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50mm – 200mm Diameter Range
IR Trans. 2–14μm Transmission Window
μₑ = 3900 cm²/V·s Electron Mobility
CZ / VGF Growth Crystal Growth
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High-Purity Single-Crystal Germanium Substrates

Germanium (Ge) is a Group IV indirect-bandgap semiconductor (0.66 eV) that occupies a unique position between silicon and III-V compound semiconductors. With an electron mobility of 3,900 cm²/V·s — nearly three times that of silicon — and broadband infrared transparency from 2μm to 14μm, germanium substrates enable critical applications that silicon alone cannot address: long-wave infrared (LWIR) optics, high-efficiency multi-junction space photovoltaics, ultra-high-speed SiGe heterojunction bipolar transistors, and gamma-ray spectroscopy detectors.

The germanium wafer market has experienced sustained growth driven by the expansion of thermal imaging systems (automotive ADAS, industrial inspection, defense), the deployment of low-earth-orbit (LEO) satellite constellations demanding radiation-hard multi-junction solar cells, and the proliferation of millimeter-wave 5G/6G infrastructure requiring SiGe BiCMOS technology. Ge substrates are produced in diameters from 50mm to 200mm using Czochralski (CZ) and Vertical Gradient Freeze (VGF) growth methods, with 5N+ (99.999%) purity levels as the standard for optical and electronic grades.

At GINECHIP, we supply single-crystal germanium wafers in N-type (Sb-doped), P-type (Ga-doped), and intrinsic (undoped) grades across all standard diameters. Every lot includes a full Certificate of Analysis (CoA) documenting resistivity, Hall mobility, EPD, IR transmission spectra, surface roughness, and dimensional metrology. Epi-ready surface finish (RMS < 2Å), custom off-cut orientations, and AR/AR coating services are available on request.

Crystal Growth: Czochralski & Vertical Gradient Freeze

Two primary methods are employed for the production of device-grade single-crystal germanium ingots, each offering distinct advantages for specific application requirements.

Czochralski (CZ) Growth

The Czochralski method is the most widely used technique for germanium crystal growth at production scale. High-purity germanium feedstock (5N+) is melted in a graphite or quartz crucible under a controlled atmosphere (typically H₂ or Ar). A precisely oriented single-crystal seed is dipped into the melt and slowly withdrawn while rotating, producing dislocation-free or low-EPD ingots up to 200mm diameter. CZ germanium achieves resistivities from 0.01 Ω·cm (heavily doped N-type for optoelectronics) to > 40 Ω·cm (intrinsic for IR optics). The method provides excellent diameter control, high throughput, and cost efficiency for volume production.

Vertical Gradient Freeze (VGF) Growth

In VGF growth, the germanium charge and seed crystal are contained within a sealed ampoule, and crystallization proceeds by precisely controlling a temperature gradient as the entire assembly is cooled through the melting point. The absence of melt convection and the controlled axial gradient produce crystals with exceptionally low dislocation densities (EPD < 500/cm² achievable) and superior dopant uniformity compared to CZ. VGF is preferred for the highest-quality IR optics and for intrinsic germanium used in radiation detector fabrication, where crystallographic perfection directly impacts detector energy resolution.

Infrared Optics & Thermal Imaging

Germanium is the dominant material for long-wave infrared (LWIR, 8–14μm) optical components due to its unique combination of broad IR transparency, high refractive index (n ≈ 4.0), and excellent mechanical properties. Unlike ZnSe, ZnS, and chalcogenide glasses, germanium does not exhibit significant multiphonon absorption in the 8–12μm atmospheric window, enabling high-transmission optical systems without cryogenic cooling.

Key IR optical applications include:

  • FLIR & Thermal Imaging: Germanium lenses and windows for uncooled microbolometer arrays (VOx, a-Si) in automotive night vision, industrial thermography, predictive maintenance, and building diagnostics.
  • CO₂ Laser Systems: Output couplers, beam expanders, and focusing lenses for industrial CO₂ lasers (10.6μm) used in cutting, welding, marking, and medical surgery. Ge's low absorption coefficient (< 0.02 cm⁻¹ at 10.6μm) minimizes thermal lensing at multi-kilowatt power levels.
  • Military & Defense Optics: Armored windows, missile seeker domes, and targeting pod optics operating in MWIR (3–5μm) and LWIR bands with diamond-like carbon (DLC) anti-reflective and protective coatings.
  • Spectroscopy: ATR (attenuated total reflection) crystals for FTIR chemical analysis and Ge etalons for wavelength calibration in tunable laser spectroscopy.

