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Lithium Ion Conductivity of A‐Site Deficient Perovskite Solid Solution La0.67 − x Li3x TiO3
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1994
Year
Materials ScienceLithium Ion ConductivitySolid-state IonicEngineeringPerovskite Solar CellSubstitution MechanismLi-ion Battery MaterialsLithium-ion BatteryApplied PhysicsPerovskite MaterialsCondensed Matter PhysicsEnergy StorageHalide PerovskitesMaximum ConductivityPerovskite SubcellsChemistrySolid-state BatteryFunctional Materials
solid solution forms in the range by the substitution mechanism . Superstructure reflections observed in this range are consistent with a superlattice consisting of the stacking of two perovskite subcells. A line‐splitting phenomenon observed for indicates that the tetragonal distortion of the cubic perovskite subcell occurs. The solid solutions exhibit high lithium ion conductivities greater than 10−4 S cm−1 at room temperature in a wide range, . A maximum conductivity of is found at . The dome‐shaped composition dependence of conductivity indicates that the conduction mechanism involves the movement of lithium ions through the A‐site vacancies.