Showing 1–12 of 19 results
-
- 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
-
- 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)
-
- Strong and efficient emission at 2940 nm, ideal for water-rich tissue targeting
- Direct pumping at 980 nm or 1532 nm allows use of commercially available diode lasers
- High slope efficiency and low quantum defect, minimizing thermal load
- High thermal conductivity (~11 W/m·K) for superior heat dissipation
- Stable performance under high average and peak power operations
- High optical homogeneity and low absorption losses
- Durable mechanical properties, chemically stable in demanding environments
- Broad transparency range: 0.5 μm to 5.5 μm
-
- Wide transmission range: 350–5300 nm
- High nonlinear optical coefficients
- Excellent electro-optic properties
- Low absorption at 1064 nm and 1533 nm
- Suitable for mid-IR frequency conversion
- High laser damage threshold
- Reduced gray-tracking effect compared with KTP
- Chemically stable and non-hygroscopic
-
$1,285.00
- Single crystal KTN with composition KTa₀.₅Nb₀.₅O₃
- <001> crystallographic orientation for optimal electro-optic performance
- Size: 10 × 10 × 0.5 mm
- High electro-optic coefficient (r33 ≈ 30–50 pm/V)
- Strong photorefractive effect
- Excellent dielectric tunability
- Wide optical transparency (~350 nm – 5500 nm)
- Low defect density and high optical uniformity
-
- 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.
-
- Wide optical transparency range: 280 nm – 5.5 μm
- Excellent electro-optic and piezoelectric properties
- High Curie temperature (~605 °C)
- Outstanding pyroelectric performance for IR sensing
- Good thermal and chemical stability
- Low dielectric loss and low optical absorption
- Suitable for SAW and RF filter devices
- High resistance to optical damage compared with LiNbO₃
- Available in multiple orientations (X, Y, Z-cut)
-
- 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
-
- Ultra-wide transmission range: 0.12 – 9 μm
- Excellent UV and VUV transparency down to ~120 nm
- Low refractive index and low Fresnel reflection loss
- High laser damage threshold
- Natural birefringence suitable for polarization optics
- Excellent thermal and chemical stability
- Non-hygroscopic and moisture resistant
- Low absorption and high optical homogeneity
- Suitable for high-power laser applications
-
- High efficiency lasing at 1064 nm
- Enhanced pump absorption under broadband light (flashlamp)
- Ce³⁺ doping improves resistance to UV-induced damage
- Low thermal lensing and high optical quality
- Supports high-energy Q-switched operation
- High chemical and mechanical stability
- Long fluorescence lifetime and excellent beam quality
- Transparent from 0.25 μm to 5.0 μm
-
- Dual emission wavelengths: 1047 nm (σ polarization) and 1053 nm (π polarization)
- Naturally polarized output (birefringent crystal)
- Low thermal lensing and low quantum defect
- Longer fluorescence lifetime than Nd:YAG (~480 µs)
- Broad absorption bands suitable for diode pumping (e.g., 792 nm and 797 nm)
- High efficiency and excellent beam quality
- Suitable for high-energy pulsed and mode-locked operations
-
High-Purity Single Crystal Quartz for Optical, Piezoelectric, Electronic and Research Applications
High-quality Quartz (SiO₂) single crystals offering excellent piezoelectric properties, optical transparency, low dielectric loss, and long-term stability. Available in natural or synthetic grades, with X, Y, Z, AT, BT, SC, ST, and custom cuts. Custom sizes, shapes, and surface finishes are available for optical, acoustic, sensor, frequency-control, and research applications.
