The energy storage revolution is at nanoscale and quantum materials, are the foundation.
Modern energy storage systems — Li-ion, Na-ion, supercapacitors and solid-state batteries — are being pushed to deliver higher power, faster charge rates, and longer cycle life.
Traditional electrode materials face limitations:
Slower Ion and Electron Transport: Bulk materials have long diffusion paths, limiting charge/discharge speed.
Capacity Fade Over Time: Grain boundaries, defects, and particle fracture reduce usable capacity over repeated cycles.
Thermal and Mechanical Instability: Conventional materials often degrade under high-rate operation or elevated temperatures.
Energy Density Constraints: Limited surface area reduces the number of active sites for ion storage.
RESULT: Devices struggle to meet the performance, longevity, and reliability demanded by modern applications, from EVs to grid-scale storage.
Quantum nanomaterials are engineered at the scale where atomic structure directly dictates performance. By controlling dimension, surface area, and crystallinity, these materials overcome the limitations of traditional electrodes:
Shorter ion and electron pathways → ultra-fast charge/discharge.
Enhanced reaction kinetics improve power density without sacrificing cycle life.
More active sites per unit volume → higher energy storage capacity.
Accelerates ion adsorption/desorption and electron transfer for rapid response.
Defect-free flakes, nanotubes, and nanoparticles resist degradation over thousands of cycles.
Maintains electrode integrity under mechanical stress or high-rate cycling.
Nanotubes and ultrathin flakes provide guided electron transport → efficient, high-power performance.
Reduces energy loss, heat generation, and performance drop during high-current operation.
Energy storage systems incorporating quantum nanomaterials gain measurable, real-world advantages:
FASTER CHARGING: Ideal for EVs, grid balancing, and high-power electronics.
HIGHER ENERGY DENSITY: Maximises active material utilisation within the same volume.
SUPERIOR DURABILITY: Maintains performance over thousands of cycles, reducing maintenance and warranty costs.
THERMAL STABILITY: Operates safely and efficiently at elevated temperatures or under demanding conditions.
BOTTOM LINE: Quantum nanomaterials aren’t just “nice-to-have”—they are essential for devices that need to outperform conventional limits.
THE OPPORTUNITY
OEMs and engineers integrating quantum nanomaterials into electrodes can:
Differentiate their products in speed, capacity, and longevity.
Reduce downtime, degradation, and replacement costs.
Enable next-generation applications, from ultra-fast charging EV batteries to high-capacity grid storage.
WHY NANOARC ?
NANOARC’s advanced nanomaterials are engineered at the quantum scale to deliver unmatched performance in energy storage systems. By carefully controlling dimension, structure, and surface area, our materials provide:
HIGH ENERGY DENSITY: Maximise storage capacity without increasing volume or weight.
EXCEPTIONAL DURABILITY: Grain-boundary-free and defect-free structures maintain performance over thousands of cycles.
REDUCED WEIGHT: Nanomaterials allow lighter electrodes, optimising system-level efficiency.
FAST CHARGE/DISCHARGE: Ultrafine flakes and nanotubes enable rapid ion and electron transport.
RESULT: Energy storage devices that are smaller, lighter, longer-lasting, and faster — giving OEMs a clear competitive edge.
