GLAN TAYLOR POLARIZER
Keywords:
Keywords:
GLAN TAYLOR POLARIZER
Basic Parameters
Glan Taylor Polarizercontain a variety of materials, including Calcite crystals, A-BBO crystals, YVO4 crystals, . Glan Taylor Polarizer are compact and shorter in length than Glan Laser Polarizer, making them suitable for high polarization applications at low to medium power. It can make the input unpolarized beam into a pure polarized light, and is often used as a bias or bias detector for optical path systems.
|
FEATURES |
|
Air -spaced design |
|
Compact structure |
|
Highly polarized output |
|
No escape window on the side |
|
Suitable for low and medium power |
|
Broadband anti-reflection film can be plated |
Processing Index
| Standard Specifications | Calcite | a-BBO/Barium Borate | YVO4/Yttrium Vanadate |
| Wavelength | 350-2000nm | 190-3500nm | 500-4000nm |
| Extinction Ratio | <5*10-5 | <5*10-6 | <5*10-6 |
| Surface Quality | 20/10 Scratch/Dig | ||
| Beam Deviation | < 3 arc minutes | ||
| TWD | <λ/4@633nm | ||
| LIDT | >200MW/cm2@1064nm, 20ns, 20Hz | ||
| Coating | P Coating，Customizable coating available per customer requirements | ||
| Mounting |
Anodized Aluminum Mount Square or round mount available |
||
a-BBO Standard Products：
| Type | Wavelength | Extinction Ratio | Angle | CA | Square Mount (mm) | Round Mount (mm) |
| GTP1206 | 200-300nm | <5*10-6 | >6° | φ6.0 | 9*9*8 | φ15*15 |
| GTP1210 | φ10 | 13*13*11 | φ25.4*19 | |||
| GTP1215 | φ15 | 18*18*16 | φ30*23 | |||
| GTP1220 | φ20 | 24*24*20 | φ38*29 | |||
| GTP1306 | 300-700nm | <5*10-6 | >6° | φ6.0 | 9*9*8 | φ15*15 |
| GTP1310 | φ10 | 13*13*11 | φ25.4*19 | |||
| GTP1315 | φ15 | 18*18*16 | φ30*23 | |||
| GTP1320 | φ20 | 24*24*20 | φ38*29 | |||
| GTP1706 | 700-3500nm | <5*10-6 | >6° | φ6.0 | 9*9*8 | φ15*15 |
| GTP1710 | φ10 | 13*13*11 | φ25.4*19 | |||
| GTP1715 | φ15 | 18*18*16 | φ30*23 | |||
| GTP1720 | φ20 | 24*24*20 | φ38*29 |
Calcite Standard Products：
| Type | Wavelength | Extinction Ratio | Angle | CA | Square Mount (mm) | Round Mount (mm) |
| GTP2006 | 350-2300nm | <5*10-5 | >6° | φ6.0 | 9*9*8 | φ15*15 |
| GTP2010 | φ10 | 13*13*11 | φ25.4*19 | |||
| GTP2015 | φ15 | 18*18*16 | φ30*23 | |||
| GTP2020 | φ20 | 24*24*20 | φ38*29 |
YVO4 Standard Products：
| Type | Wavelength | Extinction Ratio | Angle | CA (mm) |
Square Mount (mm) |
Round Mount (mm) |
| GTP3006 | 500-4000nm | <5*10-6 | >6° | φ6.0 | 9*9*8 | φ15*15 |
| GTP3010 | φ10 | 13*13*11 | φ25.4*19 | |||
| GTP3015 | φ15 | 18*18*16 | φ30*23 | |||
| GTP3020 | φ20 | 24*24*20 | φ38*29 |
Solutions
Scientific research and testing field
Aviation field
Medical cosmetology field
Laser field
Related Products
YVO4
Yttrium alumate (YVO4) is an excellent birefringent crystal material, which is a negative uniaxial crystal. The crystal has good physical and mechanical properties, wide light transmission range, high transmittance, large birefringence coefficient and easy processing. YVO4 crystal can replace ice SPAR and crystal red stone in the field of optical fiber communication, is the key material in optical communication passive devices such as optical isolators, circulators, polarization splitters, polarizers.
Caicite
Caicite Crystal is a kind of natural birefringent material, in the shape of diamond, birefringence coefficient is large, through the spectrum is wide, from visible to near infrared has relatively good optical properties. Although the mechanical strength of Iceland SPAR material is soft and easy to scratch, it still does not affect its wide application in polarization devices. Caicite is mainly used in Glan POLARIZER.
LiNbO3
LiNbO3 is widely used in optical fiber communication as a birefringent crystal. The crystal has good physical and mechanical properties, wide light transmission range, high transmittance, easy processing, and lower material cost than other materials. Lithium niobate crystals are widely used in passive optical communication devices such as optical isolators, circulators, polarization splitters, polarizers, etc
POLARIZING BEAM SPLITTER（PBS）
The polarization splitter prism is plated with a multilayer film structure on the inclined surface of the right Angle prism, and then glued into a cube structure. By taking advantage of the property that the transmission rate of P-polarized light is 1 and that of S-polarized light is less than 1 when the light incident at Brewster Angle, the P polarization component can be completely penetrated after the light passes through the multilayer film structure at Brewster Angle for many times. And most of the S polarization component is reflected. Note: Specific bands and extinction ratios can be customized according to customer requirements.
Product Inquiry
*Note: Please be sure to fill in the information accurately and keep the communication open. We will contact you as soon as possible.
Email Address