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Substrate Data. Engineering Answers.
Transmission curves, optical constants, thermal behavior, and electrical properties for every material we fabricate — the numbers your optical designer needs, on one page.
Side by Side
Eight Materials Compared
Key attributes at a glance. Refractive index quoted at 587.6 nm (nd) for visible-range materials and at the primary IR working wavelength for IR materials.
| Material | Useful Range (µm) | Index n | dn/dT (10⁻⁶/K) | Density (g/cm³) | Knoop (kgf/mm²) | CTE (10⁻⁶/K) | k (W/m·K) | Resistivity (Ω·cm) |
|---|---|---|---|---|---|---|---|---|
| ZnSe | 0.6 – 16 | 2.403 @ 10.6 µm | +61 | 5.27 | 120 | 7.1 | 18 | ~10¹² |
| ZnS (FLIR) | 0.4 – 12 | 2.192 @ 10.6 µm | +38.7 | 4.08 | ~230 | 7.6 | 16.7 | ~10¹² |
| ZnS MS / Cleartran® | 0.37 – 14 | 2.192 @ 10.6 µm | +38.7 | 4.08 | ~160 | 7.6 | 27 | ~10¹² |
| Germanium | 2 – 14 | 4.003 @ 10.6 µm | +396 | 5.33 | 780 | 6.1 | 59 | 5 – 40 |
| GaAs | 1 – 15 | 3.27 @ 10.6 µm | +149 | 5.32 | 750 | 5.7 | 52 | >10⁷ (SI) |
| Silicon | 1.2 – 7 | 3.422 @ 5 µm | +160 | 2.33 | 1150 | 2.55 | 148 | 10 – 1000 |
| Sapphire | 0.17 – 5.5 | 1.768 (nd) | +13.1 | 3.97 | 2200 | 5.3 | 27 | >10¹⁴ |
| Fused Silica | 0.18 – 2.5 | 1.458 (nd) | +11.9 | 2.20 | 500 | 0.55 | 1.38 | >10¹⁷ |
| CaF₂ | 0.13 – 10 | 1.434 (nd) | −10.6 | 3.18 | 158 | 18.85 | 9.7 | Insulator |
| Chalcogenide | 1 – 14 | 2.5–2.8 @ 10 µm* | +30 – 60* | ~4.4 – 4.7* | ~100 – 170* | ~20* | ~0.25* | High-R insulator |
* Composition-dependent (Ge-As-Se / As-Se glass systems). Data compiled from published optical materials references (Edmund Optics, Coherent/II-VI, ISP Optics, Crystran); values typical at 293 K. Confirm per-lot specifications with American Photonics engineering.
Useful Transmission Ranges
Zinc Selenide
The CO₂ laser workhorse — lowest absorption at 10.6 µm of any practical IR material.
Chemical-vapor-deposited zinc selenide is the standard transmissive material for high-power CO₂ laser systems and broadband IR imaging. Extremely low bulk absorption (<0.0005 cm⁻¹ at 10.6 µm for laser grade) minimizes thermal lensing, and its visible transmission (it's amber-transparent) makes system alignment with a visible pointer practical.
| Optical | |
|---|---|
| Useful range | 0.6 – 16 µm (transmits to ~21 µm) |
| Refractive index | 2.403 @ 10.6 µm · nd 2.403 |
| dn/dT | +61 × 10⁻⁶/K |
| Uncoated transmission | ~71% (2 surfaces, Fresnel-limited) |
| Physical & Thermal | |
| Density | 5.27 g/cm³ |
| Knoop hardness | 120 kgf/mm² (soft — handle with care) |
| Thermal conductivity | 18 W/m·K |
| Thermal expansion (CTE) | 7.1 × 10⁻⁶/K |
| Electrical & Structure | |
| Resistivity | ~10¹² Ω·cm (semi-insulating) |
| Band gap | 2.7 eV |
| Structure / growth | Polycrystalline cubic (zincblende), CVD |
Typical uncoated transmission, 2 surfaces — representative curve
Zinc Sulfide — Three Grades
Harder and tougher than ZnSe — from rugged FLIR windows to water-clear multispectral apertures.
| Attribute | CVD ZnS (FLIR Grade) | Multispectral ZnS | Cleartran® — Hellma Materials |
|---|---|---|---|
| Useful range | 0.4 – 12 µm (best 8 – 12) | 0.37 – 14 µm | 0.35 – 14 µm |
| Appearance | Translucent yellow-orange | Water-clear | Water-clear, single-crystal-like |
| Process | CVD as-deposited | CVD + HIP (hot isostatic press) | CVD + HIP — Hellma Materials brand |
| Knoop hardness | ~230 kgf/mm² | ~160 kgf/mm² | ~160 kgf/mm² |
| Thermal conductivity | 16.7 W/m·K | ~27 W/m·K | ~27 W/m·K |
| Best for | Rugged LWIR windows & domes, rain/sand erosion | Shared VIS + IR apertures | Premium common-aperture systems: visible camera + IR detector + laser through one window |
The HIP treatment removes zinc-hydride defects and normalizes the crystal structure, converting yellow FLIR-grade ZnS into a water-clear multispectral material transmitting from the visible through the LWIR. Cleartran® — produced by Hellma Materials — is the benchmark of that class, with single-crystal-like transmittance from 0.35 to 14 µm. Standard FLIR grade trades that visible clarity for higher hardness, making it the choice where erosion resistance matters more than a shared aperture.
