Glan–Taylor Crystal Polarizing Prism GT10-T8

Glan–Taylor Crystal Polarizing Prism GT10-T8

Supplier
Jcoptix
Part Number
GT10-T8
Category
Polarization Optics
Origin
China

Glan crystal polarizing prisms use the Glan-Taylor design: two high-grade birefringent crystals are placed back-to-back with their inclined faces facing each other. The prisms have the same optical-axis orientation, parallel to the reflecting surface and perpendicular to the propagating beam. Birefringence produces different refractive indices along and perpendicular to the optical axis. At the glass-air interface between the prisms, total internal reflection occurs: the reflected light includes all ordinary (o) light and some extraordinary (e) light, while the transmitted light is highly linearly polarized e light, suitable for applications requiring high-quality polarized beams. An air gap rather than chemical bonding between the crystals raises the damage threshold for high-power use. JCOPTIX Glan-Taylor prisms are mounted in black-anodized housings. A coating on the prism surface absorbs reflected light, making them suitable for medium-power lasers. For high-power applications, JCOPTIX offers Glan-laser prisms made from very low-scattering birefringent crystals. Contact technical support for custom substrates, coatings, or sizes. Glan-Taylor housings have standard SM1 external threads for direct installation in standard SM1 internally threaded mounts, such as MMR-1T rotation mounts. JCOPTIX's proprietary cushioning rubber washer at the base of the SM1 thread allows the prism polarization direction to align directly with a specific rotation-mount angle. Operation is simple and quick: 1. Screw the prism into the rotation mount until the SM1 thread reaches its end; lock the mount's rotating part as needed. 2. Check the angular difference between the polarization direction (white housing line) and the target scale mark (0° or 90°). 3. Apply slight force to continue turning the protruding cylindrical housing until the white polarization line aligns with the target mark. The adjustment range is approximately 60°.

Specification Snapshot
Operating Wavelength
700-3000 nm
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Overview

Glan crystal polarizing prisms use the Glan-Taylor design: two high-grade birefringent crystals are placed back-to-back with their inclined faces facing each other. The prisms have the same optical-axis orientation, parallel to the reflecting surface and perpendicular to the propagating beam. Birefringence produces different refractive indices along and perpendicular to the optical axis. At the glass-air interface between the prisms, total internal reflection occurs: the reflected light includes all ordinary (o) light and some extraordinary (e) light, while the transmitted light is highly linearly polarized e light, suitable for applications requiring high-quality polarized beams. An air gap rather than chemical bonding between the crystals raises the damage threshold for high-power use. JCOPTIX Glan-Taylor prisms are mounted in black-anodized housings. A coating on the prism surface absorbs reflected light, making them suitable for medium-power lasers. For high-power applications, JCOPTIX offers Glan-laser prisms made from very low-scattering birefringent crystals. Contact technical support for custom substrates, coatings, or sizes. Glan-Taylor housings have standard SM1 external threads for direct installation in standard SM1 internally threaded mounts, such as MMR-1T rotation mounts. JCOPTIX's proprietary cushioning rubber washer at the base of the SM1 thread allows the prism polarization direction to align directly with a specific rotation-mount angle. Operation is simple and quick: 1. Screw the prism into the rotation mount until the SM1 thread reaches its end; lock the mount's rotating part as needed. 2. Check the angular difference between the polarization direction (white housing line) and the target scale mark (0° or 90°). 3. Apply slight force to continue turning the protruding cylindrical housing until the white polarization line aligns with the target mark. The adjustment range is approximately 60°.

Specifications

ParameterValue
Optical element materialLaser-Grade α-BBO
Operating Wavelength700-3000 nm
Prism Dimensions12.2 mm × 13.7 mm
Clear Aperture DimensionØ10.0 mm
Extinction Ratio100,000:1
Acceptance angle [REF]< ± 2° REF
Beam Deviation<10 arcsec
Transmitted wavefront error [@633 nm]< λ/8
Structural DesignHigh-Damage-Threshold Air-Spaced Structure
Housing DiameterØ25.4 mm +0.0/-0.2 mm
Housing Thickness16 mm ± 0.1 mm
Housing threadSM1 external thread
Surface quality (scratch/dig) [Exit/Entrance Face / Side Face]20/10 (Exit/Entrance Faces), 80/50 (Side Faces)

Key Features

High extinction ratio above 100,000:1. High laser damage threshold, suitable for medium-power lasers. Operating wavelength: 200-3000 nm. Special cushioning rubber-pad design. Prealigned kit: Glan-Taylor crystal polarizing prism with a rotation mount. Prealigned kit: polarization direction precisely aligned with the mount's 0° graduation.

Datasheet

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Supplier Information

Jc
Jcoptix
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Nanjing Jingcui Optical Technology Co., Ltd. (formerly Suzhou Jingcui Optical Technology Co., Ltd., abbreviated as JCOPTIX) is a national high-tech enterprise and a national-level specialized and sophisticated 'little giant' enterprise, established on the foundation of the Liquid Crystal and Photonics Research Center of Nanjing University. It engages in R&D, manufacturing, and sales of advanced optical technologies and products. JCOPTIX is dedicated to building a product platform for China's optical community, offering liquid crystal photonics components, precision optical components, optomechanics, fiber optic assemblies, motion control devices, and system solutions. All listed products can be found and ordered online at www.JCOPTIX.com.

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Glan–Taylor Crystal Polarizing Prism GT10-T8
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