双折射晶体
α-BBO晶体
High temperature phase of BaB2O4 is an excellent birefringent crystal; it is characterized by large birefringent coefficient and wide transmission window from 189nm to 3500nm, particularly it is suita..
High temperature phase of BaB2O4 is an excellent birefringent crystal; it is characterized by large birefringent coefficient and wide transmission window from 189nm to 3500nm, particularly it is suitable to make the high power UV polarizer, due to its unique UV transparency and good mechanical properties. The physical, chemical, thermal and optical properties of β-BBO crystals are similar to those of α-BBO, for instant high optical homogeneity (better than 1x10-6/cm), extremely low absorption in the UV to IR range (<0.5% from 300-2300nm), low hygroscopic susceptibility, high damage threshold. However, the nonlinear optical propertie of α-BBO is vanished due to the centric symmetry with its crystal structure. a-BBO is an excellent crystal to replace Calcite, TiO2, and LiNbO3, etc. in Glan-Taylor and Glan-Thompson polarizers as well as walk-off beam splitters, especially for high power and UV polarizer, due to its unique UV transparency, good mechanical properties and high damage threshold. Specifications:
Diameter | max. 40~50mm |
Length: | max. 25~35mm |
Surface Quality: | 2 0/10 |
Optical Deviation: | <1 arc min |
Optical Axis Orientation: | +/-0.5° |
Flatness: | <λ/8@633nm |
Wave Front: | <λ/8@633nm |
Coating: | According to custmer request |
Transparency Range | 189-3500nm |
Density | 3.85g/cm3 |
Therm-Optic Coefficients | dno/dT=-9.3X10-6/℃ dne/dT=-16.63X10-6/℃ |
Optical Homogeneity | Δn≈10-6/cm |
Damage Threshold | 1 GW/cm2 at 1064nm;500 MW/com2 at 532nm |
Hygroscopic Susceptibility | Low |
Thermal Expansion Coefficients (25℃-900℃) | aa=4X10-6/K ac=4X10-6/K |
Linear Absorption Coefficients | a<0.005cm-1 from 300nm to 2300nm |
Refractive Indices, Birefringence (Δn=ne-no) and Walk-Off Angle at 45℃(ρ) | ne=1.58462,no=1.65790,Δn=-0.073282;ρ=-4.9532o at 1064nm ne=1.60206, no=1.67755, Δn=-0.075491;ρ=-5.0407o at 532nm ne=1.67190, no=1.76171, Δn=-0.089805;ρ=-5.6926o at 266nm |