| Common Properties (all grades) | |
|---|---|
| Refractive index | 2.192 @ 10.6 µm · nd 2.631 |
| dn/dT | +38.7 × 10⁻⁶/K |
| Density | 4.08 g/cm³ |
| Thermal expansion (CTE) | 7.6 × 10⁻⁶/K |
| Resistivity | ~10¹² Ω·cm (semi-insulating) |
| Band gap | 3.6 eV |
| Structure / growth | Polycrystalline cubic, CVD (± HIP) |
| Service limit | Avoid use above ~250 °C in normal atmosphere |
Multispectral / Cleartran® grade shown — FLIR grade cuts on near 0.4 µm with visible scatter
Germanium
The highest-index workhorse of thermal imaging — and the strategic material we reclaim domestically.
Germanium's very high refractive index (n ≈ 4.0) lets designers achieve high optical power with shallow, easy-to-manufacture curves — the reason it dominates LWIR thermal camera objectives. Its high Knoop hardness makes it rugged in the field, and DLC-coated Ge front elements survive sand, rain, and cleaning abuse. American Photonics operates a domestic Germanium reclaim program that recovers value from scrap and keeps this strategic material in the U.S. supply chain.
| Optical | |
|---|---|
| Useful range | 2 – 14 µm (transmits to ~16 µm) |
| Refractive index | 4.003 @ 10.6 µm |
| dn/dT | +396 × 10⁻⁶/K (highest of common IR materials) |
| Uncoated transmission | ~47% (2 surfaces — AR coating essential) |
| Physical & Thermal | |
| Density | 5.33 g/cm³ |
| Knoop hardness | 780 kgf/mm² |
| Thermal conductivity | 59 W/m·K |
| Thermal expansion (CTE) | 6.1 × 10⁻⁶/K |
| Electrical & Structure | |
| Resistivity (optical grade) | 5 – 40 Ω·cm |
| Band gap | 0.66 eV |
| Structure / growth | Mono- or polycrystalline, diamond cubic |
Typical uncoated transmission at 25 °C, 2 surfaces — representative curve
Gallium Arsenide
The rugged alternative for high-power CO₂ delivery in harsh industrial environments.
Semi-insulating gallium arsenide is harder and stronger than ZnSe, with better resistance to thermal shock and mechanical damage — the material of choice for CO₂ laser focusing optics in dusty, high-spatter cutting environments where a ZnSe lens would degrade. Its higher index buys thinner, stiffer lens elements at equal optical power.
| Optical | |
|---|---|
| Useful range | 1 – 15 µm (transmits to ~17 µm) |
| Refractive index | 3.27 @ 10.6 µm |
| dn/dT | +149 × 10⁻⁶/K |
| Uncoated transmission | ~55% (2 surfaces — AR coating essential) |
| Physical & Thermal | |
| Density | 5.32 g/cm³ |
| Knoop hardness | 750 kgf/mm² |
| Thermal conductivity | 52 W/m·K |
| Thermal expansion (CTE) | 5.7 × 10⁻⁶/K |
| Electrical & Structure | |
| Resistivity (semi-insulating) | >10⁷ Ω·cm |
| Band gap | 1.42 eV |
| Structure / growth | Single crystal, zincblende (LEC/VGF) |
Typical uncoated transmission, 2 surfaces — representative curve
Silicon
Lightweight, hard, thermally excellent — the cost-effective choice for MWIR.
Optical-grade silicon combines the lowest density of the IR semiconductors with the highest hardness and outstanding thermal conductivity — ideal where weight matters (airborne MWIR payloads) or where heat must be spread (laser mirrors on Si substrates). A strong lattice absorption band near 9 µm rules it out for CO₂ laser transmission, but for 3–5 µm imaging it is hard to beat on cost per performance.
| Optical | |
|---|---|
| Useful range | 1.2 – 7 µm (strong absorption near 9 µm) |
| Refractive index | 3.422 @ 5 µm |
| dn/dT | +160 × 10⁻⁶/K |
| Uncoated transmission | ~54% (2 surfaces — AR coating essential) |
| Physical & Thermal | |
| Density | 2.33 g/cm³ (lightest IR semiconductor) |
| Knoop hardness | 1150 kgf/mm² |
| Thermal conductivity | 148 W/m·K |
| Thermal expansion (CTE) | 2.55 × 10⁻⁶/K |
| Electrical & Structure | |
| Resistivity (optical grade) | 10 – 1000 Ω·cm |
| Band gap | 1.12 eV |
| Structure / growth | Single crystal, diamond cubic (CZ/FZ) |
Typical uncoated transmission, 2 surfaces — note 9 µm lattice absorption band
Sapphire
Second only to diamond in hardness — the ultimate survivable window.