PORTFOLIO & IMPACT
NANOARC offers a portfolio of quantum nanomaterials engineered for performance, durability, and system efficiency:
2D ZINCENE OXIDE (<1 nm)
Maximise surface area for rapid ion/electron transport and stable cycling
SUGGESTED DOSAGE: 0.5–3 wt%
APPLICATIONS: Supercapacitors, Li/Na-ion anodes
2D MAGNETENE - FexOy (<1 nm)
Defect-free, highly conductive sheets for exceptional cycle stability and fast charge/discharge
SUGGESTED DOSAGE: 0.3–2 wt%
APPLICATIONS: High-rate Li/Na-ion batteries, supercapacitors
0D TIN OXIDE - SnO₂ (~1.4 nm)
Grain-boundary-free for ultra-high capacity and long-lasting cycling
SUGGESTED DOSAGE: 1–5 wt%
APPLICATIONS: High-capacity anodes, fast-charge battery cells
1D SILICENE CARBIDE NANOTUBES (<3 nm)
Directional conductivity and mechanical resilience enable ultra-fast charge/discharge
SUGGESTED DOSAGE: 0.2–1 wt%
APPLICATIONS: High-rate batteries, flexible energy storage devices
0D ZINC OXIDE - ZnO (5 nm)
High surface area and robust stability support rapid kinetics
SUGGESTED DOSAGE: 1–4 wt%
APPLICATIONS: Li-ion/Na-ion anodes, hybrid energy storage systems
0D SILICENE CARBIDE (~8 nm)
Quantum confinement provides high-temperature stability and long cycle life
SUGGESTED DOSAGE: 0.5–2 wt%
APPLICATIONS: Solid-state batteries, high-temperature energy storage
APPLICATION SECTORS
ELECTRIC VEHICLES (EVs): Lighter, higher-energy electrodes for faster charging and longer range.
GRID-SCALE STORAGE: High-capacity, durable solutions for renewable integration and peak-shaving.
CONSUMER ELECTRONICS: Compact, high-performance cells with extended cycle life.
SUPERCAPACITORS: Ultrafast charge/discharge for energy recovery systems and hybrid devices.
ADVANCED BATTERIES: Solid-state, Na-ion, and Li-ion systems requiring thermal stability and reliability.
AEROSPACE: High-performance, lightweight energy storage for satellites, UAVs, and aviation applications where weight, reliability, and high energy density are critical.
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The Higher the surface area (BET) of the nanoparticles, the more effective the nanomaterial and the lower the required dose.
**Doses can be varied depending on the designated application and functional need.
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APPLICATIONS : Supercapacitor electrode material with energy density of ~ 877 Ah g−1
Anode nanomaterial for rechargeable Lithium ion batteries, with a high (theoretical) capacity of ~ 1320 - 2830 mAh g−1, which is higher than that of other transition metal oxides such as CoO (715 mAh g−1), NiO (718 mAh g−1) and CuO (674 mAh g−1).
In lithium-ion batteries using electrolytes like LiPF6, decomposition can produce harmful HF, which attacks the cathode. The ultra-high surface area of zincene oxide helps act as an HF scavenger, reacting with and neutralising the acid to improve overall battery stability and cycle life.
NANOARCHITECTURE : Atomically thin sheets ( < 1nm or 10 Å )
DIMENSIONS : < 10 Å thickness, up to 2 um lateral width
BAND GAP : ~ 3.5 eV
SURFACE AREA (BET) : 63520 m²/kg
COLOUR : White Powder
HEAT RESISTANCE : Up to 1975 °C (3587°F)
APPLICATIONS : Supercapacitor electrode material with energy density of ~ 650 Ah g−1
Anode nanomaterial for rechargeable Lithium ion batteries, with a high (theoretical) capacity of ~ 978 - 2096 mAh g−1, which is higher than that of other transition metal oxides such as CoO (715 mAh g−1), NiO (718 mAh g−1) and CuO (674 mAh g−1).
In lithium-ion batteries using electrolytes like LiPF6, decomposition can produce harmful HF, which attacks the cathode. The high surface area of atomically-architectured 0D-Zinc Oxide serves the purpose of an HF scavenger, reacting with and neutralising the acid to improve overall battery stability and cycle life.
NANOARCHITECTURE : ~ 5 nm ( 50 Å ) spherical nanoparticles
SURFACE AREA (BET) : 41530 m²/kg
BAND GAP : ~ 3.5 eV
COLOUR : White Nanopowder
HEAT RESISTANCE : Up to 1975 °C (3587°F)
NANOARCHITECTURE : ~ 14 Å spherical particles
SURFACE AREA (BET) : 1,486,388 cm²/g
BAND GAP : 2.5 - 3.7 eV
COLOUR : CREAM-White / White Nanopowder
HEAT RESISTANCE : Up to 1630 °C (2970°F)
APPLICATIONS : At a dimension of 1.4 nm (14 Å) this SnOx is a quantum material, at the intersection of nano- and angstrom (Å) scale technology. For perspective, a Hydrogen atom is ~ 1.1 Å (0.11 nm) in width.
