Substrate Materials
Fused Silica
General Information
Fused Silica (SiO2) is one of the most important materials in the optical industry. For the production of high-performance optics, Fused Silica of particularly high quality is required. Synthetic materials are used instead of natural quartz sand in the production of this high-quality Fused Silica SiO2 corresponds in its chemical composition to the simplest form of glass and is its most stable modification. Fused Silica has a refractive index of 1.46 (for λ = 500 nm) and an Abbe number of 67.70. It transmits light from 180 nm to about 3 µm. Absorption bands also occur within this transmission range due to the hydroxyl groups it contains. Fused Silica with a high OH content is suitable for UV applications. For transmissive components in the wavelength range of 940 nm, 1390 nm and 2 µm - 3 µm, quartz glass with a low OH content is recommended.
Production
For the production of an amorphous (bubble- and streak-free) Fused Silica without impurities, there are different approaches that influence the final product in terms of optical specifications (see table).
Manufacturing process | OH | Cl | Cations | UV- Edge 50 % transmission | Examples for trade marks |
---|---|---|---|---|---|
Electrofusion of quartz sand or rock crystal | < 20 ppm | 0 ppm | 50 – 300 ppm | 220 nm | Infrasil® Vitreosil-IR® |
Single-stage CVD process (flame hydrolysis) using organic Si compounds | 200 – 500 ppm | 0 ppm | 10 – 50 ppm | 210 nm | Homosil® Optosil® |
Two-stage process CVD deposition and densification, use of org. Si compounds | 600 – 1200 ppm | 50 – 100 ppm | < 1 ppm | 170 nm | Corning 7980® Suprasil 1® J-Plasma SQ® |
Silicon tetrachloride in hydrogen/oxygen flame | < 20 ppm | < 200 ppm | 1 – 2 ppm | 170 nm | Suprasil 3001® |
Properties and Applications
The most important properties of Fused Silica, which are essential for LAYERTEC´s products:
- High chemical purity
- Durability
- Heat resistance
- Low coefficient of thermal expansion at high temperatures
- High softening temperature
- High transparency over a wide spectral range (UV-IR)
- High radiation resistance
In the short wavelength and visual range Fused Silica (with higher OH content, e.g. Corning 7980®) is used. Excimergrade materials are used for transmissive optics for UV high power lasers. Standard Fused Silica is of limited use for transmissive optics in the infrared range. Naturally occurring Fused Silica (e.g. Infrasil®) and specially manufactured Fused Silica (e.g. SUPRASIL 3001/3002/300®, …) have an extremely low OH content (< 20 ppm) and can therefore also be used for the infrared wavelength range to approximately 3 µm.
Calcium Fluoride
General Information
CaF2 (calcium fluoride, fluorspar, fluoride) is an optically homogeneous crystal material with a cubic structure. The refractive index of 1.43 (for λ = 500 nm) is very homogeneous, the Abbe number is 94.996. The material has a wide transmission range from 0.125 µm to 8 µm. The main application as a UV material requires high purity and crystal quality. The material is ideally suited for correcting chromatic aberration in the spectral range from VIS to NIR.
Production
While natural fluorspar has lost its importance, CaF2 is now synthesized from the purest raw materials and grown into large-volume crystals. The purity and perfection of the crystals determines the material’s possible applications.
Properties and Applications
The mechanical properties of CaF2 make machining optics a challenge. The material is very soft (Mohs hardness 4) and is therefore scratched easily. It can be easily cleaved (cleavage level 5 after {111}). Due to its high coefficient of thermal expansion, there is a risk of cracking if machined quickly or at high temperature gradients. In addition, it cannot be cemented to other materials. Uncoated polished surfaces react with atmospheric moisture and become hazy after prolonged exposure as micro-roughness increases. This creates stray light and reduces contrast.
Because of the high coefficient of thermal expansion, fluoride substrates should also be coated with fluoride layers if possible. Furthermore, heating and cooling rates must be observed to prevent cracking of the substrates.
Calcium fluoride is used at LAYERTEC for special applications in the ultraviolet range. It is processed into laser mirrors, output couplers, beam splitters, lenses, windows for excimer lasers and frequency-multiplied solid-state lasers, among others. In fluorine environment, the lifetime of CaF2 optics is significantly longer than that of other materials.
Due to the mechanical properties, it should be ensured in the application that the products are not subject to temperature fluctuations and temperature gradients. The optics should be stored with desiccant and under constant conditions. Therefore, the packaging should be opened only shortly before use.
Sapphire
General Information
The sapphire (Al2O3) is a variation of the mineral corundum. For the optical industry, the synthesized form is used. Sapphire is an anisotropic material with a rhombic-hexagonal structure and shows different optical properties depending on the crystal axis and angle of incidence. These must be taken into account for the calculation of the final products. Sapphire is transparent in the range from 180 nm to about 4 µm. The refractive index of the material is 1.77 – 1.78 (for λ = 500 nm).
Production
Various growing processes are used industrially to produce sapphire. In addition to HEM (heat exchanging method) and the Czochralski process (both growing from the melting phase), the Verneuil process (flame melting process) is also used.
