Our true zero-order quarter-wave waveplates consist of a birefringent polymer film cemented between two high-precision N-BK7 optical windows, each with a high efficiency, broadband antireflection coating. Polymer wave plates offer several benefits over quartz wave plates, such as better angular acceptance and less sensitivity to wavelength change.
- λ/4 waveplate for converting plane-polarized light to circularly polarized
- ±λ/350 retardation accuracy
- Birefringent polymer film cemented between two windows
- Less sensitive to wavelength change than quartz waveplates
- Better angular acceptance than either multiple-order or zero-order quartz See All Features
| Compare | Description | Drawings, CAD & Specs | Avail. | Price | ||
|---|---|---|---|---|---|---|
![]() | 05RP34-532Zero-Order Waveplate, Quarter-Wave, Polymer, 12.7 mm Diameter, 532 nm | In Stock | ||||
![]() | 05RP34-780Zero-Order Waveplate, Quarter-Wave, Polymer, 12.7 mm Diameter, 780 nm | In Stock | ||||
![]() | 05RP34-1300Zero-Order Waveplate, Quarter-Wave, Polymer, 12.7 mm Diameter, 1300 nm | In Stock | ||||
![]() | 10RP34-532Zero-Order Waveplate, Quarter-Wave, Polymer, 25.4 mm Diameter, 532 nm | In Stock | ||||
![]() | 10RP34-1064Zero-Order Waveplate, Quarter-Wave, Polymer, 25.4 mm Diameter, 1064 nm | In Stock | ||||
![]() | 10RP34-1550Zero-Order Waveplate, Quarter-Wave, Polymer, 25.4 mm Diameter, 1550 nm |
Mounting Options
Manual Rotation Mounts
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| Retaining Thread | 1.063-20 | |||||
| Compatible Optic Diameter* | 25.4 mm 12.7 mm ( |
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| Special Features | 1 in. Mirror Mounts Compatibility | OpticsCage+™ Compatibility | Tip&Tilt Adjustments | Fine Adjustments | ||
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| Models | ( |
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| Retaining Thread | 0.546-32 | 1.040-32 | 1.035-40 | 1.063-20 | 2.063-20 1.063-20 |
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| Compatible Optic Diameter* | 12.7 mm | 25.4 mm | 25.4 mm 12.7 mm ( |
50.8 mm 25.4 mm 12.7 mm ( |
50.8 mm ( 38.1 mm ( 25.4 mm ( 12.7 mm ( 6.35 mm ( |
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| Special Features | Compact | Stackable | A-Line™ Compatibility | Fine Adjustments | Quick Exchange | |
Specifications
- Retardationλ/4
- Retardation Accuracy±λ/350
- MaterialGrade A N-BK7
- HousingBlack anodized aluminum
- Acceptance Angle±9°
- Transmitted Beam Deviation≤1 arc min
- Wavefront Distortion≤λ/5 at 632.8 nm over the full aperture
- Damage Threshold500 W/cm2 CW
- Pulse Damage Threshold0.5 J/cm2 with 10 nsec pulses, @ 1064 nm
0.3 J/cm2 with 10 nsec pulses @ 532 nm - Reflectivity per Surface<0.5%
- Antireflection CoatingBroadband, multilayer coating
- Surface Quality40-20 scratch-dig
- Diameter Tolerance±0.13 mm
- Operating Temperature Range-20 to 50°C
- Cleaning
Features
Polymer Zero-Order Waveplate Construction
Our true zero-order wave plates consist of a birefringent polymer film cemented between two high-precision N-BK7 optical windows, each with a high efficiency, broadband antireflection coating. This construction ensures excellent transmitted wavefront quality, while minimizing beam deviation and surface reflection losses. The assembly is mounted in a black anodized aluminum housing for protection and ease of mounting, with the wave plate fast axis marked for alignment reference.
Convert Plane-polarized Light to Circularly Polarized
Quarter-wave waveplates are used to turn plane-polarized light into circularly polarized light and vice versa. To do this, we must orient the wave plate so that equal amounts of fast and slow waves are excited – for example, by orienting an incident plane-polarized wave at 45° to the fast (or slow) axis. On the other side of the waveplate, we again examine the wave at a point where the fast-polarized component is at maximum. At this point, the slow-polarized component will be passing through zero, since it has been retarded by a quarter-wave or 90° in phase. If we move an eighth wavelength farther, we will note that the two are the same magnitude, but the fast component is decreasing and the slow component is increasing. Moving another eighth wave, we find the slow component is at maximum and the fast component is zero. If we trace the tip of the total electric vector, we find it traces out a helix, with a period of just one wavelength. This describes circularly polarized light.
Retardation is Insensitive to Wavelength
The polymer material has very low birefringence that is nearly constant with wavelength. The retardance δ at a new wavelength λ that is different from the center wavelength λc is given by: δ = δc(λc/λ) where δc is the retardance at λc. The primary benefit is a moderate insensitivity to wavelength change, making them ideal for laser diode or tunable laser applications.



























