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2″ – 8″ Diameter Diameter Range
C-plane (0001) Orientation
GaN Epi 2–8μm Epi Thickness
DD < 5×10⁸/cm² Dislocation Density
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Gallium Nitride on Sapphire (GaN-on-Sapphire) Substrates

Gallium Nitride on Sapphire (GaN-on-Sapphire) is the foundational epitaxial substrate platform for the global solid-state lighting industry and is rapidly expanding into power electronics and RF applications. GaN's wide direct bandgap of 3.4 eV, high critical electric field (3.3 MV/cm), and the spontaneous formation of a high-mobility two-dimensional electron gas (2DEG) at AlGaN/GaN heterointerfaces make it the most versatile wide-bandgap semiconductor commercially available.

Because bulk GaN substrates remain expensive and limited in diameter, heteroepitaxial growth on sapphire (α-Al₂O₃) has become the dominant commercial approach. Sapphire offers a hexagonal crystal structure compatible with wurtzite GaN, outstanding thermal and chemical stability at MOCVD growth temperatures (1,000–1,100°C), transparency across the visible and near-UV spectrum (critical for LED light extraction), and availability in large diameters up to 8″ at moderate cost. The 16% lattice mismatch is managed through optimized low-temperature buffer layers (AlN or GaN) that nucleate high-quality GaN growth.

The GaN-on-Sapphire substrate market exceeds USD 800 million annually, driven primarily by LED production (over 100 billion die per year), with power electronics and RF representing the fastest-growing segments. The transition from 4″ to 6″ and 8″ sapphire substrates in LED fabs has driven a 3× reduction in cost per lumen over the past decade, making LED lighting the dominant illumination technology worldwide.

At GINECHIP, we supply GaN-on-Sapphire epitaxial substrates in UID, N-type Si-doped, and P-type Mg-doped variants from 2″ to 8″ diameters. Standard GaN epi thicknesses from 2μm to 8μm, with AlN buffer layer included in all templates. Premium-grade substrates with XRD (0002) FWHM below 200 arcsec and dislocation density below 1×10⁸/cm² are available for laser diode and high-reliability applications.

Epitaxial Growth Methods

Three distinct epitaxial growth approaches deliver GaN-on-Sapphire substrates, each optimized for different defect density, thickness, and cost requirements. MOCVD dominates volume production, while HVPE and ELOG serve high-value specialty applications.

Industry Standard

MOCVD on Sapphire

TMGa + NH₃ precursors — highest throughput

Diameter 2″ – 8″
Thickness Uniformity ±5%
Dislocation Density < 5×10⁸/cm²
Throughput High (production)

Metal-Organic Chemical Vapor Deposition (MOCVD) is the dominant production method for GaN-on-Sapphire epitaxial substrates. Trimethylgallium (TMGa) and ammonia (NH₃) precursors are introduced into a heated reactor (1,000–1,100°C) where they pyrolyze and deposit GaN onto a C-plane sapphire wafer. A thin AlN or low-temperature GaN buffer layer nucleates the growth, managing the 16% lattice mismatch between GaN and sapphire. MOCVD enables precise thickness control (±5%), uniform doping, and high throughput for 2″ through 8″ wafers. This is the standard template for blue/green LED production worldwide.

Thick Layers

HVPE Templates

GaCl + NH₃ chemistry — thick layers

Diameter 2″ – 4″ (typical)
Growth Rate 50–200 μm/hr
Dislocation Density < 1×10⁷/cm²
Throughput Low (specialty)

Hydride Vapor Phase Epitaxy (HVPE) uses GaCl (formed by HCl gas flowing over liquid gallium) and NH₃ to deposit GaN at growth rates exceeding 100μm/hour — over 50× faster than MOCVD. HVPE is primarily used to grow thick (10–300μm) GaN layers that serve as quasi-bulk templates. These templates are subsequently separated from the sapphire substrate via laser lift-off or chemical etching to create free-standing GaN wafers, or kept as low-defect-density templates for high-voltage vertical power devices where thick drift layers are required.

Lowest Defect

ELOG (Epitaxial Lateral Overgrowth)

Patterned mask regrowth — lowest defect density

Diameter 2″ – 4″
Dislocation Density < 5×10⁶/cm²
Process Complexity High (multi-step)
Throughput Low (laser-grade)

Epitaxial Lateral Overgrowth (ELOG) is a defect-reduction technique where a patterned dielectric mask (SiO₂ or SiNₓ) is deposited on a GaN template layer. During subsequent MOCVD regrowth, GaN nucleates selectively in mask openings and then grows laterally over the mask, bending and annihilating threading dislocations. The regions above the mask achieve dislocation densities below 5×10⁶/cm² — two orders of magnitude improvement over standard MOCVD GaN. ELOG substrates are essential for laser diodes where dislocation density directly determines device lifetime and threshold current density.

Growth Method Comparison: MOCVD vs HVPE vs ELOG

The choice between MOCVD, HVPE, and ELOG depends on the target device's defect tolerance, required GaN thickness, and economics. The table below summarizes key differentiating factors.

