| HS Code | 925819 |
| Chemical Name | Lithium Lanthanum Titanium Oxide |
| Chemical Formula | Li0.33La0.56TiO3 |
| Molecular Weight | 175.95 g/mol |
| Appearance | White to off-white powder or sintered ceramic pellet |
| Crystal Structure | Perovskite-type (tetragonal, space group P4/mmm) |
| Density | ~5.0 g/cm³ |
| Bulk Ionic Conductivity | ~1 × 10⁻³ S/cm at 25 °C |
| Activation Energy For Ionic Conduction | ~0.30 eV |
| Band Gap | ~3.6 eV |
| Melting Point | Decomposes above ~1400 °C |
| Solubility In Water | Insoluble |
| Lithium Ion Transference Number | ~1 |
As an accredited Lithium Lanthanum Titanium Oxide factory, we enforce strict quality protocols—every batch undergoes rigorous testing to ensure consistent efficacy and safety standards.
| Packing | Supplied in sealed polyethylene bag within a fiber drum. Quantity: 1 kg net. Store tightly closed in dry, cool conditions. |
| Container Loading (20′ FCL) | 20′ FCL: 20-foot container loaded with drums/bags of Lithium Lanthanum Titanium Oxide, secured, labeled, and ventilated per chemical safety regulations. |
| Shipping | Ship Lithium Lanthanum Titanium Oxide as a sealed, moisture-proof container with desiccant, packed in sturdy outer packaging. Avoid exposure to humidity and extreme temperatures. Label as non-hazardous industrial material; use protective gloves and dust mask during handling. Transport via standard ground freight, keeping packages upright and secure. |
| Storage | Store Lithium Lanthanum Titanium Oxide in a tightly sealed, inert container under a dry, moisture-free atmosphere, ideally inside an argon-filled glovebox. Keep away from water, humidity, and acidic vapors to prevent degradation. Store at room temperature in a cool, dry, well-ventilated area, protected from light and physical damage. |
| Shelf Life | Shelf life: 2–5 years when stored sealed, dry, and away from moisture; handle under inert atmosphere to prevent degradation. |
In a dry-room coating line processing poly(ethylene oxide) (PEO) and lithium bis(trifluoromethanesulfonyl)imide (LiTFSI), lithium lanthanum titanium oxide (Li3xLa(2/3)−xTiO3) powder with a median particle size of 0.2–1.0 µm is incorporated as a passive ceramic filler. The LLTO is pre-dried at 200 °C under −0.1 MPa vacuum for 12 h; batch-to-batch variation in LLTO surface moisture is a recognized cause of impedance scatter if the pre-drying step is not standardized, and surface moisture above 50 ppm increases grain boundary impedance after dispersion. The slurry is prepared at an ethylene oxide-to-lithium molar ratio of 8:1 to 16:1, with LLTO loading held at 5 wt% to 15 wt% of the dry solids. Anhydrous acetonitrile is used as the carrier solvent, and the mixture is dispersed in a high-shear mixer at 5,000 rpm for 30 min; batches with visible agglomerates are passed once through a three-roll mill with a gap setting of 25 µm. The slurry is cast onto a poly(ethylene terephthalate) release liner through a doctor blade with a wet film thickness of 150–400 µm. Drying proceeds at 60 °C under a dry nitrogen stream until the residual solvent concentration falls below 200 ppm. Ionic conductivity is measured by electrochemical impedance spectroscopy using stainless-steel blocking electrodes, with an AC amplitude of 10 mV and a frequency range from 1 MHz to 0.1 Hz. Composite films containing 10 wt% LLTO typically exhibit total ionic conductivity in the range of 10⁻⁵ S·cm⁻¹ to 10⁻⁴ S·cm⁻¹ at 25 °C, whereas loadings above 15 wt% tend to produce agglomeration-driven conductivity loss and reduced film uniformity. Tensile properties are evaluated according to ASTM D882-18; ceramic loading generally increases tensile modulus while lowering elongation at break. Because lanthanum ions leach under acidic conditions, aqueous formulations are avoided, and processing is confined to anhydrous solvents. The resulting free-standing membranes are used as composite solid electrolytes in lithium-ion cells where direct contact with metallic lithium is not required.
