASICON compounds with general formula LiTiSc(PO) (0 ≤ x ≤ 0.5) have been prepared using a conventional solid-state reaction and characterized by X-ray diffraction (XRD), nuclear magnetic resonance (NMR), and impedance spectroscopy. The partial substitution of Ti by Sc and Li in pristine LiTi(PO) increases unit-cell dimensions and the number of charge carriers. In Sc-rich samples, the analysis of XRD data and Li/Li, P, and Sc MAS NMR spectra confirms the presence of secondary LiScO and LiScPO phases that reduce the amount of lithium incorporated in the NASICON phase. In samples with x < 0.3, electrostatic repulsions between Li ions located at M1 and M3 sites increase Li mobility. For x ≥ 0.3, ionic conductivity decreases because of secondary nonconducting phases formed at grain boundaries of the NASICON particles (core-shell structures). For x = 0.2, high bulk conductivity (2.5 × 10 S·cm) and low activation energy (E = 0.25 eV) measured at room temperature make LiTiSc(PO) one of the best lithium ionic conductors reported in the literature. In this material, the vacancy arrangement enhances Li conductivity.

摘要

采用传统固态反应法制备了通式为LiTiSc(PO)(0 ≤ x ≤ 0.5)的菱面体NASICON化合物,并通过X射线衍射(XRD)、核磁共振(NMR)和阻抗谱对其进行了表征。在原始的LiTi(PO)中用Sc和Li部分替代Ti会增加晶胞尺寸和载流子数量。在富Sc样品中,XRD数据以及Li/Li、P和Sc的固体高分辨核磁共振谱分析证实了次生LiScO和LiScPO相的存在,这些相减少了掺入NASICON相中的锂的量。在x < 0.3的样品中,位于M1和M3位点的Li离子之间的静电排斥增加了Li的迁移率。对于x ≥ 0.3,由于在NASICON颗粒的晶界处形成了次生非导电相(核壳结构),离子电导率降低。对于x = 0.2,在室温下测得的高体电导率(2.5 × 10 S·cm)和低活化能(E = 0.25 eV)使LiTiSc(PO)成为文献报道的最佳锂离子导体之一。在这种材料中,空位排列提高了Li的电导率。

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