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Solid-State Electrolytes

    • Product Name: Solid-State Electrolytes
    • Factroy Site: Yudu County, Ganzhou, Jiangxi, China
    • Price Inquiry: admin@ascent-chem.com
    • Manufacturer: Ascent Petrochem Holdings Co., Limited
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    Specifications
    HS Code 705587
    Ionic Conductivity 10^-4 to 10^-2 S/cm at room temperature
    Electrochemical Stability Window 0 to 5 V vs Li/Li+
    Thermal Stability stable up to 200-300°C
    Mechanical Strength high fracture toughness and shear modulus
    Density 1.7-5.5 g/cm3 depending on material
    Chemical Compatibility stable against lithium metal and electrode materials
    Interfacial Resistance 10-1000 ohm cm2
    Activation Energy 0.2-0.5 eV
    Transference Number close to 1 for lithium ions
    Cost moderate to high depending on raw materials and processing

    As an accredited Solid-State Electrolytes factory, we enforce strict quality protocols—every batch undergoes rigorous testing to ensure consistent efficacy and safety standards.

    Packing & Storage
    Packing Packaged in hermetically sealed, argon-filled containers to prevent moisture and oxygen exposure. Quantity: 1 kg.
    Container Loading (20′ FCL) Solid-state electrolytes, moisture-sensitive, packed in sealed drums, palletized and secured, loaded into a 20-foot FCL container.
    Shipping Solid-state electrolytes ship in sealed, moisture-resistant containers under inert atmosphere to prevent degradation. No hazardous goods classification if stable, but protect from impact and humidity. Use dry, insulated packaging, avoid strong oxidizers, and label as sensitive to air/moisture. Standard ground freight with temperature control recommended.
    Storage Store solid-state electrolytes in airtight, moisture-free containers within an argon-filled glovebox or desiccator. Protect from humidity, oxygen, and contamination. Keep at room temperature, away from heat sources and direct sunlight. Verify container seals regularly. Handle under inert gas to preserve ionic conductivity and prevent degradation. Label clearly with composition and date.
    Shelf Life Shelf life depends on storage; keep sealed, dry, and inert. Typically stable for months to years under proper conditions.
    Application of Solid-State Electrolytes

    Solid electrolyte materials are supplied as sulfide glass-ceramic powders, oxide ceramic powders, sputtering targets, and screen-printable inks. Downstream application tracks differ by cathode active material, cell assembly method, atmosphere control, and certification scheme. The following scenarios reference production-scale equipment behavior and validation standards, not laboratory half-cell data.

    Table 1. Application track and critical boundary matrix
    Application trackSolid electrolyte classPrimary standard setCritical process limit
    Automotive tractionLi6PS5Cl sulfide argyroditeIATF 16949:2016, GB 38031-2020Dew point ≤ -40°C, stack pressure 5–150 MPa
    Consumer micro-batteryLiPON thin filmIEC 62133-2:2017, UL 1642Film thickness ≤ 5 μm
    Medical implantableLLZO cubic garnetISO 13485:2016, ISO 14971:2019Sintering aid window 800–900°C
    Borehole and geothermalLATP NASICONMIL-STD-810H, RTCA DO-160GContinuous operation 150°C
    Industrial IoT sensor nodeLATP printed filmRoHS 2011/65/EU, REACH 1907/2006Sintering 800–1000°C, ramp ≤ 5°C/min

    How Does Sulfide Argyrodite Electrolyte Enter Automotive Cell Coating Lines Without Hydrolysis?

    Sulfide argyrodite Li6PS5Cl is selected for automotive traction cells because pressed-pellet ionic conductivity values of 1 mS/cm to 10 mS/cm reduce internal resistance in thick cathode composites. Moisture exposure is the primary processing constraint. The P-S bond hydrolyzes at dew points above -30°C, releasing H2S and forming oxysulfide surface phases with resistivity above 10⁴ Ω·cm. Production-scale dry rooms therefore maintain a dew point at or below -40°C, with oxygen below 1 ppm where lithium metal foils are handled. Solvent selection is limited to anhydrous nonpolar or weakly polar systems. N-methyl-2-pyrrolidone is excluded because polar aprotic solvents degrade the P-S network and raise interfacial impedance on the argyrodite surface. Slurry casting is replaced on multiple pilot lines by dry film extrusion through a twin-screw extruder with a screw diameter of 25–50 mm and L/D ratio between 20:1 and 36:1, followed by heated calendering. Dry pre-mixing is performed at 20–30°C to avoid sulfide particle agglomeration.

