Solid Electrolytes

Perovskite Lithium Conductors

A-site-deficient perovskites in the (Li,La)TiO3 (LLTO) family with bulk ionic conductivities above 1 mS/cm. Grain-boundary resistance and Ti4+ reduction against lithium metal define their engineering limits.

At a glance

Class Statistics

Compounds Tracked
58
Multi-Source DFT
0
With Synthesis Routes
8
Avg. Agreement
—
Overview

What are Perovskite Lithium Conductors?

Perovskite lithium conductors, primarily represented by the lithium lanthanum titanate (LLTO) family, are a class of solid-state electrolyte materials characterized by an ABO3 perovskite crystal structure. These materials are typically engineered to be A-site deficient, which facilitates the migration of lithium ions through the lattice via a vacancy-hopping mechanism. Chemically, they consist of a rigid framework of corner-sharing TiO6 octahedra, with lithium and lanthanum cations occupying the A-sites. The high bulk ionic conductivity of these materials makes them significant candidates for next-generation solid-state batteries, as they offer the potential for high power density and improved safety compared to traditional liquid electrolytes. However, their practical application is constrained by several engineering hurdles. Notably, the high grain-boundary resistance significantly limits total ionic transport across polycrystalline samples. Furthermore, the thermodynamic instability of the Ti4+ species when in direct contact with lithium metal leads to reduction, causing electronic conductivity that can result in short-circuiting. Despite these challenges, LLTO remains a cornerstone of solid-state ionics research. Notable members include various compositions within the Li(3x)La(2/3-x)TiO3 series, where the precise stoichiometry of lithium and lanthanum is tuned to optimize the vacancy concentration and lattice parameters. Ongoing research focuses on grain-boundary engineering and protective coating strategies to mitigate reactivity, aiming to harness the exceptional bulk transport properties of these perovskites for stable, high-performance energy storage devices.

Members

Top Perovskite Lithium Conductors

Ranked by data richness — literature synthesis coverage, multi-source DFT corroboration, and patent activity.

FormulaBand GapBest EAH (eV/atom)StabilityDFT SourcesRecipes
LiLaTi2O61.79–2.02 eV0.0442Metastable114
LaLiO6Ti21.68–1.77 eV0.0623Metastable—14
La0.5Li0.5O3TiMetallic / not reported—Not assessed—14
LaLiO12Sr2Ti41.83 eV0.0582Metastable—2
La0.56Li0.33O3TiMetallic / not reported—Not assessed—6
LiLaTiO42.24–2.31 eV0.0236Stable10
La0.57Li0.3O3TiMetallic / not reported—Not assessed—5
La2Li2O10Ti32.07–2.53 eV0.0204Near hull (likely stable)—0
LaLiO4Ti2.26 eV0.0288Metastable—0
La5LiO24Ti81.93–2.12 eV0.0279Metastable—0
La2LiNaO12Ti41.67–2.00 eV0.0309Metastable—0
La5Li3Nb2O26Ti61.91 eV0.0573Metastable—0
LiLa5Ti8O242.04 eV0.0386Metastable—0
Cr3La8Li3O36Ti91.30 eV0.0669Metastable—0
CrLa2LiO6Ti0.22 eV0.2914Above hull—0
CrLa2LiO9Ti22.26 eV0.0424Metastable—0
HfLaLiO6Ti2.38 eV0.1870Above hull—0
La3Li2NaO18Ti61.93 eV0.0488Metastable—0
La3LiNa2O18Ti62.07 eV0.0247Near hull (likely stable)—0
La3LiO9Ti22.69 eV0.0305Metastable—0
La4Li5Nb7O28Ti0.77 eV0.0505Metastable—0
LaLiO9SrTi31.84 eV0.0749Metastable—0
Li2La2Ti3O102.08 eV0.0245Near hull (likely stable)—0
Li7La3Ti2O123.58 eV0.0274Metastable—0
La0.6Li0.2O3TiMetallic / not reported—Not assessed—3
La2Li2O8Ti22.96 eV—Not assessed—0
La5Li1O24Ti82.35 eV—Not assessed—0
La0.61Li0.18O3TiMetallic / not reported—Not assessed—2
La2LiO6TiMetallic / not reported0.0628Metastable—0
La3Li2Nb2O13Ti2Metallic / not reported0.1070Above hull—0
La3LiO12Ti4Metallic / not reported0.0287Metastable—0
CrLa3LiO12Ti3Metallic / not reported0.0579Metastable—0
La4Li8Nb7O28TiMetallic / not reported0.0360Metastable—0
La4LiO12Ti3Metallic / not reported0.0306Metastable—0
La5Li3O24Ti8Metallic / not reported0.0734Metastable—0
La5Li4Nb2O26Ti6Metallic / not reported0.0490Metastable—0
LaLiO12Ti4Metallic / not reported0.2030Above hull—0
LiLa3Ti4O12Metallic / not reported—Not assessed—0
La0.6Li0.18O3TiMetallic / not reported—Not assessed—0
LiLa2TiO6Metallic / not reported—Not assessed—0
LiLa4Ti3O12Metallic / not reported—Not assessed—0
Cr0.44La1.33Li0.44O6Ti1.56Metallic / not reported—Not assessed—0
Cr0.66La1.33Li0.66O6Ti1.33Metallic / not reported—Not assessed—0
La2.25Li2Nb1.25O13Ti2.75Metallic / not reported—Not assessed—0
La0.52Li0.43O3TiMetallic / not reported—Not assessed—0
La0.59Li0.21O3TiMetallic / not reported—Not assessed—0
La0.59Li0.24O3TiMetallic / not reported—Not assessed—0
La0.62Li0.14O3TiMetallic / not reported—Not assessed—0
La0.62Li0.18O3TiMetallic / not reported—Not assessed—0
La0.62Li0.38O3TiMetallic / not reported—Not assessed—0
Reference

Frequently Asked Questions

How many perovskite lithium conductors are in the database?

58 perovskite lithium conductors are tracked, of which 0 have multi-source DFT validation and 8 have documented synthesis routes.

More questions
What is the most data-rich perovskite lithium conductor?
LiLaTi2O6 is the most thoroughly characterized, with 8 reported structures.
Which perovskite lithium conductor has the widest band gap?
Among the top compounds, Li7La3Ti2O12 has the widest reported DFT band gap (3.58 eV).
What is the primary mechanism of lithium-ion transport in LLTO?
Lithium ions move through the perovskite lattice primarily via a vacancy-hopping mechanism, where ions migrate between available A-site vacancies within the rigid titanium-oxygen framework.
Why is the grain boundary a major limitation for these materials?
In polycrystalline samples, the grain boundaries often exhibit significantly higher resistance than the bulk material, which severely restricts the overall ionic conductivity of the electrolyte.
Can perovskite lithium conductors be used directly with lithium metal anodes?
Generally, no. The Ti4+ ions in the perovskite structure are prone to reduction when in contact with lithium metal, which increases electronic conductivity and can lead to internal short-circuiting.
How does A-site deficiency affect the performance of these conductors?
A-site deficiency is crucial because it introduces the necessary vacancies in the crystal lattice that allow lithium ions to move; without these vacancies, the ionic conductivity would be negligible.
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