1030, 1050 or 1064 nm Center Wavelengths
High Power PBS Cube Beamsplitter
High Verdet Constant
Low Absorption Coefficients
4 mm or 8 mm Aperture
1/2 Waveplate Option
Our high power Faraday optical isolators can be used in the 1013 nm to 1077 nm wavelength range and provides double escape ports for applications where rejected power exceeds 0.5 W.
| Model | Description | Availability | Price | Qty. | |
|---|---|---|---|---|---|
| ISO-FRDY-04-1030-N | High Power Faraday Optical Isolator, 4 mm Aperture, 1030 nm Center | Call | ¥20,980.10 | ADD |
| ISO-FRDY-04-1030-W | High Power Faraday Optical Isolator, 4 mm, 1030 nm, 1/2 Waveplate | Call | ¥22,732.09 | ADD |
| ISO-FRDY-04-1050-N | High Power Faraday Optical Isolator, 4 mm Aperture, 1050 nm Center | Call | ¥20,980.10 | ADD |
| ISO-FRDY-04-1050-W | High Power Faraday Optical Isolator, 4 mm, 1050 nm, 1/2 Waveplate | Call | ¥22,732.09 | ADD |
| ISO-FRDY-04-1064-N | High Power Faraday Optical Isolator, 4 mm Aperture, 1064 nm Center | Call | ¥25,403.88 | ADD |
| ISO-FRDY-04-1064-W | High Power Faraday Optical Isolator, 4 mm, 1064 nm, 1/2 Waveplate | Call | ¥27,155.87 | ADD |
| ISO-FRDY-08-1030-N | High Power Faraday Optical Isolator, 8 mm Aperture, 1030 nm Center | Call | ¥30,659.86 | ADD |
| ISO-FRDY-08-1030-W | High Power Faraday Optical Isolator, 8 mm, 1030 nm, 1/2 Waveplate | Call | ¥32,411.85 | ADD |
| ISO-FRDY-08-1050-N | High Power Faraday Optical Isolator, 8 mm Aperture, 1050 nm Center | Call | ¥30,659.86 | ADD |
| ISO-FRDY-08-1050-W | High Power Faraday Optical Isolator, 8 mm, 1050 nm, 1/2 Waveplate | Call | ¥32,411.85 | ADD |
| ISO-FRDY-08-1064-N | High Power Faraday Optical Isolator, 8 mm Aperture, 1064 nm Center | Call | ¥31,973.85 | ADD |
| ISO-FRDY-08-1064-W | High Power Faraday Optical Isolator, 8 mm, 1064 nm, 1/2 Waveplate | Call | ¥32,411.85 | ADD |
| Model | ISO-FRDY-04-1030-N | ISO-FRDY-04-1050-N | ISO-FRDY-04-1064-N | ISO-FRDY-08-1030-N | ISO-FRDY-08-1050-N | ISO-FRDY-08-1064-N |
|---|---|---|---|---|---|---|
| Clear Aperture (mm) | 4 | 4 | 4 | 8 | 8 | 8 |
| Center Wavelength (nm) | 1030 | 1050 | 1064 | 1030 | 1050 | 1064 |
| Spectral Range (nm) | 1017 - 1043 | 1037 - 1063 | 1051 - 1077 | 1017 - 1043 | 1037 - 1063 | 1051 - 1077 |
| Isolation (dB) @ 22°C | 30 | 30 | 30 | 30 | 30 | 30 |
| Transmission (%) @ 22°C | > 92 | > 92 | > 92 | > 92 | > 92 | > 92 |
|
Pulse Damage Threshold (J/cm2), for 10ns pulses | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps | 10 J/cm² @ 10ns; 1 J/cm² @ 8ps |
| Polarizer Type | PBS Cube Polarizer | |||||
| Rotating Medium | Terbium Gallium Garnet | |||||
Our high power Faraday optical isolators use high damage threshold Fused Silica polarizing beamsplitter (PBS) cubes that are optically contacted rather than cemented. They also utilize double escape ports for added application flexibility.
The TGG utilized in our Faraday Isolators, creates a large Verdet constant that ultimately describes the strength of the Faraday effect.
Our Faraday Isolators have low absorption as a function of the TGG and Polarizers.
High power faraday optical isolators are offered with 4 mm apertures or 8 mm apertures for larger beam sizes.
We offer versions with an added 1/2 wave plate at the output stage so that the direction of the output beam polarization can be rotated to a desired direction.
| Low Power Faraday Optical Isolators | Broadband Faraday Optical Isolators | Mid-IR Faraday Optical Isolators | Broadband Polarizing Cube Beamsplitters |
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