A tape-casting slurry for monolithic LLTO separator tapes is formulated at 35–55 vol% ceramic solids in an ethanol/toluene solvent system, with poly(vinyl butyral) binder at 3–5 wt%, a phthalate-free plasticizer at 3–5 wt%, and a phosphate ester dispersant. Green tape thickness is set between 25 µm and 200 µm by doctor blade gap adjustment, and the tape is dried at 60 °C before debinding. Binder burn-out is conducted at 400–600 °C for 2 h with a ramp rate of 2 °C·min⁻¹; sintering follows at 1100–1350 °C for 2–6 h in flowing oxygen. Lithium oxide volatilization above 1000 °C is controlled by placing lithium-rich packing powder around the green tape or by using a closed crucible to reduce lanthanum titanate secondary phase formation. Final sintered density above 95% of theoretical is required for separator use. Electrochemical impedance spectroscopy reveals separate bulk and grain boundary arcs; bulk conductivity at 25 °C commonly falls between 10⁻⁴ S·cm⁻¹ and 10⁻³ S·cm⁻¹, while total conductivity remains between 10⁻⁵ S·cm⁻¹ and 10⁻⁴ S·cm⁻¹ because grain boundary resistance dominates. Sintered tapes are polished to 1 µm diamond finish to reduce interfacial roughness, and flexural strength is measured by ASTM C1161-18. Direct contact with metallic lithium is avoided because Ti⁴⁺ reduction at low potential introduces electronic conductivity and accelerates degradation. The finished separator tape is used against high-voltage cathode layers or with a Li-stable interlayer when a lithium metal anode is employed.
| Property | Standard | Test condition |
|---|---|---|
| Particle size distribution | ISO 13320:2020 | Laser diffraction, wet dispersion in isopropanol |
| Moisture content | ISO 760 | Karl Fischer coulometric titration |
| Sintered density | ISO 1183-1:2019 | Archimedes immersion in ethanol |
| Film tensile properties | ASTM D882-18 | Gauge length 50 mm, test speed 25 mm·min⁻¹ |
| Ceramic flexural strength | ASTM C1161-18 | Four-point bending, span 40 mm |
A solid-state cathode layer containing LiNi0.6Mn0.2Co0.2O2 (NMC622) and LLTO powder is processed for bulk all-solid-state cells. The cathode formulation comprises 60–70 wt% NMC622, 25–35 wt% LLTO, and 2–5 wt% conductive carbon, with the LLTO fraction adjusted to balance ionic percolation and electrochemically active volume. The LLTO powder used in this layer has a median particle size of 0.3–0.8 µm to maximize contact area with the cathode grains. Dry mixing is performed in a planetary centrifugal mixer at 2,000 rpm for 15 min; a slurry route is used only when subsequent solvent removal can be completed below 150 °C to prevent cathode surface degradation. Green cathode layers are compacted under uniaxial pressure of 150–350 MPa, producing a green density between 60% and 75% of theoretical. Co-sintering above 900 °C is avoided because interdiffusion of transition metals and lanthanum leads to resistive secondary phases; hot-pressing or low-temperature sintering is preferred. Because Ti⁴⁺ in LLTO can be reduced at low potential, the cathode composite is not discharged below 2.5 V versus Li⁺/Li when LLTO is in the cathode layer. Electrochemical performance is tested in half cells with lithium anodes through a catholyte-compatible interlayer, and impedance is recorded from 1 MHz to 10 mHz. The finished cathode layer is laminated onto a ceramic separator tape under 100–200 MPa at 80 °C to reduce interfacial porosity.
