Faraday Isolator / Rotator — a kind of magneto-optical device based on the Faraday magneto-optical effect.
Faraday Isolator can rotate the polarization direction of the polarized light to a certain angle, and the rotation direction is only related to the internal magnetic field. It has nothing to do with the light direction. The rotation angle of the standard Faraday isolator is designed as 45˚ or 90˚. A 45˚ Rotator is placed between two polarizers in a 45˚ configuration to form a faraday optical isolator. Faraday optical isolator is a kind of magneto-optical device with unidirectional light transmission, widely used in laser amplification systems, film-locked laser, and laser measurement equipment.
Our company has independently developed and produced a series of Rotators and Isolators. They are made of high-quality terbium gallium garnet (TGG) magneto-optical crystal, polarizing spectroprism, and high coercive magnetic materials. The series products have the highest isolation, transmittance, laser damage threshold resistance, and temperature application range.
- High isolation
- Low insertion loss
- Multiple clear apertures
- Double escape windows at both ends
- Multiple wavelengths available
- Practicality of a certain wavelength bandwidth
- Output polarization controllable
- Seed light amplifying laser
- Lock film laser
- A semiconductor laser
- Optical measuring equipment
- Optical parametric oscillator
Parameter (25℃）
| Model | Central Wavelength | Clear Aperture | Isolation @25℃ | Transmittance @25℃ | Polarizer | Damage Threshold @10ns | Assembly |
| CL-ISO-532-5 | 532nm | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 2# |
| CL-ISO-633-2.5 | 633nm | 2.5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 1# |
| CL-ISO-633-5 | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 1# | |
| CL-ISO-780-2.5 | 780nm | 2.5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 1# |
| CL-ISO-780-5 | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 2# | |
| CL-ISO-785-2.5 | 785nm | 2.5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 1# |
| CL-ISO-785-5 | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 2# | |
| CL-ISO-920-5 | 920nm | 5mm | ＞30dB | >95% | PBS Cube | 10J/cm2 | 5# |
| CL- ISO-1030-2.5 | 1030nm | 2.5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 3# |
| CL-ISO-1030-5 | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 3# | |
| CL-ISO-1064-2.5 | 1064nm | 2.5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 3# |
| CL-ISO-1064-5 | 5mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 3# | |
| CL-ISO-1064-8 | 8mm | ＞30dB | >90% | PBS Cube | 10J/cm2 | 4# |
| Model | Center wavelength | Clear Aperture | Isolation @25℃ | Transmittance@25℃ | Polarizer | Damage Threshold @10ns | Size |
| CLC-ISO-488-5 | 488nm | 5mm | ≥30dB | ≥80% | PBS scheme | 3.5J/cm2 10ns 10Hz 1064nm | φ30×70mm |
| CLC-ISO-488-4 | 4mm | φ20×50mm | |||||
| CLC-ISO-633-2.5 | 633nm | 2.5mm | Polarizer | φ20×26mm |
| Model | Central Wavelength | Clear Aperture | Extinction ratio @25℃ | Transmittance @25℃ | Rotation angle @25℃ | Damage Threshold @10ns | Assembly |
| CL-ROT-532-5 | 532nm | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 2# |
| CL-ROT-633-2.5 | 633nm | 2.5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 1# |
| CL-ROT-633-5 | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 2# | |
| CL-ROT-780-2.5 | 780nm | 2.5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 1# |
| CL-ROT-780-5 | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 2# | |
| CL-ROT-785-2.5 | 785nm | 2.5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 1# |
| CL-ROT-785-5 | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 2# | |
| CL- ROT-1030-2.5 | 1030nm | 2.5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 3# |
| CL-ROT-1030-5 | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 3# | |
| CL-ROT-1064-2.5 | 1064nm | 2.5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 3# |
| CL-ROT-1064-5 | 5mm | ＞30dB | ＞95% | 45°±1° | 10J/cm2 | 3# |
