Our medium power Farady optical isolators use SF1 polarizing beamsplitters (PBS) for 461, 532, 650, 780, 850, 980 nm laser applications requiring up to a 2 kW/cm2 CW damage threshold. Double escape ports are provided for applications where rejected power exceeds 0.5 W.
- 461, 532, 650, 780, 850, 980 nm center wavelengths
- High Verdet constant
- Low absorption coefficients
- 1/2 Waveplate Option (-W models)
- Tunability over a broad spectral range See All Features
| Compare | Description | Drawings, CAD & Specs | Avail. | Price | ||
|---|---|---|---|---|---|---|
![]() | ISO-04-461-MP Medium Power Faraday Optical Isolators | |||||
![]() | ISO-04-532-MP Medium Power Faraday Optical Isolators | |||||
![]() | ISO-04-532-MP-W Medium Power Faraday Optical Isolators | |||||
![]() | ISO-04-650-MP Medium Power Faraday Optical Isolators | |||||
![]() | ISO-04-650-MP-W Medium Power Faraday Optical Isolators | |||||
![]() | ISO-04-780-MP Medium Power Faraday Optical Isolators | Discontinued | ||||
![]() | ISO-04-780-MP-W Medium Power Faraday Optical Isolators | Discontinued | ||||
![]() | ISO-04-850-MP Medium Power Faraday Optical Isolators | Discontinued | ||||
![]() | ISO-04-850-MP-W Medium Power Faraday Optical Isolators | Discontinued | ||||
![]() | ISO-04-980-MP Medium Power Faraday Optical Isolators | Discontinued | ||||
Features
High Efficiency Performance
The TGG crystal utilized in our Faraday isolators creates a large Verdet constant that ultimately describes the strength of the Faraday effect and provides effective isolation of back-reflected light. Additionally, these isolators have low absorption as a function of the TGG crystal and polarizers, resulting in reliable transmission of light in the forward direction.
Easy Placement into Optical Train
These isolators are packaged in a compact, cylindrically-shaped magneto-optic device with a base plate for easy mounting into an optical train.
Resources
Manuals
MP ISO Faraday Isolators User's Manual(732.8 kB, PDF)