LLTO sputtering targets are produced from calcined powder by cold isostatic pressing at 200–300 MPa followed by sintering in oxygen; lithium-enriched targets with 10–30 at% excess Li₂CO₃ are used to compensate lithium loss during deposition. Target diameter is typically 50–150 mm, and density above 90% of theoretical is required to avoid arcing. Thin-film deposition is performed by RF magnetron sputtering at a power density of 2–5 W·cm⁻² and a process pressure of 0.5–2 Pa, with an argon-to-oxygen ratio between 95:5 and 80:20. Substrate temperature during deposition ranges from 25 °C to 600 °C; amorphous films are post-annealed at 500–700 °C in oxygen for 1 h to promote perovskite crystallization. Film thickness is maintained between 100 nm and 500 nm for solid electrolyte layers in thin-film cells. Ionic conductivity is extracted from impedance measurements on Pt/LLTO/Pt capacitor structures; room-temperature values for sputtered films are generally lower than bulk ceramics and fall between 10⁻⁶ S·cm⁻¹ and 10⁻⁵ S·cm⁻¹, depending on crystallographic texture and lithium content. Because the as-deposited film is susceptible to lithium loss and grain boundary depletion, post-deposition lithium compensation is not generally possible, so target stoichiometry is controlled instead. The LLTO layer is deposited only on cathode stacks; direct contact with a lithium metal anode is avoided due Ti⁴⁺ reduction.
For polyolefin separator coating lines operating in low-humidity cleanrooms, LLTO nanoparticles are dispersed into poly(vinylidene fluoride-co-hexafluoropropylene) (PVDF-HFP) solutions to produce ceramic-polymer composite coatings. The PVDF-HFP content is 85–95 wt% of the dry coating, and LLTO is added at 5–15 wt%; higher loadings increase slurry viscosity and produce slot-die streak defects. PVDF-HFP is dissolved in anhydrous N-methyl-2-pyrrolidone at 50 °C, then LLTO is added after full polymer dissolution and dispersed with a high-shear rotor-stator mixer at 10,000 rpm. The coating is applied to a polyethylene separator substrate by slot-die or gravure coating at line speeds between 5 m·min⁻¹ and 30 m·min⁻¹, with a dry coating thickness of 2–10 µm. Drying ovens are operated at 60–80 °C to remove residual solvent below 200 ppm. After activation with 1 M LiPF6 in ethylene carbonate/dimethyl carbonate 1:1 v/v, the gel electrolyte maintains ionic conductivity governed by the liquid phase, while the LLTO filler improves dimensional stability under thermal abuse. Coating adhesion and tensile properties are evaluated according to ASTM D882-18; delamination during slitting is an observed failure mode when LLTO loading exceeds 15 wt% or when the separator substrate has not been corona-treated. The coated separator is used in lithium-ion cells as a ceramic-reinforced gel polymer electrolyte membrane.
LLTO sintered discs function as lithium-ion conducting solid electrolytes in potentiometric carbon dioxide sensing cells where a carbonate auxiliary electrode is attached to one side and a reference electrode to the other. The cell potential follows the Nernst equation for the carbonate decomposition equilibrium, and the LLTO disc provides lithium-ion transport between the electrodes. Discs are fabricated from the same high-density ceramic route used for separator tapes, with thickness between 0.5 mm and 2 mm and surface roughness below 0.1 µm after polishing. The operating temperature is typically 300–500 °C, where LLTO grain boundary conductivity improves sufficiently for sensor response; published data for this specific configuration is limited, and sensor response time depends on electrode morphology and carbonate layer thickness. The LLTO disc is not exposed to reducing atmospheres because Ti⁴⁺ reduction increases electronic conductivity and depresses sensor accuracy. Sensor housings use alumina or quartz envelopes, and the LLTO electrolyte is sealed with glass or ceramic frit to separate the reference gas.
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Lithium lanthanum titanium oxide (LLTO) with nominal stoichiometry Li0.33La0.557TiO3 is a perovskite-structured lithium-ion conductive ceramic supplied as a high-purity powder. The crystalline phase at ambient temperature is tetragonal P4/mmm, verified by powder X-ray diffraction using Cu Kα radiation and Rietveld refinement. Product designations LLTO-1.2, LLTO-3.8, and LLTO-8.0 correspond to median particle size targets of 1.2 µm, 3.8 µm, and 8.0 µm Dv50. Each grade is prepared from the same calcined perovskite lot and differs only in downstream deagglomeration and air classification; this avoids phase-composition drift across particle-size variants. The powder is packaged under nitrogen in sealed aluminium-laminated bags with moisture content below 0.2 wt% as measured by Karl Fischer titration.
