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Waveplates retards change the state of polarization. They resolve
an incident beam of light into orthogonally polarized
components and retard the phase of one component relative
to the other. The emergent usually has a different polarization
state from the incident beam.
The most common type of retarder is a slice of birefringent
material in which the o-ray travels at different velocities.
Two rays that start in phase develop a phase difference
with respect to each other. For light of wavelength
^ the phase difference 0 is given by:
0 = +- 2 (pie) d (ne-no)/^
Where:
d= thickness of waveplate
ne= refractive index for extraordinary ray
no= refractive index for the ordinary ray
We can offer multiple order and zero order wavelengths.
Zero order wavelengths have higher acceptance angles,
wide bandwidth and lower temperature coefficients than
multiple order waveplates. Wavelenghts are within the
range of 200 to 2300 nm
1/2 Wave Plate
A 1/2 waveplate is used in rotating the plane of linear
polarization.

1/4 waveplate
A 1/4 waveplate is used in changing linear polarized
light to circularly polarized or creating linear polarization
from circular.
Specifications
| Material: |
Crystal Quartz |
| Dimension Tolerance: |
+0.0, -0.2mm |
| Wavefront Distortion: |
<^/8 @ 632.8mm |
| Retardation Tolerance: |
<^/300 |
| Parallelism: |
< 10 arc seconds |
| Surface Quality: |
20-10 scratch and dig |
| AR-Coating: |
R < 0.2% at centre wavelength |
| Retardation: |
<^/2, <^/4 |
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