We synthesized polycrystalline perovskite-type
Li-ion-conducting
oxides (general formula: ABO3), Sr0.5–xLi0.3+2xTi0.3Ta0.7O3 (x = 0.030–0.100),
and assessed their crystal structure, microstructure, ionic conductivity,
and electrochemical stability. Based on first-principles calculations,
local structure changes accompanied by Li-ion diffusion were discussed.
It was found that the average structure of Sr0.5–xLi0.3+2xTi0.3Ta0.7O3 (x = 0.030–0.100)
is a cubic perovskite-type one, and at x = 0.042,
i.e., Sr0.458Li0.384Ti0.3Ta0.7O3, the highest bulk ionic conductivity and the total
ionic conductivity at 300 K were observed to be 1.87 × 10–3 and 1.05 × 10–3 S cm–1, respectively, which are greater than those of La2/3–xLi3xTiO3(LLTO).
The first-principles calculations suggested that BO6 octahedra
are distorted, and the Li-ion diffusion is assisted by the dynamic
distortion of BO6 octahedra coupled with the second-order
Jahn–Teller effect. The reduction potential of Sr0.458Li0.384Ti0.3Ta0.7O3 was
1.6–1.7 V vs Li/Li+, which is comparable to that
of LLTO. A cell using a Sr0.458Li0.384Ti0.3Ta0.7O3 pellet with a deposited thin
film LiCoO2 cathode on one side was successfully operated
as a secondary battery at room temperature, indicating that the compound
can be applied as a solid electrolyte for Li-ion batteries.