The material functions as a ceramic electrolyte separator or as a conductive filler in polymer-ceramic composite electrolytes. In sintered form, bulk ionic conductivity is typically 1.0 × 10−3 S cm−1 at 25 °C, while total polycrystalline conductivity is attenuated to 10−4–10−5 S cm−1 by grain-boundary impedance. Electronic conductivity remains below 1 × 10−8 S cm−1. The chemical specification includes total rare-earth oxide content of 99.5 % minimum and lithium excess of 2 wt% over stoichiometric target to compensate for volatilization during sintering. Trace impurities of aluminium, sodium, and zirconium are controlled below 500 ppm, 200 ppm, and 300 ppm, respectively, as determined by inductively coupled plasma mass spectrometry following acid digestion.
In polycrystalline LLTO, the dominant impedance originates at grain boundaries rather than in the perovskite lattice. Electrochemical impedance spectroscopy on sintered pellets with sputtered gold blocking electrodes typically resolves a high-frequency bulk semicircle with capacitance on the order of 10−12 F and a mid-frequency grain-boundary semicircle with capacitance near 10−10 F. The bulk ionic conductivity derived from the high-frequency intercept follows Arrhenius behaviour with activation energy near 0.30 eV. Across individual grain boundaries, lithium depletion and secondary phase enrichment reduce conductivity by up to two orders of magnitude. Sintering conditions that produce average grain sizes above 20 µm reduce the number of resistive boundaries per unit path length, but excessive grain growth can increase lithium loss and pore coalescence.
Grain-boundary conductivity is improved by adding 0.5–2.0 wt% of lithium excess or by hot-pressing at 1150 °C and 40 MPa in graphite tooling. However, direct contact with graphite at high temperature can reduce Ti4+ to Ti3+; therefore, molybdenum foil or boron nitride isolation is required when hot pressing is used. Published data for the effect of hot-press soaking time on LLTO grain-boundary conductivity are limited, but laboratory lots show that soak times beyond 4 h produce no measurable improvement in total conductivity under argon.
Release criteria for each LLTO grade are determined by laser diffraction, Archimedes density after sintering, and four-point DC electronic resistance measurements. The following specification table applies to calcined powder prior to tape casting or pellet pressing.
| Parameter | Test method | Value |
|---|---|---|
| Particle size Dv50, grade LLTO-1.2 | ISO 13320:2020 | 1.2 ± 0.3 µm |
| Particle size Dv50, grade LLTO-3.8 | ISO 13320:2020 | 3.8 ± 0.5 µm |
| Particle size Dv50, grade LLTO-8.0 | ISO 13320:2020 | 8.0 ± 0.8 µm |
| Specific surface area, LLTO-1.2 | ISO 9277:2022 | 2.0–4.0 m2 g−1 |
| Perovskite phase purity | XRD-Rietveld | ≥ 98 %; La2Ti2O7 ≤ 2 % |
| Loss on ignition at 1000 °C | ISO 11358-1:2022 | ≤ 1.5 wt% |
| Sintered density after 1350 °C, 2 h | ASTM C373-18 | ≥ 4.75 g cm−3 |
| Total metal impurities | ISO 17294-2:2016 | Al ≤ 500 ppm, Fe ≤ 200 ppm, Na ≤ 200 ppm |
| Moisture content | ISO 15512:2019 | ≤ 0.2 wt% |
Storage at relative humidity above 60 % for more than 72 h causes surface carbonate formation detectable by FTIR at 1430 cm−1. Pre-drying at 120 °C under vacuum for 2 h restores flowability and prevents carbon dioxide retention during sintering.
For tape-cast LLTO separator layers, a slurry batch of 100 g powder is dispersed in a solvent mixture of anhydrous ethanol and methyl ethyl ketone at 60/40 wt% with polyvinyl butyral binder and benzyl butyl phthalate plasticizer. The slurry is deaired under 50 kPa vacuum and cast with a doctor blade gap of 120–180 µm on silicone-coated polyester film. After drying at 65 °C, the green tape is cut, laminated at 70 °C and 15 MPa, and fired in a covered alumina sagger with LLTO sacrificial mother powder to maintain lithium vapour pressure. Debinding is conducted at 600 °C in an oxygen-nitrogen atmosphere with residual oxygen content below 100 ppm. Sintering is performed at 1350 °C for 2–6 h in oxygen flow of 100 mL min−1. The resulting sintered thickness ranges from 70 to 110 µm, and relative density measured by the Archimedes method exceeds 94 % of theoretical density 5.06 g cm−3.