    Formulation ratios at the cathode side are adjusted to maintain a continuous ionic percolation network. A dry-basis cathode blend of LiNi0.8Mn0.1Co0.1O2, Li6PS5Cl, and vapor-grown carbon nanofiber is mixed at 70:30:2 by weight. Binder addition is held between 1 wt% and 3 wt% using hydrogenated nitrile butadiene rubber dissolved in anhydrous xylene. Excess carbon above 5 wt% interferes with grain-boundary conduction and lowers the effective lithium transference number. After coating or extrusion, the electrolyte separator is calendered at a linear pressure of 100–300 N/mm. Below 100 N/mm, residual porosity above 10% permits lithium filament penetration. Above 500 N/mm, microcracks propagate along the separator and increase cell impedance under thermal cycling.

    Cell assembly is performed with a stack pressure between 5 MPa and 150 MPa during the formation cycle. Pressure below 5 MPa results in interfacial delamination at the LiNi0.8Mn0.1Co0.1O2/Li6PS5Cl interface, detected as a rise in charge-transfer resistance above 200 Ω·cm² by electrochemical impedance spectroscopy. Pressure above 250 MPa initiates creep deformation of the sulfide layer and can reduce separator thickness below the 10 μm safety threshold. Symmetric lithium cells are used to measure critical current density for lithium penetration at 1–3 mA/cm². The terminal automotive pouch cells carry capacities between 50 Ah and 100 Ah and are validated under GB 38031-2020, ECE R100.02, and UN 38.3 test T4 altitude simulation. Process quality is controlled under IATF 16949:2016 with in-process dry room dew-point logging at 1 s intervals.

    Magnetron-sputtered LiPON thin films are deposited onto Pt/Ti/Si or stainless steel current collectors when the downstream device requires a rechargeable micro-battery with a footprint below 1 cm². The electrolyte is produced from a Li3PO4 sputtering target with purity 99.9%, using RF magnetron sputtering in a nitrogen plasma at a working pressure of 0.5–2.0 Pa. The film thickness is limited to 1–2 μm. Beyond 5 μm, residual compressive stress causes delamination and vertical cracking. The resulting ionic conductivity of 2×10⁻⁶ S/cm is lower than bulk sulfide or oxide electrolytes, but the short diffusion path in a 1 μm film keeps area-specific resistance below 50 Ω·cm². Cathode deposition proceeds by thermal evaporation or sputtering of LiCoO2, with a post-deposition anneal at 300–700°C in oxygen to restore crystallinity. Substrate temperature is held below 250°C to prevent lithium evaporation from the LiPON film. The completed thin-film cell is encapsulated with parylene and tested under IEC 62133-2:2017 and UL 1642. Terminal products include smart cards per ISO/IEC 7816-1:2011, RFID data loggers, hearables, and compact medical patches. In these formats, the electrolyte enables a cell thickness below 100 μm, which cannot be achieved with liquid electrolyte gaskets.

    Sintering Window Conflicts in LLZO-Based Implantable Cell Stacks

    For neurostimulator and pacemaker batteries, cubic LLZO with nominal composition Li7La3Zr2O12 is selected because it does not form a liquid phase and does not produce combustible vapors under crush abuse. The main process conflict arises between cathode densification and electrolyte sintering. LiCoO2 loses lithium above 900°C, while conventional LLZO air sintering requires 1100–1200°C to reach grain-boundary resistance below 100 Ω·cm². Production-scale routes therefore add Li3BO3 sintering aid at 1–3 wt% to the LLZO green body, which reduces densification temperature to 800–900°C and maintains total sintered density above 95% of theoretical. Uniaxial hot pressing at 1100°C under 20–60 MPa in a graphite die lined with boron nitride is an alternative for cathode-separator stacks that can tolerate brief lithium loss. A mother powder bed of LLZO is placed around the samples to suppress lithium volatilization, and the furnace atmosphere is dry air or flowing oxygen with water vapor below 50 ppm.

    The cathode composite is formed with LiCoO2, LLZO, and carbon at a weight ratio of 70:25:5 on a dry basis. Carbon is limited to below 3 wt% in separator-facing regions because carbon black reduces LLZO above 800°C and creates electronic leakage paths. After co-sintering, assemblies are inspected by X-ray computed tomography for delamination cracks larger than 5 μm. Assembled cells are hermetically sealed in Ti-6Al-4V enclosures by laser welding, with a helium leak rate below 1×10⁻⁸ Pa·m³/s. The terminal implantable cells deliver pulse currents of 10–100 mA for 1–10 ms and are validated under ISO 13485:2016 clause 7.5.2, ISO 14971:2019, and ISO 10993-1:2018. Published cycle-life data for LLZO/LiCoO2 implantable stacks with this exact configuration is limited, especially beyond 1000 cycles at body temperature.