Single-crystal aluminum oxide transmits from the deep UV through the MWIR while shrugging off sand erosion, high-velocity rain, chemical attack, and extreme temperature. When the window is the last line of defense — aircraft sensor apertures, missile domes, sight glasses on pressure vessels — sapphire is the default answer.
| Optical | |
|---|---|
| Useful range | 0.17 – 5.5 µm |
| Refractive index | nd 1.768 (birefringent: no−ne ≈ 0.008) |
| Abbe number | 72.2 |
| dn/dT | +13.1 × 10⁻⁶/K |
| Uncoated transmission | ~86% (2 surfaces) |
| Physical & Thermal | |
| Density | 3.97 g/cm³ |
| Knoop hardness | 2200 kgf/mm² (Mohs 9) |
| Thermal conductivity | 27 W/m·K |
| Thermal expansion (CTE) | 5.3 × 10⁻⁶/K |
| Melting point | 2040 °C |
| Electrical & Structure | |
| Resistivity | >10¹⁴ Ω·cm |
| Structure / growth | Single crystal, hexagonal (Kyropoulos/HEM/EFG) |
Typical uncoated transmission, 2 surfaces — representative curve
Fused Silica
The precision standard for UV–NIR laser optics — near-zero thermal expansion.
Synthetic amorphous silica offers the best combination of UV transmission, laser damage threshold, thermal stability, and figure retention of any common optical material. With a CTE twenty times lower than most glasses, fused silica optics hold their figure through thermal cycling — the reason interferometer references, laser windows, and 1 µm fiber-laser optics are made from it.
| Optical | |
|---|---|
| Useful range | 0.18 – 2.5 µm (IR grade to ~3.5 µm) |
| Refractive index | nd 1.458 |
| Abbe number | 67.8 |
| dn/dT | +11.9 × 10⁻⁶/K |
| Uncoated transmission | ~93% (2 surfaces) |
| Physical & Thermal | |
| Density | 2.20 g/cm³ |
| Knoop hardness | 500 kgf/mm² |
| Thermal conductivity | 1.38 W/m·K |
| Thermal expansion (CTE) | 0.55 × 10⁻⁶/K (exceptionally low) |
| Softening point | ~1600 °C |
| Electrical & Structure | |
| Resistivity | >10¹⁷ Ω·cm |
| Structure | Amorphous SiO₂, synthetic (flame hydrolysis) |
Typical uncoated transmission, 2 surfaces — OH absorption limits IR edge
Calcium Fluoride
Deep-UV to LWIR in one crystal — with famously low dispersion.
Calcium fluoride's enormous transmission window (vacuum UV at 130 nm out to ~10 µm) and very high Abbe number make it indispensable in broadband and multispectral systems, excimer laser optics, and cooled MWIR imagers. Its negative dn/dT can be exploited to passively athermalize lens assemblies.
| Optical | |
|---|---|
| Useful range | 0.13 – 10 µm |
| Refractive index | nd 1.434 |
| Abbe number | 95.1 (very low dispersion) |
| dn/dT | −10.6 × 10⁻⁶/K (negative — athermalization tool) |
| Uncoated transmission | ~94% (2 surfaces) |
| Physical & Thermal | |
| Density | 3.18 g/cm³ |
| Knoop hardness | 158 kgf/mm² (soft) |
| Thermal conductivity | 9.7 W/m·K |
| Thermal expansion (CTE) | 18.85 × 10⁻⁶/K (high — thermal shock sensitive) |
| Electrical & Structure | |
| Electrical behavior | Insulator |
| Solubility | 0.0017 g/100 g H₂O (slightly hygroscopic) |
| Structure / growth | Single crystal, cubic fluorite (Bridgman) |
Typical uncoated transmission, 2 surfaces — representative curve
Chalcogenide Glass
The moldable, athermal alternative to Germanium for volume LWIR production.
Chalcogenide glasses (Ge-As-Se and As-Se systems such as Ge₃₃As₁₂Se₅₅ and As₄₀Se₆₀) transmit across SWIR–LWIR with a dn/dT roughly an order of magnitude lower than Germanium — enabling passively athermalized thermal camera lenses. Because they are glasses, they can be precision-molded, cutting per-unit cost dramatically at volume and freeing designs from Germanium price volatility.
| Optical (composition-dependent — typical) | |
|---|---|
| Useful range | 1 – 14 µm (some compositions 0.8 – 16 µm) |
| Refractive index | 2.5 – 2.8 @ 10 µm |
| dn/dT | +30 – 60 × 10⁻⁶/K (~10× lower than Ge) |
| Uncoated transmission | ~62 – 66% (2 surfaces) |
| Physical & Thermal (typical) | |
| Density | 4.4 – 4.7 g/cm³ |
| Knoop hardness | 100 – 170 kgf/mm² |
| Thermal conductivity | ~0.25 W/m·K |
| Thermal expansion (CTE) | ~20 × 10⁻⁶/K |
| Glass transition (Tg) | ~185 °C |
| Structure | |
| Electrical behavior | High-resistivity amorphous semiconductor/insulator |
| Structure / forming | Amorphous glass — grindable, polishable, precision-moldable |
Typical uncoated transmission, 2 surfaces — composition-dependent
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