Broadband Quartz Waveplate 30mm Diameter Wavelength Range 700 - 1000nm λ/4
WPQW-NIR-4M
Air spaced two piece waveplates are suitable for use with high-energy lasers (no optical contact occurs). These products utilize birefringence of quartz and give phase difference of λ/4 (π/2, 90°) or λ/2 (π, 180°) to the input beams. λ/4 retarders convert linearly polarization to circularly and circularly polarization to linearly. λ/2 retarders convert the direction of polarization arbitrarily.
◦Air spaced type waveplates are zero-order (first-order) retardation plates (phase plates) which are assembled from pairs of crystalline quartz plates and are mounted on aluminum frames.
| Name | Broadband Quartz Waveplate 30mm Diameter Wavelength Range 700 - 1000nm λ/4 |
|---|---|
| Gewicht | 0.0110kgs |
| Standard Coatings Available | Nein |
| Guide |
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| Remark | - |
| Attention |
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| Design wavelength | 700 - 1000nm |
| Image Label | Broadband Quartz Waveplate 30mm Diameter Wavelength Range 700 - 1000nm λ/4 |
| Material | Crystalline quartz , MgF2 |
| Material propreties | Aluminum (Finishing ; Black Anodized) |
| Clear aperture | 14×14mm |
| Transmitted wavefront distortion | λ/4( Per one pice of substrate) |
| Angular deviation of beam | ＜5″ |
| Coating | Antireflection Coating on both side (Total 4 surfaces) |
| Transmittance | ＞Average 98% |
| type | λ/4 |
| Wavelength range λ | 700 - 1000nm |
| Theoretical retardation (fｉｒｓt Wavelength) | 172.4nm (at 700nm) |
| Theoretical retardation (Second Wavelength) | 201nm (at 800nm) |
| Theoretical retardation (Third Wavelength) | 225.2nm (at 900nm) |
| Theoretical retardation (4th Wavelength) | 247.2nm (at 1000nm) |
| Laser Damage Threshold<sup>*</sup> | 7J/cm2 |
| Availability | Please contact |
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SKU
WPQW-NIR-4M
1.343,60 €
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Air spaced two piece waveplates are suitable for use with high-energy lasers (no optical contact occurs). These products utilize birefringence of quartz and give phase difference of λ/4 (π/2, 90°) or λ/2 (π, 180°) to the input beams. λ/4 retarders convert linearly polarization to circularly and circularly polarization to linearly. λ/2 retarders convert the direction of polarization arbitrarily.