Optical Transmission Characteristics

Wavelength RangeTransmission (uncoated, 1mm thick)Application Band
2.0 – 3.0 μm~47% (two-surface reflection limited)MWIR short edge
3.0 – 5.0 μm~47% (intrinsic transparency)MWIR atmospheric window
8.0 – 12.0 μm~47% (intrinsic transparency)LWIR atmospheric window
10.6 μm~47% (CO₂ laser line)Industrial laser optics
12.0 – 14.0 μm> 40% (multiphonon edge begins)Extended LWIR

Note: All values are for uncoated germanium. With broadband anti-reflection (BBAR) coatings optimized for 8–12μm, transmission exceeds 95%. Diamond-like carbon (DLC) hard coatings provide environmental durability for external surfaces.

Multi-Junction Solar Cells for Space Photovoltaics

Germanium substrates form the foundation of state-of-the-art triple-junction (3J) and four-junction (4J) solar cells used in space power systems. In the standard GaInP/GaAs/Ge architecture, the germanium substrate serves a dual role: mechanical support for epitaxial III-V layers and an active bottom subcell that converts photons with energies between the GaAs bandgap (1.42 eV) and the Ge bandgap (0.66 eV) — corresponding to wavelengths from 870nm to 1880nm.

The Ge bottom junction contributes approximately 200–250 mV to the total open-circuit voltage and generates 6–10 mA/cm² of photocurrent under AM0 (air mass zero, space) illumination. Modern 3J cells on Ge achieve AM0 efficiencies exceeding 30% (beginning-of-life) with excellent radiation resistance due to the inherent defect tolerance of the germanium lattice. For LEO constellations and GEO communications satellites, Ge-based multi-junction cells provide the highest specific power (W/kg) and power density (W/m²) of any flight-proven photovoltaic technology.

GINECHIP supplies germanium substrates optimized for MOCVD epitaxial growth of III-V solar cell structures, with epi-ready surface finish (RMS < 2Å), controlled off-cut orientation ((100) 6° toward (111) for step-bunching suppression), and tight resistivity specifications (0.01–0.04 Ω·cm, N-type) required for low series resistance in the Ge bottom cell.

High-Speed SiGe Electronics

Silicon-germanium (SiGe) heterojunction bipolar transistor (HBT) technology leverages the narrower bandgap and higher carrier mobility of germanium relative to silicon to achieve RF performance that rivals III-V (GaAs, InP) technologies while maintaining CMOS integration compatibility. Modern SiGe BiCMOS processes use epitaxially grown SiGe base layers on silicon substrates, but direct germanium and germanium-on-insulator (GeOI) substrates are increasingly important for advanced nodes requiring higher mobility channels.

Key specifications for Ge substrates used in SiGe epitaxy include: (100) orientation with precise off-cut control, ultra-low surface roughness (< 2Å RMS), low EPD (< 5×10³/cm²) to prevent threading dislocation propagation into epitaxial layers, and controlled resistivity for RF substrate isolation. SiGe HBTs fabricated on optimized Ge substrates achieve fT > 300 GHz and fmax > 500 GHz, enabling 77 GHz automotive radar transceivers, 60 GHz WiGig (802.11ad/ay) radios, 100G/400G optical modulator drivers, and THz imaging arrays for security screening.

Radiation Detectors & X-Ray Optics

High-purity germanium (HPGe) represents the pinnacle of gamma-ray spectrometry, providing energy resolution of < 0.1% at 1.33 MeV (⁶⁰Co) — an order of magnitude superior to scintillation detectors (NaI, LaBr₃) and unmatched by any other solid-state detector technology. HPGe detectors operate at liquid nitrogen temperatures (77K) to minimize thermally generated leakage current in the narrow-bandgap (0.66 eV) material, and are fabricated from intrinsic germanium crystals with net impurity concentrations below 10¹⁰ cm⁻³.

Applications span nuclear safeguards and non-proliferation monitoring, environmental radioactivity analysis, neutron activation analysis for materials science, astrophysical gamma-ray spectroscopy, and medical PET/SPECT calibration. GINECHIP supplies intrinsic-grade germanium wafers with resistivity > 40 Ω·cm as starting material for detector-grade crystal growth and planar detector fabrication.

Technical Specifications

ParameterAvailable Range / Values
Material Single-crystal Germanium (Ge), 5N+ purity
Diameter 50mm, 100mm, 150mm, 200mm
Dopant / Type N-type (Sb-doped), P-type (Ga-doped), Intrinsic (undoped)
Resistivity N-type: 0.01–40 Ω·cm, P-type: 0.01–30 Ω·cm, Intrinsic: > 40 Ω·cm
Orientation (100), (111), (110), off-cut ±0.5°
Thickness 200μm–1000μm, standard SEMI thicknesses
Surface Polish SSP, DSP, Epi-Ready, RMS < 2Å
EPD (Etch Pit Density) < 5×10³/cm²
TTV / Bow / Warp TTV < 5μm, Bow < 15μm, Warp < 20μm
Bandgap 0.66 eV (indirect)
Electron Mobility 3,900 cm²/V·s
Hole Mobility 1,900 cm²/V·s
IR Transmission Range 2–14μm, n ≈ 4.0
Refractive Index 4.003 @ 10.6μm (CO₂ laser wavelength)
Thermal Conductivity 60 W/m·K
Density 5.323 g/cm³
Packaging Vacuum-sealed, single-wafer shippers, Class 100

Applications & Market Segments

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Infrared Optics & Thermal Imaging

Germanium's broad transparency from 2μm to 14μm and high refractive index (n ≈ 4.0) make it the premier material for IR lenses, windows, and beamsplitters in FLIR systems, thermal imaging cameras, and forward-looking infrared (FLIR) military and industrial systems. AR/AR coatings (DLC, BBAR) are applied for 8–12μm LWIR atmospheric window performance.