    At borehole temperatures above 120°C, liquid carbonate electrolytes decompose by ester hydrolysis and solvent oxidation, whereas LATP NASICON films maintain ionic conductivity of 1×10⁻⁴ S/cm to 1×10⁻³ S/cm at 25°C. Downhole measurement-while-drilling tools use LATP solid electrolyte separators screen-printed onto alumina or quartz substrates. The slurry is prepared from Li1.3Al0.3Ti1.7(PO4)3 powder with a D50 of 1–3 μm, dispersed in a binder system of ethyl cellulose and terpineol. After screen printing through a 200–325 mesh screen, the green film is dried at 120°C and sintered in air at 800–1000°C for 2 h. Sintering below 800°C leaves porosity above 15%. Sintering above 1050°C initiates secondary-phase formation and loss of lithium phosphate. The sintered separator thickness is 20–50 μm.

    The cell design places LATP against a lithium titanate anode because direct contact with lithium metal reduces Ti4+ to Ti3+, forming an electronically conductive interface that can self-discharge the cell. The terminal battery packs are rated for continuous operation at 150°C and are qualified under MIL-STD-810H Method 501.7 high-temperature storage, RTCA DO-160G, and UN 38.3. In geothermal logging sondes, the electrolyte provides vibration tolerance under IEC 60068-2-64 without the mass penalty of liquid electrolyte containment. Capacity values for these assembled packs are typically 0.5–5 Ah, depending on the sonde power budget. Published production-scale failure data for long-term 150°C operation is limited, but interfacial impedance increases above 300°C are documented for NASICON-type separators.

    When LATP Replaces Liquid Electrolytes in Screen-Printed Sensor Nodes

    For autonomous wireless sensor nodes in industrial IoT, LATP-based solid-state cells eliminate liquid electrolyte leakage and enable direct integration with flexible printed circuit boards. The electrolyte layer is applied by screen printing under ambient humidity below 30% RH. Higher humidity causes powder agglomeration and increases screen clogging. The ink contains LATP particles with a D50 of 0.8–2 μm, ethyl cellulose binder, and terpineol at a solid-to-solvent ratio of 40:60 by weight. After printing, the wet film is dried at 120°C and sintered at 800–1000°C in air, producing a separator thickness of 10–30 μm. The sintered film has an ionic conductivity of 1×10⁻⁴ S/cm to 1×10⁻³ S/cm at 25°C, measured by electrochemical impedance spectroscopy on blocking electrodes.

    Cell assembly uses a Li4Ti5O12 anode and a LiFePO4 cathode to avoid direct LATP/lithium metal contact, because Ti4+ in LATP is reducible at potentials below 1.5 V vs Li/Li+. The terminal printed cells provide 1–10 mAh capacity for vibration sensors, cold-chain loggers, and structural health monitors. Compliance is demonstrated under RoHS 2011/65/EU Annex II, REACH 1907/2006 Article 33, IEC 60068-2-64, and ISO 9227 salt spray testing. In production, the critical control point is the co-fired cell footprint. Thermal expansion mismatch between LATP and alumina substrates above 100°C causes edge cracking if heating rates exceed 5°C/min during sintering.

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    Certification & Compliance
    More Introduction

    The solid-state electrolyte product family described in this specification comprises four product codes—SSE-LZ700, SSE-LS100, SSE-PC12, and SSE-HL350—covering garnet-type oxide, sulfide argyrodite, polymer-ceramic composite, and halide chemistries. No liquid phase is present in the as-supplied material; the products are furnished as dry powder, cast tape, or pressed pellet. Ionic conductivity values determined by electrochemical impedance spectroscopy according to ISO 16773-1:2016 range from 2.5 × 10⁻⁵ S/cm for the composite at 25 °C to 4.8 × 10⁻³ S/cm for the sulfide grade at 25 °C. Activation energies derived from Arrhenius fits between 0 °C and 80 °C lie between 0.22 eV and 0.41 eV. The oxide and sulfide grades are intended for separator layers in lithium-metal cells; the composite grade is used where flexible lamination is required; the halide grade is selected for high-voltage cathode compatibility without the hydrogen sulfide release associated with sulfides.

