Superionic bulk conductivity in Li1.3Al0.3Ti1.7(PO4)3 solid electrolyte

被引:62
|
作者
Mertens, Andreas [1 ,2 ,3 ]
Yu, Shicheng [1 ,3 ]
Schoen, Nino [1 ,3 ]
Gunduz, Deniz C. [1 ,3 ]
Tempel, Hermann [1 ]
Schierholz, Roland [1 ]
Hausen, Florian [1 ,3 ]
Kungl, Hans [1 ]
Granwehr, Josef [1 ,4 ]
Eichel, Ruediger-A [1 ,3 ]
机构
[1] Forschungszentrum Julich, Inst Energy & Climate Res, Fundamental Elect IEK9, D-52425 Julich, Germany
[2] Helmholtz Inst Munster HI MS, D-48149 Munster, Germany
[3] Rhein Westfal TH Aachen, Inst Phys Chem, D-52074 Aachen, Germany
[4] Rhein Westfal TH Aachen, Inst Tech & Macromol Chem, D-52074 Aachen, Germany
关键词
Solid electrolyte; LATP; Impedance spectroscopy; Distribution of relaxation times; Activation energy; Ionic conductivity; Brick layer model; IONIC-CONDUCTIVITY; GRAIN-BOUNDARIES; IMPEDANCE SPECTROSCOPY; LITHIUM MOBILITY; NMR; MICROSTRUCTURES; CERAMICS;
D O I
10.1016/j.ssi.2017.07.023
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
Superionic lithium -ion conductors of NASICON structure are promising solid electrolytes for all solid-state batteries. But still further improvement of the ionic conductivity is necessary to be competitive with today's liquid electrolytes. This requires a thorough understanding of grain and grain boundary ion transport properties. However, distinguishing between the impedance contributions of both regimes proved to be difficult before, due to their overlapping time constants, which often necessitate measurements below 0 degrees C. In contrast, we analyze a Li1.3Al0.3Ti1.7(FO4)(3) (LATP) solid electrolyte under battery operation temperatures between 10 degrees C and 50 degrees C by impedance measurements in combination with a distribution of relaxation time analysis in two dimensions (2D-DRT). By correlation with microstructural observation in the laser-scanning microscope (LSM), scanning electron microscope (SEM) and atomic force microscope (ARV!) the dominating ion transport pathway is determined within a bricklayer model on a macroscopic scale. Moreover, the ionic conductivities of grain and grain boundary are calculated. For the grain, conductivity values of 2 mS cm(-1) at room temperature are found. The ion transport activation energies of both domains are determined to be 182 meV and 430 meV, respectively. Optimization routes for further ionic conductivity improvements are derived.
引用
收藏
页码:180 / 186
页数:7
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