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- Broad Transparency Window: 189 nm to 3500 nm, covering UV, visible, and near-IR
- Wide Phase-Matching Range: Supports multiple nonlinear optical processes
- High Damage Threshold: ~1 GW/cm² for 1064 nm, 10 ns pulses
- High Nonlinear Coefficients: Ensures efficient frequency conversion
- Low Birefringence Walk-Off: Enhances conversion efficiency
- Excellent Thermal and Mechanical Stability: Reliable under high-power laser operations
- Chemical Stability: Resistant to atmospheric moisture under normal use
- Customizable Phase Matching: Optimized for specific laser wavelengths and conversion processes
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- Excellent UV Transmission down to 180 nm
- High Nonlinear Coefficient for efficient frequency conversion
- Wide Phase-Matching Range for SHG, THG, and OPO applications
- High Laser Damage Threshold (> 2 GW/cm²)
- Low Absorption in UV and Visible Range
- Suitable for High-Average-Power Lasers
- Large Aperture Crystal Growth up to 20 × 20 mm available
- Ideal for Deep-UV Generation (<200 nm)
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- High Nonlinear Optical Coefficient: ~15 times that of KDP crystals.
- Broad Transparency Range: 350 nm to 4500 nm.
- High Damage Threshold: >500 MW/cm² for nanosecond pulses.
- Excellent Electro-optic Properties: Suitable for Q-switching and Pockels cells.
- Large Angular Acceptance and Low Walk-off Angle: Easier beam alignment and higher conversion efficiency.
- Stable Physical and Chemical Properties: High mechanical strength and environmental stability.
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- Wide Transparency Range: 160 nm to 2600 nm
- Broad Phase-Matching Capability: Suitable for SHG, THG, OPO, SFG, DFG across UV to IR
- High Damage Threshold: >2 GW/cm² for 1064 nm, 10 ns pulse
- Low Walk-Off Angle: Ideal for high-beam-quality laser systems
- High Nonlinear Coefficients: Enables efficient frequency conversion
- Excellent Optical Homogeneity: Δn < 10⁻⁶/cm
- Good Mechanical Hardness: Mohs hardness ~6
- Stable Physical and Chemical Properties: Resistant to humidity and environmental degradation
- Nonhygroscopic: No special humidity control required
