Transmission range extends from 110–120 nm to 7.5–8.5 μm, with >80% transmittance at 170 nm and ~60% at 121.6 nm without color-center formation .
Higher bandgap than CaF₂: Bandgap of 11.8 eV (vs. 10.0 eV for CaF₂), providing superior resistance to ArF excimer laser radiation at 193 nm .
Excellent deep-UV performance: Internal transmittance >99% at 193 nm; intrinsically low absorption and strong resistance to DUV radiation.
Superior mechanical properties: Knoop hardness of 415 kg/mm², significantly harder than CaF₂, with good thermal shock resistance and mechanical strength .
Low refractive index: n ≈ 1.38 at visible wavelengths, minimizing Fresnel reflection losses.
Birefringent and polarizing capability: Positive uniaxial crystal (nₑ > nₒ); naturally birefringent, suitable for retardation plates and polarizing elements, particularly in the 0.13–0.30 μm range .
Typical Specifications
Crystal structure: Tetragonal (rutile-type), space group P4₂/mnm (No.136); positive uniaxial
Thermal expansion coefficient: 13.7 × 10⁻⁶/°C (parallel to c-axis); 8.9 × 10⁻⁶/°C (perpendicular to c-axis)
Thermal conductivity: 0.3 W/(m·K) @ 300 K
Solubility in water: 0.0002 g/100g H₂O @ 0 °C
Laser damage threshold: >60 J/cm² @ 248 nm, 14 ns.
Main Applications
Excimer laser optics: Windows, lenses, and prisms for ArF (193 nm), KrF (248 nm), and other excimer laser systems.
UV/DUV optical components: Windows, prisms, and lenses for vacuum ultraviolet and deep ultraviolet applications, including X-ray lithography and optical filters.
Polarizing elements and waveplates: Birefringent plates, polarization rotators, and retardation plates for the 130–300 nm wavelength range.
Infrared optical elements: Windows, dome and lenses for IR spectroscopy and thermal imaging (up to 7.5–8.5 μm).