Low Order Dual Wavelength Waveplates

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Low Order Dual Wavelength Waveplates
Low order dual wavelength waveplates control polarization precisely for dual wavelength sources.
Traitements AR(R<0.2 %) on each surface
Tolérances de diamètre, mm +0/-0.2 mm
Seuil de dommage laser, J/cm² >5 J/cm2 for 10 ns pulses @ 1064 nm
Material Crystalline Quartz
Parallelism, arcsec < 3 arcsec
Retardation Tolerance λ/300 @ 20 °C
Qualité de surface, s-d 20/10 S/D
Tolérance d'épaisseur, mm ±0.2 mm
Transmitted Wavefront Distortion <λ/10@632.8 nm
Mounting Mounted in Ø25.4x 6 mm black anodized metal mount
Description

Détails

Waveplates are made from materials which exhibit birefringence. The velocities of the extraordinary and ordinary rays through the birefringent material varies inversely with their refractive indices. Difference in velocities gives rise to a phase difference when two beams recombine. At any specific wavelength the phase difference is governed by the thickness of the retarder - waveplate.

Dual wavelength low order waveplates are made from high quality crystalline quartz and are available at quarter-wave, half-wave and full-wave retardance. One of possible examples is a waveplate, which is designed to be used in dual wavelength setup at 800 nm and 400 nm. It operate as a λ/2 plate at 800 nm and λ plate at 400 nm. This means that 45° rotation of waveplate, induces 90° rotation of electrical vector at 800 nm and does not change state of polarization at 400 nm. Another possible configuration is λ/2 plate at 800 nm and λ/4 plate at 400 nm. In this case waveplate rotates electrical vector by 90° at 800 nm and provides a circular polarization at 400 nm. These are just two possible configurations out of many available. All waveplates are mounted in Ø25,4 mm black anodized aluminum ring and feature clear aperture of 18 mm.
Fonctionnalités
  • Controls polarization for dual wavelength sources
Name Ouverture utile, mmRetardation and wavelength Prix Quantité

2-LODW-L-1030-L/2-515

> 18λ @ 1030 nm + λ/2 @ 515 nm
266,50 $US

2-LODW-L-1064-L/2-532

> 18λ @ 1064 nm + λ/2 @ 532 nm
266,50 $US

2-LODW-L-355-L/2-1064

> 18λ @ 355 nm + λ/2 @ 1064 nm
266,50 $US

2-LODW-L-355-L/2-532

> 18λ @ 355 nm + λ/2 @ 532 nm
266,50 $US

2-LODW-L-800-L/2-400

> 18λ @ 800 nm + λ/2 @ 400 nm
266,50 $US

2-LODW-L/2-1030-L-515

> 18λ/2 @ 1030 nm + λ @ 515 nm
266,50 $US

2-LODW-L/2-1030-L/4-515

> 18λ/2 @ 1030 nm + λ/4 @ 515 nm
266,50 $US

2-LODW-L/2-1064-L-532

> 18λ/2 @ 1064 nm + λ @ 532 nm
266,50 $US

2-LODW-L/2-1064-L/4-532

> 18λ/2 @ 1064 nm + λ/4 @ 532 nm
266,50 $US

2-LODW-L/2-355-L-1064

> 18λ/2 @ 355 nm + λ @ 1064 nm
266,50 $US

2-LODW-L/2-355-L-532

> 18λ/2 @ 355 nm + λ @ 532 nm
266,50 $US

2-LODW-L/2-355-L/4-1064

> 18λ/2 @ 355 nm + λ/4 @ 1064 nm
266,50 $US

2-LODW-L/2-355-L/4-532

> 18λ/2 @ 355 nm + λ/4 @ 532 nm
266,50 $US

2-LODW-L/2-800-L-400

> 18λ/2 @ 800 nm + λ @ 400 nm
266,50 $US

2-LODW-L/2-800-L/4-400

> 18λ/2 @ 800 nm + λ/4 @ 400 nm
266,50 $US

2-LODW-L/4-1030-L/2-515

> 18λ/4 @ 1030 nm + λ/2 @ 515 nm 
266,50 $US

2-LODW-L/4-1064-L/2-532

> 18λ/4 @ 1064 nm + λ/2 @532 nm 
266,50 $US

2-LODW-L/4-355-L/2-1064

> 18λ/4 @ 355 nm + λ/2 @ 1064 nm
266,50 $US

2-LODW-L/4-355-L/2-532

> 18λ/4 @ 355 nm + λ/2 @ 532 nm
266,50 $US

2-LODW-L/4-800-L/2-400

> 18λ/4 @ 800 nm + λ/2 @ 400 nm
266,50 $US
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