Lithium volatilization is the principal processing boundary. Weight loss during sintering should not exceed 0.8 wt%; larger losses shift the perovskite A-site occupancy and reduce bulk conductivity. Powder bed ratios of 1:3 tape-to-mother-powder by mass are used to stabilise lithium activity. Sintering above 1380 °C triggers secondary phase formation, including La2Ti2O7 and TiO2, detectable by XRD at volume fractions below 2 %. Sintering below 1300 °C results in residual porosity above 8 vol% and a sharp drop in mechanical strength; no closed-porosity threshold is achieved.
In solid-state battery assembly, LLTO is employed as a separator layer in cells with lithium iron phosphate or lithium cobalt oxide cathodes and lithium metal anodes only when an interfacial coating is interposed. Direct contact between LLTO and lithium metal is avoided because Ti4+ is reduced at potentials below approximately 1.5 V vs Li/Li+, creating electronic conductivity and short-circuit pathways. Gold, germanium, lithium phosphorus oxynitride, or polymer interlayers with thickness below 100 nm are used to mitigate interfacial degradation. For composite cathodes, LLTO powder is dry-mixed with coated LiNi0.8Co0.1Mn0.1O2 at 2–5 wt% to improve lithium-ion migration through the cathode thickness.
In polymer-ceramic composite electrolytes, the LLTO-1.2 grade is dispersed in poly(ethylene oxide) at 20 wt% using high-shear planetary mixing at 2000 rpm for 30 min. The resulting film exhibits ionic conductivity near 10−4 S cm−1 at 60 °C. Above 30 wt% LLTO loading, the composite becomes brittle and film-forming capability is lost. Addition of 5 wt% propylene carbonate plasticizer partially restores flexibility but increases electrolyte evaporation loss above 70 °C.
In hybrid electrolyte architectures, LLTO differs from garnet-type Li7La3Zr2O12 (LLZO) primarily in electrochemical stability and processing temperature. LLTO densifies at 1300–1360 °C, which is 100–200 °C lower than conventional LLZO sintering to closed porosity. The lower sintering temperature permits co-sintering with selected phosphate-based cathode coatings that decompose above 1400 °C. However, LLTO cannot be used directly against lithium metal, whereas LLZO with suitable surface cleaning can be cycled against lithium metal. Total ionic conductivity of LLTO polycrystalline pellets is commonly 1 × 10−4 to 5 × 10−5 S cm−1, one order lower than dense LLZO membranes with total conductivity near 3 × 10−4 S cm−1. Against NASICON-type LATP, LLTO offers lower raw-material cost and avoids phosphorus volatility during thermal processing, but LATP sintered ceramics can achieve total conductivity up to 7 × 10−4 S cm−1 at room temperature with sintering below 1000 °C. Sulfide electrolytes such as Li6PS5Cl exhibit higher conductivity near 10−2 S cm−1 but require cell assembly in dry-room conditions below −40 °C dew point.
| Electrolyte | Total conductivity at 25 °C (S cm−1) | Sintering temperature for dense ceramic (°C) | Direct lithium metal stability | Air sensitivity |
|---|---|---|---|---|
| LLTO | 10−4–10−5 | 1300–1360 | Unstable below 1.5 V | Low; surface carbonation after prolonged humidity |
| LLZO | 3 × 10−4 | 1150–1230 | Stable after surface treatment | Low; forms Li2CO3 on moist air exposure |
| LATP | 7 × 10−4 | 900–1000 | Unstable | Low |
| Li6PS5Cl | 10−2 | Room-temperature pressing; not conventionally sintered | Reactive but can form passivating interface | Highly sensitive to moisture; generates H2S |
For separator integration, LLTO tape can be handled in ordinary dry-room conditions with dew point below −20 °C; this is less stringent than sulfide electrolyte handling. Cleaning of sintered LLTO surfaces before electrode deposition is performed by argon-ion milling at 0.5 kV for 3 min to remove lithium carbonate films. Devices assembled with sintered LLTO and LiFePO4 cathodes have demonstrated cycle stability under limited laboratory configurations, but published data for long-term cycling beyond 500 cycles at 1C remain limited.