Transparency range: 0.35–5.5 μm, with high optical quality.
Two intense Raman shifts: 905 cm⁻¹ (E∥Nₘ) and 765 cm⁻¹ (E∥N_g), polarization-dependent, making KYW an excellent stimulated Raman scattering (SRS) crystal for frequency conversion.
Excellent acousto-optic performance: Acousto-optic figure of merit M₂ = 15 × 10⁻¹⁵ s³/kg (along N_g–30°), approximately 7 times that of quartz, with damage threshold up to 2 GW/cm² at 1064 nm (10 ns) .
High radiation resistance and thermal stability: Superior to quartz and paratellurite for high-power laser modulation in the 1–3 μm range.
Versatile rare-earth doping host: Y³⁺ sites can be substituted by Yb³⁺, Tm³⁺, Er³⁺, Ho³⁺, and other rare-earth ions, enabling a wide range of laser applications .
Good mechanical properties: Mohs hardness of 4–5, suitable for high-power operation .
Typical Specifications
Crystal structure: Monoclinic, space group C2/c (α-phase, low-temperature form); point group 2/m
Lattice parameters: a = 8.05 Å, b = 10.35 Å, c = 7.54 Å, β = 94°
Orientation: b-cut (Nₘ-axis parallel to input/output faces)
Surface quality: 10/5 Scratch/Dig
Surface flatness: λ/8 @ 632.8 nm
Parallelism: <20 arcsec
Perpendicularity: <10 arcmin
Clear aperture: >90%
Coatings: AR/AR available at 980–1080 nm
Main Applications
KYW is a primary choice for Raman shifting, with two large Raman shifts (765 and 905 cm⁻¹) enabling wavelength conversion beyond the fundamental laser output .
Acousto-optic Q-switches for 3 μm lasers: KYW-based acousto-optic shutters have been demonstrated in Er:YAG and Cr:Er:YSGG lasers, achieving 10 mJ pulses at 100 ns FWHM, with energy scaling up to 85.7 mJ in MOPA systems.
Acousto-optic modulators and deflectors: High acousto-optic figure of merit and damage threshold make KYW suitable for high-power laser modulation in the infrared and far-infrared regions.