    Ionic Transport and Microstructural Control in Garnet-Type Separator Layers

    SSE-LZ700 is a cubic garnet powder with a nominal composition Li₆.₄La₃Zr₁.₄Ta₀.₆O₁₂ and a median particle size D50 of 0.6 µm as determined by laser diffraction. Tape-cast layers are sintered at 1150 °C for 2 h under flowing oxygen; the Archimedes density measured with anhydrous ethanol according to ISO 18754:2020 reaches 97.5% of the theoretical density. The residual porosity resides primarily at triple-grain junctions and acts as a high-resistance secondary phase. Total lithium-ion conductivity decreases from 1.1 × 10⁻³ S/cm at 25 °C to 3.9 × 10⁻⁴ S/cm at 0 °C; the corresponding activation energy is 0.31 eV. Processing above 1250 °C accelerates lithium oxide volatilization and promotes the formation of La₂Zr₂O₇, which reduces both conductivity and fracture strength. In production-scale tube furnaces, batch-to-batch variation in room-temperature conductivity has been observed to track the crucible loading density and the ramp rate through the 900–1050 °C calcination window. A ramp rate of 2 °C/min through this window, with the furnace charge limited to 40% of the hot-zone volume, is specified to keep the conductivity spread within ±0.15 log10 S/cm across 200 g batches. Calcination of the spray-dried precursor is performed in an alumina crucible with a bed depth not exceeding 20 mm. A lithium excess of 6–8 mol% is added to compensate for lithium loss during high-temperature processing. Crucible lids of platinum foil are used to suppress lithium carbonate uptake from ambient CO₂; pre-drying at 150 °C for 4 h is required if storage humidity has exceeded 60% RH. The formation of lithium carbonate at grain boundaries is detected by Raman spectroscopy at 1090 cm⁻¹ and correlates with an increase in grain-boundary resistance.

    Comparative electrochemical data for the product family are tabulated below. The values represent typical midpoints of characterization lots after the processing steps specified in the relevant product data sheet, not upper specification limits.

    Table 1. Typical electrochemical and transport properties of solid-state electrolyte product codes.
    Product codeChemistry/classIonic conductivity (S/cm)Activation energy (eV)Electrochemical stability window (V vs Li/Li⁺)Form factor
    SSE-LZ700Garnet-type oxide Li₆.₄La₃Zr₁.₄Ta₀.₆O₁₂1.1 × 10⁻³ at 25 °C0.310.0–5.0sintered tape
    SSE-LS100Sulfide argyrodite Li₆PS₅Cl4.8 × 10⁻³ at 25 °C0.220.0–4.5cold-pressed pellet/film
    SSE-PC12PEO/LiTFSI + 10 wt% LATP2.5 × 10⁻⁵ at 25 °C; 1.2 × 10⁻⁴ at 60 °C0.410.0–4.8cast film
    SSE-HL350Halide Li₃YCl₆3.0 × 10⁻⁴ at 25 °C0.400.0–4.8cold-pressed pellet/film

    Conductivity values were obtained by impedance spectroscopy with blocking electrodes under 10 MPa stack pressure for pellet and film samples. Stability windows were measured using gold-coated lithium electrodes under slow-scan voltammetry.

    What Limits Interfacial Impedance in Sulfide-Argyrodite Separator Films?

    In SSE-LS100 separator films, bulk ionic conductivity is not the limiting cell parameter. Impedance spectra of Li/SSE-LS100/Li symmetric cells recorded under 10 MPa uniaxial pressure at 25 °C exhibit two semicircles: a high-frequency feature above 1 MHz assigned to bulk transport and a lower-frequency feature between 10 Hz and 100 kHz assigned to the electrode/electrolyte interphase. The area-specific resistance of the interfacial term is 15–25 Ω·cm² for as-pressed films with 92% relative density; after 1 h of in situ pressure conditioning, this value falls to 8–12 Ω·cm². The improvement is associated with void closure at the lithium metal interface, not with bulk densification, because the bulk resistance remains unchanged during conditioning. Cold pressing at 300–500 MPa produces films with relative densities of 85–95% depending on die wall lubrication and particle size distribution. Densification above 95% is difficult without sintering because the argyrodite phase decomposes above 550 °C, releasing sulfur species and reducing ionic conductivity. For cathode-facing applications, the sulfide is blended with NMC 811 at a weight ratio of 70:30; the cathode composite is pressed onto aluminum foil at 200 MPa. In dry-room handling, the material begins to evolve H₂S when the dew point exceeds -40 °C; exposure must remain below the ACGIH TLV-TWA of 1 ppm H₂S and the STEL of 5 ppm. Processing of SSE-LS100 therefore requires enclosed powder handling, H₂S sensors calibrated to 1 ppm full-scale, and dew-point-controlled dry rooms with ISO 14644-1:2015 ISO Class 7 or better for dust control.

