Glan Taylor Polarizer.docx
Glan Taylor polarizer is made of two same birefringent material prisms that are assembled with an air space.Its length to aperture ratio which is less than 1.0 makes it a relatively thin polarizer.The polarizer with no side escape windows is suitable for low to medium power application where the side rejected beams are not required .The angular field of different materials of polarizers is listed below for comparison.
Air-spaced
Close to Brewster's Angle Cutting
High Polarization Purity
Short Length
Wide Wavelength Range
Suitable for medium power application
Close to Brewster's Angle Cutting
High Polarization Purity
Short Length
Wide Wavelength Range
Suitable for medium power application
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Item
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Calcite GTP
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a-BBO GTP
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YVO4 GTP
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Wavelength Range
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350-2000nm
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190-3500nm
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500-4000nm
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Extinction Ratio
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<5*10-5
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<5*10-6
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<5*10-6
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Surface Quality
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20/10 Scratch/Dig
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Beam Deviation
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< 3 arc minutes
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Wavefront Distortion
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<λ/4@633nm
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Damage Threshold
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>200MW/cm2@1064nm, 20ns, 20Hz
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Coating
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P Coating Or AR Coating
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Mount
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Black Anodized Aluminium
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Angular Field vs Wavelength:
 350-2300nn Calcite
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 200-300nm a-BBO
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 300-700nm a-BBO
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 700-3500nm a-BBO
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Standard Products:
a-BBO Glan Taylor Polarizer
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Part No
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Wavelength Range
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Ratio
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Angular Field
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CA(mm)
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Holder(mm)
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200-300nm
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<5*10-6
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>6°
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φ6.0
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φ15*15
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|
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GTP1210
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φ10
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φ25.4*19
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|||
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GTP1215
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φ15
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φ30*23
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|||
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GTP1220
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φ20
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φ38*29
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|||
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GTP1306
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300-700nm
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<5*10-6
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>6°
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φ6.0
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φ15*15
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GTP1310
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φ10
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φ25.4*19
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|||
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GTP1315
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φ15
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φ30*23
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|||
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GTP1320
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φ20
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φ38*29
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|||
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GTP1706
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700-3500nm
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<5*10-6
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>6°
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φ6.0
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φ15*15
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GTP1710
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φ10
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φ25.4*19
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|||
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GTP1715
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φ15
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φ30*23
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|||
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GTP1720
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φ20
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φ38*29
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Calcite Glan Taylor Polarizer：
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Part No
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Wavelength Range
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Ratio
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Angular Field
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CA(mm)
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Holder(mm)
|
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GTP2006
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350-2300nm
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<5*10-5
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>6°
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φ6.0
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φ15*15
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GTP2010
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φ10
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φ25.4*19
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|||
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GTP2015
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φ15
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φ30*23
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|||
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GTP2020
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φ20
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φ38*29
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YVO4 Glan Taylor Polarizer：
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Part No
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Wavelength Range
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Ratio
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Angular Field
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CA(mm)
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Holder(mm)
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GTP3006
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500-4000nm
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<5*10-6
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>6°
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φ6.0
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φ15*15
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GTP3010
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φ10
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φ25.4*19
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|||
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GTP3015
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φ15
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φ30*23
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