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格兰泰勒棱镜

 

是由两片相同双折射晶体材料棱镜制成的偏光器件,中间采用空气隙结构。此棱镜的长度与通光孔径的比值小于1.0, 使之成为相对较薄的偏光器件。此棱镜无逃逸窗口,因此适用于中低功率系统。由不同材料制成的格兰泰勒棱镜,其接收角各不相同,以下列表有相对应参数可对比。

产品特点:

·空气隙

·带宽覆盖紫外,可见和中红外

·接近布儒斯特切割角

·无逃逸窗口,反射光线被吸收,适用于中低功率系统

·高偏振度

·长度短,紧凑

Specifications:

Material: a-BBO, Calcite or YVO4
Wavelength Range: a-BBO: 200-3500 nm, Calcite: 350-2300 nm YVO4:500-5000 nm
Extinction Ratio: Calcite:<5x10-5; a-BBO:<5x10-6 ,YVO4:<5x10-6
Parallelism: <1 arc Min
Surface Quality: 20/10
Beam Deviation: < 3 arc minutes
Wavefornt Distortion: l /4@632.8nm
Damage Threshold: >200 MW/cm2
Coating: Single MgF2
Mount: Black Anodized Aluminium

 

1. Calcite Glan Taylor Polarizer

Part No. Wavelength Rang(nm) Extinction Ratio Angular Field(°) C.A. fa(mm) O.D. fd(mm) L ±0.1(mm)
GTP6006 350-2300 <5x10-5 >7.7 6.0 15.0 15.0
GTP6008 8.0 25.4 17.0
GTP6010 10.0 25.4 19.0
GTP6015 15.0 30.0 23.0
GTP6020 20.0 38.0 29.0

2. a-BBO Glan Taylor Polarizer

Part No. Wavelength Rang(nm) Extinction Ratio Angular Field(°) C.A. fa(mm) O.D. fd(mm) L±0.1(mm)
GTP5206 200-270 <5x10-6 >6.0 6.0 15.0 15.0
GTP5208 8.0 25.4 17.0
GTP5210 10.0 25.4 19.0
GTP5215 15.0 30.0 23.0
GTP5220 20.0 38.0 29.0
GTP5306 300-700 <5x10-6 >6.0 6.0 15.0 15.0
GTP5308 8.0 25.4 17.0
GTP5310 10.0 25.4 19.0
GTP5315 15.0 30.0 23.0
GTP5320 20.0 38.0 29.0
GTP5706 700-3000 <5x10-6 >6.0 6.0 15.0 15.0
GTP5708 8.0 25.4 17.0
GTP5710 10.0 25.4 19.0
GTP5715 15.0 30.0 23.0
GTP5720 20.0 38.0 29.0

3. YVO4 Glan Taylor Polarizer

Part No. Wavelength Rang(nm) Extinction Ratio Angular Field(°) C.A. fa(mm) O.D. fd(mm) L ±0.1(mm)
GTP9006 500-4000 <5x10-6 >6.5 6.0 15.0 12.0
GTP9008 8.0 25.4 15.0
GTP9010 10.0 25.4 17.0
GTP9015 15.0 30.0 20.0
GTP9020 20.0 38.0 25.0

 

Note: Kinds of sizes are available upon request.


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