NMR and impedance studies of nanocrystalline and amorphous ion conductors: lithium niobate as a model system

被引:161
作者
Heitjans, Paul [1 ]
Masoud, Muayad [1 ]
Feldhoff, Armin [1 ]
Wilkening, Martin [1 ]
机构
[1] Leibniz Univ Hannover, Inst Phys Chem & Electrochem, D-30167 Hannover, Germany
来源
FARADAY DISCUSSIONS | 2007年 / 134卷
关键词
D O I
10.1039/b602887j
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Lithium niobate has been chosen as a model system for spectroscopic studies of the influence of different structural forms and preparation routes of an ionic conductor on its ion transport properties. The Li diffusivity in nanocrystalline LiNbO(3), prepared either mechanically by high energy ball milling or chemically by a sol-gel route, was studied by means of impedance and solid state (7)Li NMR spectroscopy. The Li diffusivity turned out to be strongly correlated with the different grain boundary microstructures of the two nanocrystalline samples and with the degree of disorder introduced during preparation, as seen especially by HRTEM and EXAFS. Although in both samples nanostructuring yields an enhancement of the Li diffusivity compared to that in coarse grained LiNbO(3), the Li diffusivity in ball milled LiNbO(3) is much higher than in chemically prepared nanocrystalline LiNbO(3). The former LiNbO(3) sample has a large volume fraction of highly disordered interfacial regions which seem to be responsible for fast Li diffusion and to have a structure very similar to that of the amorphous form. This is in contrast to the chemically prepared sample where these regions have a smaller volume fraction.
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页码:67 / 82
页数:16
相关论文
共 50 条
[1]  
[Anonymous], 1998, Lithium Ion Batteries: Fundamentals and Performance
[2]   NMR relaxation study of ion dynamics in nanocrystalline and polycrystalline LiNbO3 [J].
Bork, D ;
Heitjans, P .
JOURNAL OF PHYSICAL CHEMISTRY B, 1998, 102 (38) :7303-7306
[3]  
Brossmann U, 2004, REV ADV MATER SCI, V6, P7
[4]   18O diffusion in nanocrystalline ZrO2 [J].
Brossmann, U ;
Södervall, U ;
Würschum, R ;
Schaefer, HE .
NANOSTRUCTURED MATERIALS, 1999, 12 (5-8) :871-874
[5]  
Chadwick AV, 2005, PHYS STATUS SOLIDI C, V2, P302, DOI 10.1002/pssc.200460170
[6]   Small, but perfectly formed: The microstructure of nanocrystalline oxides [J].
Chadwick, AV .
RADIATION EFFECTS AND DEFECTS IN SOLIDS, 2003, 158 (1-6) :21-30
[7]   A comparison of the extended x-ray absorption fine structure of nanocrystalline ZrO2 prepared by high-energy ball milling and other methods [J].
Chadwick, AV ;
Pooley, MJ ;
Rammutla, KE ;
Savin, SLP ;
Rougier, A .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2003, 15 (03) :431-440
[8]  
Chandra S., 1981, SUPERIONIC SOLIDS PR
[9]   Nonstoichiometry and Electrical Conductivity of Nanocrystalline CeO\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${2 - x} $$ \end{document} [J].
E B Lavik ;
I Kosacki ;
H L Tuller ;
Y-M Chiang ;
J Y Ying .
Journal of Electroceramics, 1997, 1 (1) :7-14
[10]   A combined EXAFS and diffraction study of pure and doped nanocrystalline tin oxide [J].
Davis, SR ;
Chadwick, AV ;
Wright, JP .
JOURNAL OF PHYSICAL CHEMISTRY B, 1997, 101 (48) :9901-9908