Berek’s variable waveplates modify the polarization of collimated beams from any state to any other state with the flexibility, convenience, and precision previously found only in bulky and expensive Soleil-Babinet compensators. True zero-order retardance, minimal wavefront distortion, and beam displacement of less than 150 µm are all featured at an economical price.
- Soleil-Babinet compensator performance at a much lower cost
- Variable zero-order retardance
- Ideal for removing arbitrary ellipticity in your experiment
- Combine with a polarizer to create or analyze any polarization state
- Angular sensitivity equal to Soleil Babinet
- Less than 150 µm beam displacement See All Features
| Compare | Description | Drawings, CAD & Specs | Avail. | Price | ||
|---|---|---|---|---|---|---|
![]() | 5540-U Berek’s Variable WaveplatesVariable Wave Plate, Berek's, 8-32 and M4 Threads |
Features
Based on Polarization Compensator First Discussed by Berek
Berek's Wave Plate Mounting
The Berek’s variable waveplate can be directly mounted to an Optical Post or Pedestal Riser, but we recommend using it with our 9854 Opti-Claw adjustable 2 inch or our M2 Standard 2 inch Mirror mounts. This allows you to align the waveplate so that it is truly normal to the incident beam, ensuring zero phase retardance and the accuracy of the wave plate.
Waveplate Applications
Basic Isolator Applications
Polarization Compensator Applications
Our Berek's waveplates offer fine adjustment of a laser polarization state. A Berek’s waveplate may be used to compensate precisely for small phase shifts produced by other optics in your experiment. Vary the retardance and orientation of the waveplate to produce very small retardance until your system is optimized.





