Glan Taylor prism 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.
Material: | a-BBO, Calcite,YVO4 |
Wavelength Range: | a-BBO: 200-3500 nm, Calcite: 350-2300 nm,YVO4: 400-4000 nm |
Extinction Ratio: | Calcite:<5x10-5 ; α-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 |
Part No. | Wavelength Rang(nm) | Extinction Ratio | Angular Field(°) | C.A. fa(mm) | O.D. fd(mm) | L±0.1(mm) |
GTP6206
|
200-270
|
<5x10-6
|
>6.0
|
6.0
|
15.0
|
15.0
|
GTP6208
|
8.0
|
25.4
|
17.0
|
|||
GTP6210
|
10.0
|
25.4
|
19.0
|
|||
GTP6215
|
15.0
|
30.0
|
23.0
|
|||
GTP6306
|
300-700
|
<5x10-6
|
>6.0
|
6.0
|
15.0
|
15.0
|
GTP6308
|
8.0
|
25.4
|
17.0
|
|||
GTP6310
|
10.0
|
25.4
|
19.0
|
|||
GTP6315
|
15.0
|
30.0
|
23.0
|
|||
GTP6706
|
700-3000
|
<5x10-6
|
>6.0
|
6.0
|
15.0
|
15.0
|
GTP6708
|
8.0
|
25.4
|
17.0
|
|||
GTP6710
|
10.0
|
25.4
|
19.0
|
|||
GTP6715
|
15.0
|
30.0
|
23.0
|
Part No. | Wavelength Rang(nm) | Extinction Ratio | Angular Field(°) | C.A. fa(mm) | O.D. fd(mm) | L±0.1(mm) |
GTP7006
|
300-2300
|
<5x10-5
|
>7.7
|
6.0
|
15.0
|
12.0
|
GTP7008
|
8.0
|
25.4
|
15.0
|
|||
GTP7010
|
10.0
|
25.4
|
17.0
|
|||
GTP7015
|
15.0
|
30.0
|
20.0
|
Part No. | Wavelength Rang(nm) | Extinction Ratio | Angular Field(°) | C.A. fa(mm) | O.D. fd(mm) | L±0.1(mm) |
GTP8006
|
300-2300
|
<5x10-6
|
>6.5
|
6.0
|
15.0
|
15.0
|
GTP8008
|
8.0
|
25.4
|
17.0
|
|||
GTP8010
|
10.0
|
25.4
|
19.0
|
|||
GTP8015
|
15.0
|
30.0
|
23.0
|