    Slot-Die Deposition Parameters for Flexible Composite Electrolytes

    The flexible composite grade SSE-PC12 is formulated as a slurry of poly(ethylene oxide) with a molecular weight of 600,000 g/mol, LiTFSI at an EO:Li molar ratio of 20:1, and 10 wt% LATP filler with a D50 of 0.3 µm in acetonitrile. The slurry viscosity at 25 °C is controlled between 180 mPa·s and 220 mPa·s using a cone-and-plate rheometer at 100 s⁻¹. Slot-die coating on a 300 mm wide polyethylene terephthalate release liner uses a gap of 200 µm and a line speed of 0.6 m/min. Drying under nitrogen at 60 °C for 10 min yields a dry film thickness of 50 µm ± 3 µm. Coating defects such as pinholes and edge thickening are controlled by degassing the slurry at 200 mbar for 30 min before coating and by using vacuum box extraction at the slot-die lip. Residual solvent in the dry film is below 500 ppm by headspace GC/MS. Tensile strength measured according to ASTM D638-14 Type V is 1.8 MPa at 25 °C, with an elongation at break of 120%. The lithium transference number determined by the Bruce-Vincent method at 60 °C is 0.25. This low transference number, rather than the bulk ionic conductivity, limits the practical current density of the composite to 0.1–0.2 mA/cm² in lithium symmetric cells before the onset of dendrite-induced shorting.

    Because carbonate-based liquid electrolytes have flash points between 18 °C and 31 °C, and gel electrolytes retain a flammable solvent fraction, the substitution of a solid-state separator changes both flammability classification and processing constraints. The comparison below uses a representative carbonate liquid containing 1M LiPF₆ in EC:DMC and a PVDF-HFP gel containing the same liquid at 50 wt% solvent uptake.

    Table 2. Comparative properties of solid-state separators, liquid electrolyte, and gel electrolyte.
    PropertyCarbonate liquid (EC:DMC)Gel polymer (PVDF-HFP + liquid)SSE-LS100 sulfideSSE-LZ700 oxide
    Flash point (°C)18–3125–35No flash pointNo flash point
    Ionic conductivity at 25 °C (S/cm)1.0 × 10⁻²1.0 × 10⁻³4.8 × 10⁻³1.1 × 10⁻³
    Lithium transference number0.25–0.350.30~1.00 separator transport~1.00 separator transport
    Electrochemical stability window (V vs Li/Li⁺)0–4.30–4.50–4.50–5.0
    Leakage on pouch punctureLiquid ejectionGel retentionSolid, no liquid ejectionSolid, no liquid ejection

    In liquid systems, the lithium transference number below 0.35 leads to concentration polarization at current densities above 2 mA/cm². The solid sulfide and oxide separators have transference numbers approaching unity, so concentration polarization is negligible; however, interfacial charge transfer and stack pressure become dominant. The inorganic solid-state films do not contribute to fire propagation in a vertical flame test adapted from UL 94, provided the lithium-metal anode itself is not exposed to air. Published data for this specific configuration is limited because the fully charged cell remains reactive through the lithium metal and oxygen-releasing cathode.

    When a Halide-Based Solid Electrolyte Is Substituted for a Sulfide in High-Voltage Stacks

    In high-voltage NMC 811 stacks, SSE-HL350 is selected where the cathode environment requires an oxidation stability above the sulfide threshold. The material has a nominal composition Li₃YCl₆, a room-temperature ionic conductivity of 3.0 × 10⁻⁴ S/cm, and an activation energy of 0.40 eV. In carbon-black composite electrodes scanned at 0.1 mV/s, the oxidation current remains below 10 µA/cm² up to 4.8 V vs Li/Li⁺. The electrolyte is cold-pressed at 300 MPa into dense separator films, but the relative density is typically 85–90%. Unlike sulfide argyrodite, exposure to moisture does not liberate H₂S; however, hydrolysis reactions produce HCl and metal oxychlorides, so the dry-room dew point is maintained below -20 °C. When SSE-HL350 is substituted for SSE-LS100 in a high-voltage NMC 811 composite cathode, the cathode active-material-to-electrolyte weight ratio is 70:30. Published data for this specific configuration is limited; initial impedance spectra show a cathode/electrolyte interfacial resistance below 50 Ω·cm² at 25 °C after a forming charge at 0.05 C. The substitution removes the H₂S abatement requirement but raises raw material cost and lowers separator conductivity by approximately one order of magnitude, which restricts continuous discharge rates to 0.5 C or less in ambient-temperature cells.

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