It works for both sodium-ion batteries (SIBs) & lithium-ion batteries (LIBs) in energy storage systems, gaining notoriety due to its high theoretical capacities (LIB = 1494 mA h g−1 and SIB = 1378 mA h g−1).
To resist deformation and pulverisation, the nanoparticle has to be able to prohibit the formation of grain boundaries. In SnOx, this means nanoparticles below 7 nm, as at larger nanoparticle sizes, secondary grain boundaries start to emerge.
With a Bohr exciton radius of ~ 2.7 nm, these QUANTUM PARTICLES AT a diameter of ~ 1.4 nm, are well within the quantum-confinement range and heightened functionality for Tin Oxide and a robust, mechanically durable electrode with a higher resistance to pulverisation.
COLOUR : White Nanopowder
DIELECTRIC CONSTANT : 41
BOHR EXCITON RADIUS : 8.2nm
HEAT RESISTANCE : Up to 1512 °C (2754 °F)
APPLICATIONS : Advanced battery anode material for both lithium- and sodium-ion batteries, offering superior reversible capacity, demonstrating high capacity-retention even at high current rates, good rate capability and excellent cycling stability, compared to bulk Nb2O5. It enables good cyclic stability, meaning it can withstand repeated charge-discharge cycles without significant capacity loss.
In lithium-ion batteries it has a high theoretical capacity (~ 202 mAh g−1) and ability to facilitate fast lithium-ion intercalation. It enables charging speeds of 225 mAh g−1 at 200 mA g−1 across more than 400 cycles, at a Coulombic efficiency of 99.93%.
As a coating material, especially on silicon-based anode materials, it addresses volume expansion issues by helping improve structural stability and capacity. It is useful in applications requiring high power output and long lifespan.
NANOARCHITECTURE : Atomically thin sheets ( < 1nm or 10 Å )
SURFACE AREA (BET) : 495500 cm²/g
COLOUR : Black/Blackish-Brown powder
HEAT RESISTANCE : Up to 1597 °C (2907 °F)
APPLICATIONS : High surface area 2d-material applied as an anode material in lithium ion cells. It provides an outstanding electrochemical performance with a high lithium storage capacity, cyclability, and an excellent high rate capacity. In particular, it provides good tolerance towards charge and discharge at high current densities.
NANOARCHITECTURE : Nanospheres
DIMENSIONS : ~ 8 nm ( 80 Å ) diameter
ENERGY GAP : ~ 1.8 eV (tunable)
COLOUR : Bluish-Black/Midnight Blue Nanopowder
HEAT RESISTANCE : Up to 2830 °C (5130°F)
APPLICATIONS : Anode material enabling shortened transport lengths and resistance to degradation. The voltage profile is defined as a function of the concentration of Li adsorbed on the silicene carbide nanospheres.
QUANTITY | PRICE
50 grams (1.76 oz.) | $ 22,050
500 grams (17.6 oz.) | $ 219,000
1kg (2.2 lb) | $ 432,000
BULK ORDER RATES : From 1 Tonne | CONTACT trade@nanoarc.org
NANOARCHITECTURE : Tubular
DIMENSIONS : < 3 nm ( 30 Å ) diameter, up to 10 µm in length
COLOUR : Whitish Grey Nanopowder
ENERGY GAP : ~ 2.1 - 3.0 eV (direct and tunable)
BOHR EXCITON RADIUS : ~ 2.7 nm
HEAT RESISTANCE : Up to 2830 °C (5130°F)
APPLICATIONS : Anode material enabling shortened transport lengths and resistance to degradation. In lithium ion batteries, lithium-ions can be stored on the exterior surface as well as the interstitial sites between the SixC nanotubes and on the nanotube interiors. The voltage profile is defined as a function of the concentration of Li adsorbed on the silicene carbide nanotubes.
QUANTITY | PRICE
50 grams (1.76 oz.) | $ 24,500
500 grams (17.6 oz.) | $ 244,000
1 kg (2.2 lb) | $ 488,000
BULK ORDER RATES : From 1 Tonne | CONTACT trade@nanoarc.org