HVPE Templates

Ultra-fast growth (50–200 μm/hr) producing thick GaN layers for quasi-bulk templates. Dislocation density below 1×10⁷/cm² — one order of magnitude better than MOCVD. Used for vertical power devices requiring thick drift layers and as precursors for free-standing GaN substrates after sapphire removal.

Best for: Vertical Power, FS-GaN DD: < 1×10⁷/cm²

ELOG Regrowth

Patterned mask and lateral overgrowth reducing dislocation density to < 5×10⁶/cm² — two orders of magnitude below standard MOCVD. Essential for laser diodes where dislocation density directly correlates with device lifetime. Multi-step process with higher cost; reserved for premium applications.

Best for: Laser Diodes DD: < 5×10⁶/cm²

Wide Bandgap Material Property Comparison

GaN's material properties place it at the intersection of high-frequency (GaAs domain) and high-power (SiC domain) performance. The table below compares key semiconductor figures of merit — Johnson (JFOM) for RF power capability and Baliga (BFOM) for DC-DC converter efficiency — across the four most important semiconductor materials in modern electronics.

PropertyGaNSilicon (Si)GaAs4H-SiC
Bandgap (eV) 3.4 (direct) 1.12 (indirect) 1.42 (direct) 3.26 (indirect)
Critical Field (MV/cm) 3.3 0.3 0.4 2.8
Electron Mobility (cm²/V·s) 2,000 (2DEG) 1,350 8,500 900
Saturation Velocity (10⁷ cm/s) 2.5 1.0 1.2 2.0
Thermal Conductivity (W/m·K) 130 (bulk) / 250 (SiC) 150 55 490
Max Operating Temp (°C) > 500 150 200 > 600
JFOM (Johnson Figure of Merit) 760 1 3 280
BFOM (Baliga FOM, relative) 650 1 15 130

Power Electronics: GaN HEMT Revolution

AlGaN/GaN HEMTs represent the most disruptive wide-bandgap device technology in power electronics. The spontaneous and piezoelectric polarization fields at the AlGaN/GaN heterointerface induce a 2DEG with sheet carrier concentrations exceeding 1×10¹³/cm² and electron mobility above 2,000 cm²/V·s — without the need for impurity doping. This creates a normally-on (depletion-mode) channel with exceptionally low sheet resistance (300–800 Ω/sq).

GaN power HEMTs achieve breakdown voltages from 100V to 1,200V with specific on-resistance (RDS(on)·A) 5–10× lower than the silicon theoretical limit. A 650V GaN HEMT in a 5×6mm PQFN package replaces a silicon super-junction MOSFET in a 10×12mm package while reducing gate charge (Qg) by 80% and output capacitance (Coss) by 70% — enabling hard-switching converters at 1 MHz+ with efficiencies exceeding 98%. This is transformative for USB-C fast chargers (65W in a 30cm³ volume), telecom rectifiers (3kW in 1U), and EV traction inverters where GaN is projected to reduce inverter losses by 50% compared to Si IGBTs.

GINECHIP offers AlGaN/GaN HEMT epiwafers on 6″ and 8″ sapphire with specified 2DEG sheet resistance (300–500 Ω/sq), carrier concentration (> 8×10¹²/cm²), and mobility (> 1,800 cm²/V·s). AlN interlayers and carbon-doping for dynamic RDS(on) suppression are available for power-switching applications.

Technical Specifications

ParameterAvailable Range / Values
Base Substrate C-plane sapphire (0001), 430μm or 650μm thickness
GaN Epi Thickness 2μm, 3.5μm, 5μm, 8μm (custom on request)
Doping Options UID (unintentionally doped), N-type Si-doped, P-type Mg-doped
Dislocation Density < 5×10⁸/cm² (typical); < 1×10⁸/cm² (premium grade)
Sheet Resistance N-type: 300–800 Ω/sq; UID: > 10⁶ Ω/sq
Surface Roughness Ra < 0.5nm (AFM 5×5μm scan)
Wafer Bow ≤ 40μm (4″); ≤ 80μm (6″); ≤ 120μm (8″)
Available Diameters 2″ (50.8mm), 4″ (100mm), 6″ (150mm), 8″ (200mm)
AlN Buffer Layer 20–30nm, included in all standard templates
XRD FWHM (0002) < 300 arcsec (typical); < 200 arcsec (premium)
XRD FWHM (10-12) < 500 arcsec (typical); < 350 arcsec (premium)
GaN Bandgap 3.4 eV (direct, wurtzite crystal structure)
Sapphire Thermal Expansion 7.5×10⁻⁶/K (a-axis); 8.5×10⁻⁶/K (c-axis) at 300K
Sapphire Refractive Index nₒ = 1.768, nₑ = 1.760 at 633nm
Backside Finish As-cut, lapped, or polished per customer specification
Laser Mark SEMI M12/M13 compliant: soft-mark on front or back side
Particle Count @ 0.3μm ≤ 20 particles (laser surface scan)
Packaging Vacuum-sealed single-wafer containers, Class 100 cleanroom
Compliance SEMI Standards, RoHS, REACH

Applications & Market Segments

💡

Blue, Green & UV LEDs

GaN-on-Sapphire is the universal platform for InGaN/GaN multiple-quantum-well (MQW) LEDs spanning 365nm (UVA) to 550nm (green). The technology powers solid-state lighting, automotive headlamps, full-color displays (microLED), and UV-C sterilization. Over 100 billion GaN LEDs are produced annually on sapphire substrates — making this the highest-volume compound semiconductor application by unit count.