Properties and Applications
The most important properties of sapphire for use as a substrate material:
- Extreme hardness (Mohs hardness 9), can only be further processed with a few materials (e.g. diamond)
- Scratch resistance
- High chemical resistance
- Very good thermal conductivity
- Wide transmission range
Due to its optimum thermal conductivity and particularly good transmission properties in the mid-infrared range, sapphire is used at LAYERTEC primarily for high-performance components in the spectral range of 2 – 3 µm.
Yttrium Aluminum Garnet
General Information
Yttrium aluminum garnet (Y3Al5O12 or YAG) is a crystal material with cubic structure, which is produced synthetically. The refractive index is 1.84 (for λ = 500 nm). It indicates good transmission behavior in the range from 0.25 µm to 4 µm. Undoped YAG is free of absorption in the range of 2 – 3 µm, whereas Fused Silica shows high absorption bands exactly here due to the higher proportion of OH groups.
Production
The YAG crystal is produced mainly by the Czochralsky method. A crystal gruel is brought into contact with the melt and then slowly moved upwards while rotating. The result is a single crystal over 300 mm in length and up to 100 mm in diameter are produced.
Properties and Applications
YAG has several properties which are advantageous for the manufacturing of high performance optics. Its chemical and mechanical resistance are similar to sapphire. However, due to its lower Mohs hardness of 8.5, YAG is easier to machine. The crystal’s high thermal conductivity and low absorption losses allow it to withstand high laser energies. The YAG crystal in doped form is also well suited for use as an active medium for lasers (Yb:YAG 1030 nm, Nd:YAG 1064 nm, Tm:YAG 2.01 µm, Ho:YAG 2.1 µm, Er:YAG 2.94 µm).
At LAYERTEC undoped YAG is used especially in the mid-infrared range (MIR) up to ≈ 4 µm. It has the advantage over sapphire that it lacks birefringence and therefore the crystal orientation can be chosen arbitrarily for many purposes. In the in-house optics production YAG substrates are manufactured in different sizes both as flat parts and as curved substrates or lenses.
Various Substrate Materials for UV, VIS and NIR/IR Optics
Fused Silica (UV) | Infrasil®1) | YAG (undoped) | Sapphire (C-cut) | CaF2 | N-BK7®2) | Si | |
---|---|---|---|---|---|---|---|
Wavelength range free of absorption | 190 nm – 2.0 μm 3) | 300 nm – 3 μm | 400 nm – 4 μm | 400 nm – 4 μm | 130 nm – 7 μm | 400 nm – 1.8 μm | 1.4 – 6 μm |
Refractive Index at | |||||||
200 nm | 1.55051 | 1.49516 | |||||
300 nm | 1.48779 | 1.45403 | |||||
500 nm | 1.46243 | 1.48799 | 1.8450 | 1.775 | 1.43648 | 1.5214 | |
1 μm | 1.45051 | 1.45042 | 1.8197 | 1.756 | 1.42888 | 1.5075 | |
3 μm | 1.41941 | 1.7855 | 1.71 | 1.41785 | 3.4381 | ||
5 μm | 1.624 | 1.39896 | 3.4273 | ||||
9 μm | 1.32677 | ||||||
Absorbing in the 3 μm region | yes | yes | no | no | no | yes | no |
Absorbing in the 940 nm region | For high power applications at 940 nm the Fused Silica types SUPRASIL 300®1) and SUPRASIL 3001/3002®1) are recommended. | ||||||
Birefringence | no | no | no | yes | no 4) | no | no |
Thermal expansion coefficient [10–6 K-1] 5) (0 – 20°C) | 0.5 | 0.5 | 7 | 5 | 18 | 7 | 2.6 |
Resistance against temperature gradients and thermal shock | high | high | high | high | low | medium | low |
GDD fs² per mm | |||||||
400 nm | 98 | 98 | 240 | 150 | 68 | 120 | |
800 nm | 36 | 36 | 97 | 58 | 28 | 45 | |
1064 nm | 16 | 16 | 61 | 29 | 17 | 22 | |
1500 nm | -22 | -22 | 13 | -25 | 1.9 | -19 | |
2000 nm | -100 | -100 | -59 | -120 | -21 | -99 | |
TOD fs3 per mm | |||||||
400 nm | 30 | 30 | 75 | 47 | 19 | 41 | |
800 nm | 27 | 27 | 57 | 42 | 16 | 32 | |
1064 nm | 44 | 44 | 71 | 65 | 21 | 49 | |
1500 nm | 130 | 130 | 140 | 180 | 46 | 140 | |
2000 nm | 450 | 450 | 360 | 530 | 120 | 460 | |
1) Registered trademark of Heraeus Quarzglas GmbH & Co. KG | |||||||
2) Registered trademark of SCHOTT AG | |||||||
3) Absorption band within this wavelength range, please see transmittance curve | |||||||
4) Measurable effects only in the VUV wavelength range | |||||||
5) Please note that different authors in the literature are inconsistent. Moreover, the thermal expansion coefficient of crystals may depend also on crystal orientation. Thus, the value given here are approximated. | |||||||
All values are for informational purposes only. LAYERTEC cannot guarantee the correctness of the values given. |
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