Original Article
Correlating the effect of dopant type (Al, Ga, Ta) on the mechanical and electrical properties of hot-pressed Li-garnet electrolyte

https://doi.org/10.1016/j.jeurceramsoc.2019.12.054Get rights and content

Abstract

The effect of cubic-phase stabilizing dopant (Al, Ga, Ta) on the mechanical and electrochemical properties of Li garnet solid electrolyte was studied. Dense Li6.25La3Al0.25Zr2O12, Li6.50La3Ta0.50Zr1.5O12, Li6.25La3Ga0.25Zr2O12 were prepared by conventional solid-state synthesis of powder and densified using hot pressing. Ga-LLZO exhibited the highest fracture stress (∼143 MPa), fracture toughness (∼1.22 MPa m1/2) and total conductivity (∼1 mS/cm) of the three materials; however, the bulk conductivity was about 1.5 mS/cm. We believe that the weak grain-boundaries, as evidenced by a predominately intergranular fracture, correlates with a relatively high grain-boundary impedance, thus reducing the value of the total conductivity by about 30 % lower than that for the bulk. Based on the combined mechanical and electrical properties, overall, Li6.25La3Ga0.25Zr2O12 exhibits the most favorable combination of some of the most salient properties of the three dopants. We believe the results of this study will facilitate the commercialization of Li metal batteries using Li-garnet ceramic electrolyte.

Introduction

Owing to its potential to improve battery performance compared to state-of-the-art Li-ion, there has recently been a resurgence in the development of Li metal anode technology [[1], [2], [3]]. However, to date, efforts to cycle Li metal using liquid electrolytes with sufficient coulombic efficiency and safety have been largely insufficient to demonstrate commercial viability for electric vehicles [[4], [5], [6]]. However, Li-ion conducting solid electrolytes are attracting considerable attention to overcome the issues associated with liquid electrolytes [1,7]. The major requirements for the solid Li-ion electrolyte are: high Li-ion conductivity, low electronic conductivity, high relative density, and chemical stability with the electrodes, in particular for metallic Li, sufficient mechanical integrity and adequate rate capability [7,8]. One such solid electrolyte that meets many of these requirements is cubic Li-garnet of the nominal composition Li7La3Zr2O12 (LLZO) [9,10], in which the room temperature phase of Li7La3Zr2O12 is tetragonal [10]. It must be doped with aliovalent cations to form the high conductivity cubic phase at room temperature [11]. A large variety of dopants have been considered, with Al and Ta receiving the most attention [12]. Recently, another dopant Ga has been investigated [13]. In contrast, there is limited information on the mechanical properties of doped LLZO. Most of the mechanical property studies have focused on the elastic properties of Al or Ta doped LLZO. However, to achieve widespread adoption, LLZO will likely be in the form of dense thin (< 30 μm) membranes in which case the more important mechanical properties will be fracture stress and fracture toughness. There are very limited studies on the fracture stress and fracture toughness of Al, Ta, Ga-doped LLZO and how these properties depend on microstructure [14]. This information is required if LLZO is to be used as an electrolyte in solid-state batteries. No data is available for the case where Li garnet consisting of Al, Ta or Ga dopants have been prepared using the same densification method.

It is the purpose of this study to form dense (> 97 % relative density) single-phase cubic Al, Ta, Ga-doped LLZO by uniaxial hot-pressing and compare both their mechanical (fracture stress, characteristic strength, hardness and fracture toughness) and the electrical (bulk conductivity, grain boundary and total conductivity) properties. It was observed that each dopant had a unique effect on both the mechanical and electrochemical properties. Overall, Ga-doping exhibits the most favorable combination of some of the most salient properties of the three dopants in this study.

Section snippets

Powder preparation

Li6.25La3Al0.25Zr2O12 (Al-LLZO), Li6.50La3Ta0.50Zr1.5O12 (Ta-LLZO), Li6.25La3Ga0.25Zr2O12 (Ga-LLZO) were selected as the compositions since these compositions have been reported to yield cubic LLZO with the highest ionic conductivity for the particular doping element [8,12,[15], [16], [17]]. Powders of the three compositions were prepared through solid-state synthesis. The Al-LLZO, Ta-LLZO and Ga-LLZO materials were prepared from the following precursors powders: Lithium Carbonate (99 % Alfa

Materials characterization

From Fig. 1 it can be observed that hot-pressed Ta-LLZO, Al-LLZO and Ga-LLZO are predominantly single phase cubic LLZO. Rietveld refinement revealed that Ta-LLZO, Al-LLZO and Ga-LLZO contained about 2 wt.% La2Zr2O7 (Fig. 1 Supplemental). Examination of Table 1 reveals several important points for hot-pressed Ta-LLZO, Al-LLZO and Ga-LLZO. Firstly, they are highly dense (relative density >97 %). Ga-LLZO exhibited the highest relative density and is close to the theoretical density (99 %).

Conclusions

Dense (>97 % relative density) single-phase cubic Ta-LLZO, Al-LLZO and Ga-LLZO materials were prepared by uniaxial hot pressing. Ga-LLZO had the highest fracture stress value (∼143 MPa) of the three because its critical flaw size was smaller than those of the other two materials. Ga-LLZO also had the highest fracture toughness value (∼ 1.22 MPa-m1/2) of the three materials because its fracture mode is entirely intergranular (weak grain boundaries) leading to a crack deflection toughening

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

BK, RGM, JW, and JS would like to acknowledge financial support from the Advanced Research Project Agency-Energy award DE-AR0000653, the University of Michigan College of Engineering and technical support from the Michigan Center for Materials Characterization. GH and HC also acknowledges support from the Basic Science Research Program (NRF-2018R1D1A1B07048390; NRF2017K1A3A1A30083363) through the NRF of Korea.

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