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Multi-Junction Space Solar Cells

Germanium serves as the bottom subcell substrate in GaInP/GaAs/Ge triple-junction photovoltaic devices, achieving conversion efficiencies exceeding 30% under AM0 illumination. The Ge bottom junction absorbs photons from 900–1800nm, making it essential for satellite power systems where specific power (W/kg) and radiation hardness are critical design parameters.

High-Speed SiGe Electronics

SiGe heterojunction bipolar transistors (HBTs) on Ge or SiGe virtual substrates deliver fT > 300 GHz and fmax > 500 GHz for millimeter-wave communications (5G/6G, E-band backhaul, 77 GHz automotive radar), high-speed optical networking (100G/400G transceivers), and THz imaging circuits.

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Radiation Detectors & X-Ray Optics

High-purity germanium (HPGe) detectors provide the gold standard for gamma-ray spectroscopy with energy resolution < 0.1% at 1.33 MeV (⁶⁰Co), used in nuclear physics, homeland security, and environmental monitoring. Ge crystal monochromators are deployed at synchrotron beamlines for hard X-ray diffraction and scattering experiments.

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CO₂ Laser Optics

Germanium's exceptionally low absorption at 10.6μm (absorption coefficient < 0.02 cm⁻¹) and high thermal conductivity (60 W/m·K) make it the material of choice for CO₂ laser output couplers, beam expanders, and focusing lenses in industrial laser cutting, welding, and marking systems up to multi-kilowatt power levels.

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Research & Semiconductor Metrology

Ge substrates are used as ATR (attenuated total reflection) crystals for FTIR spectroscopy, as calibration standards for ellipsometry, and as substrates for epitaxial growth of III-V materials (GaAs/Ge virtual substrates) in research environments. Intrinsic Ge wafers serve as FIR/THz beam splitters for FTIR interferometers.

Metrology & Quality Assurance

Every germanium wafer lot undergoes comprehensive metrology at ISO 9001:2015 certified facilities. A full Certificate of Analysis (CoA) including FTIR transmission spectra, resistivity maps, Hall data, XRD rocking curves, AFM surface roughness, EPD counts, and dimensional metrology is provided with each shipment.

FTIR Transmission Spectroscopy Full-spectrum IR transmission measurement from 2μm to 14μm using FTIR spectrophotometer. Transmission > 45% at 10.6μm for AR-coated Ge windows certified per ISO 15368. Absorption coefficient mapping across the wafer surface.
Four-Point Probe Resistivity Mapping 25-point or 49-point DC resistivity mapping per ASTM F43. Radial uniformity < ±5% for device-grade substrates. Separate protocols for N-type, P-type, and intrinsic material verification.
Hall Effect Measurement Van der Pauw geometry Hall measurement at 300K and 77K for carrier concentration, mobility, and conductivity type verification. Electron mobility > 3,500 cm²/V·s and hole mobility > 1,700 cm²/V·s guaranteed for prime-grade material.
X-Ray Diffraction (XRD) High-resolution XRD rocking curve measurement of the (004) reflection for crystallinity assessment. FWHM < 25 arcsec for device-grade substrates. Orientation verification to ±0.1° using Bond method.
AFM Surface Roughness Atomic force microscopy over 1×1μm and 10×10μm scan areas. Epi-ready surface certified at RMS < 2Å. Step-terrace structure visualization for off-cut wafers.
Etch Pit Density (EPD) Preferential chemical etching (CP4 or similar) followed by Nomarski optical microscopy for dislocation density quantification. EPD < 5×10³/cm² standard; < 1×10³/cm² for IR optics grade.
TTV / Bow / Warp Interferometry Full-wafer topography via grazing-incidence interferometry. TTV < 5μm, Bow < 15μm, Warp < 20μm standard. Custom flatness specifications available for epi-ready and bonding applications.
Laser Particle Scan Surface particle inspection per SEMI M53 equivalent. Class 100 cleanroom packaging with vacuum-sealed single-wafer shippers. Particle adders < 10 at 0.3μm.

Need Germanium Substrates for Your Application?

Specify your diameter, dopant type (N-type / P-type / intrinsic), resistivity range, orientation, surface finish, and quantity — our substrate specialists will provide a detailed quotation with metrology data and lead time within 24 hours.

ISO 9001:2015 5N+ Purity Epi-Ready Surface RoHS / REACH