Low Order Waveplate
Low Order Waveplate Drawing

Low Order Waveplate

High Damage Threshold
Better Temperature Bandwidth
Low Cost
Thickness: 0.2-0.5 mm


Retardation Tolerance:

Surface Quality:


Damage Threshold:
>10J/cm², 20ns, 20Hz at 1064nm



Wavefront Distortion:
λ/8 @ 632.8nm


Low Order Waveplate can yield λ/4 or λ/2 retardation by selecting some specified thickness. And it is much better than the multi-order waveplates because of its thinner thickness, better temperature, wave length and incidence angle, bandwidth and high damage threshold. These properties make it widely used for high and low power laser application. Thickness: 0.2-0.5 mm
wdt_ID Attributes Value
76 Material: Quartz
77 Wavelength: 200~2300nm
78 Diameter Tolerance: +0.0 / -0.1mm
88 Surface Quality: 20/10
89 Parallelism: <1''
90 Retardation Tolerance: <λ/300
91 C.A: >90%
96 Wavefront Distortion: λ/8 @ 632.8nm
101 Damage Threshold: >10J/ cm², 20ns, 20Hz at 1064nm
102 Coating: AR/AR@wavelength
103 Mount: Black Anodized Aluminium
The most common types of waveplates are quarter-wave plates (λ/4 plates) and half-wave plates (λ/2 plates), where the difference of phase delays between the two linear polarization directions is π/2 or π, respectively, corresponding to propagation phase shifts over a distance of λ / 4 or λ / 2, respectively.
Some important cases are:
  • When a light beam is linearly polarized, and the polarization direction is along one of the axes of the waveplate, the polarization remains unchanged.
  • When the incident polarization does not coincide with one of the axes, and the plate is a half-wave plate, then the polarization stays linear, but the polarization direction is rotated. For example, for an angle of 45° to the axes, the polarization direction is rotated by 90°.
  • When the incident polarization is at an angle of 45° to the axes, a quarter-wave plate generates a state of circular polarization. (Other input polarizations lead to elliptical polarization states.) Conversely, circularly polarized light is converted into linearly polarized light.
Within a laser resonator, two quarter-wave plates around the gain medium are sometimes used for obtaining single-frequency operation (→ twisted-mode technique). Inserting a half-wave plate between a laser crystal and a resonator end mirror can help to reduce depolarization loss. The combination of a half-wave plate and a polarizer allows one to realize an output coupler with adjustable transmission.
Many waveplates are made of crystalline quartz (SiO2), as this optical material exhibits a wide wavelength range with very high transparency, and can be prepared with high optical quality. Other possible materials (to be used e.g. in other wavelength regions) are calcite (CaCO3), magnesium fluoride (MgF2), sapphire (Al2O3), mica (a silicate material), and some birefringent polymers.

Related Resource for reference

Half Wave Plate
The half wave plate can be used to rotate the polarization state of a plane polarized light as shown in Figure 1.
Suppose a plane-polarized wave is normally incident on a wave plate, and the plane of polarization is at an angle q with respect to the fast axis, as shown. After passing through the plate, the original plane wave has been rotated through an angle 2q.
A half-wave plate is very handy in rotating the plane of polarization from a polarized laser to any other desired plane (especially if the laser is too large to rotate). Most large ion lasers are vertically polarized. To obtain horizontal polarization, simply place a half-wave plate in the beam with its fast (or slow) axis 45° to the vertical. The l/2 plates can also change left circularly polarized light into right circularly polarized light or vice versa. The thickness of half waveplate is such that the phase difference is 1/2 wavelength (l/2, Zero order) or certain multiple of 1/2-wavelength [(2n+1)l/2, multiple order].
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