GaN Power HEMTs

AlGaN/GaN high-electron-mobility transistors (HEMTs) on silicon or sapphire substrates leverage the spontaneous and piezoelectric polarization-induced 2DEG (two-dimensional electron gas) with sheet carrier densities exceeding 1×10¹³/cm². GaN HEMTs achieve breakdown voltages above 650V with RDS(on) below 50mΩ, enabling compact, high-efficiency power supplies, EV onboard chargers, and data center PSUs that outperform silicon super-junction MOSFETs.

🔬

Laser Diodes (LDs)

GaN-based edge-emitting laser diodes operating at 405nm (violet/Blu-ray), 450nm (blue), and 520nm (green) require ELOG-quality substrates with dislocation density below 5×10⁶/cm². Applications include laser projection (pico-projectors, AR/VR waveguide displays), automotive LiDAR (scanning MEMS-mirror systems), and high-brightness laser lighting for stadium and architectural illumination.

📡

GaN RF Transistors

GaN-on-SiC and GaN-on-Si HEMTs dominate the RF power amplifier market above 3 GHz for 5G base stations, radar, and electronic warfare. With power densities exceeding 8 W/mm at 30 GHz (compared to ~1 W/mm for GaAs), GaN enables higher output power from smaller die areas, reducing system cost and thermal management complexity in phased-array antenna elements.

🧪

UV Photodetectors

GaN and AlGaN-based metal-semiconductor-metal (MSM) and Schottky photodiodes provide solar-blind UV detection (200–365nm) with visible rejection ratios exceeding 10⁴. These detectors are essential for flame sensing, missile plume detection, and UV-C disinfection monitoring where immunity to ambient visible light is critical.

🛰️

Space & Harsh Environment

GaN's wide bandgap (3.4 eV) provides inherent radiation hardness — displacement damage thresholds 10–100× higher than silicon. Combined with operating temperatures exceeding 500°C, GaN devices are qualified for satellite power systems, deep-space probes, and downhole geothermal instrumentation where silicon electronics cannot survive.

Metrology & Quality Assurance

Every GaN-on-Sapphire wafer lot is characterized through a comprehensive metrology protocol at ISO 9001:2015 certified facilities. The combination of XRD, PL mapping, AFM, and Hall effect measurements provides a complete picture of crystalline quality, optical uniformity, surface morphology, and electrical transport properties.

High-Resolution XRD Rocking Curve ω-scan of (0002) and (10-12) reflections to quantify threading dislocation density. FWHM < 300 arcsec (0002) and < 500 arcsec (10-12) for standard grade; < 200 and < 350 arcsec for premium. Screw and edge dislocation densities derived from Williamson-Hall analysis.
AFM Surface Roughness Atomic force microscopy over 5×5μm and 20×20μm scan areas. Standard specification: Ra < 0.5nm. Step-terrace morphology confirms step-flow growth mode and absence of 3D islanding. Data included in Certificate of Analysis.
Contactless Sheet Resistance Mapping Lehighton eddy-current or equivalent non-contact Rs mapping with 1mm spatial resolution across full wafer. Confirms doping uniformity ±8% for N-type GaN and verifies UID layer resistivity > 10⁶ Ω/sq.
Photoluminescence (PL) Mapping Room-temperature PL intensity and peak-wavelength mapping at 365nm excitation. Confirms band-edge emission uniformity, identifies yellow luminescence defect bands, and maps InGaN composition uniformity for LED epiwafers.
Wafer Bow / Warp Interferometry Full-wafer topography measurement via grazing-incidence interferometry. Bow ≤ 40μm (4″), ≤ 80μm (6″), ≤ 120μm (8″). Critical parameter — excessive bow causes photolithography focus errors and non-uniform epi-layer growth.
SEM / TEM Cross-Section Scanning and transmission electron microscopy of GaN/sapphire interface, AlN buffer layer integrity, and threading dislocation propagation. Included for process qualification and new product introduction lots.
Hall Effect Measurement Van der Pauw geometry at 300K and 77K for sheet carrier concentration, mobility, and sheet resistance of the 2DEG channel in AlGaN/GaN HEMT structures. Confirms 2DEG density > 8×10¹²/cm² for power HEMT templates.
Ellipsometry / Reflectometry Spectroscopic ellipsometry for GaN epi-layer thickness, AlN buffer thickness, and refractive index dispersion (n and k from 250nm to 1,700nm). Thickness accuracy ±2% with 49-point wafer map.

Need GaN-on-Sapphire Substrates?

Specify your diameter (2″–8″), GaN thickness, doping type (UID/N-type/P-type), and dislocation density grade — our wide-bandgap specialists will provide a detailed quotation with XRD, AFM, and PL mapping data within 24 hours.

ISO 9001:2015 SEMI Standards RoHS / REACH LED / HEMT Grade