Crystalline quartz waveplates

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Crystalline quartz waveplates
Zero Order (ZO), Low order (LO) or Multiple order (MO) half or quarter waveplates, polarization rotators for UV, VIS and NIR (for any wavelength in 240-2600 nm range)
Traitements antireflets R < 0.2% at each surface
Ouverture utile, mm >18
Seuil de dommage laser, J/cm² 5 J/cm2 10 ns pulsed at 1064 nm typical
Material Crystalline Quartz
Parallelism, arcsec < 3 arcsec
Retardation Tolerance λ/300 @ 20 °C
Qualité de surface, s-d 20-10 scratch & dig
Wavefront Distortion λ/10 @ 632.8 nm
Mounting Mounted in Ø 25.4x6 mm black anodized metal mount
Description

Détails

To suit different applications, air spaced, glued or optically contacted Zero Order compensated phase retardation plates are available.

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. This difference in velocities gives rise to a phase difference when the two beams recombine. At any specific wavelength the phase difference is governed by the thickness of the retarder - waveplate.

Half (λ/2) Waveplate. A linearly polarized beam incident on a half wave crystal quartz waveplate emerges as a linearly polarized beam but rotated such that its angle to the optical axis is twice that of the incident beam. Therefore, half-waveplates can be used as continuously adjustable polarization rotators. Half-waveplates are used to rotate the plane of polarization, electro-optic modulation and as a variable ratio beamsplitter when used in conjunction with a polarization cube.

Quarter (λ/4) Waveplate - thin-film compensator. If the angle between the electric field vector of the incident linearly polarized beam and the retarder principal plane of the quarter-waveplate is 45, the emergent beam is circularly polarized. When a quarter waveplate is double passed, i.e. by mirror reflection, it acts as a half waveplates and rotates the plane of polarization to a certain angle. Quarter waveplate are used in creating circular polarization from linear or linear polarization from circular, ellipsometry, optical pumping, suppressing unwanted reflection and optical isolation.
Zero Order waveplates are generally preferred since they are least sensitive to variations in wavelength, angle of incidence and temperature.

Air-spaced crystal quartz waveplates are also available. Its performance is as good as cemented zero-order waveplate. Additionally, the air-spaced construction enables it is suitable for the high power laser application. The damage threshold is more than 500 MW/cm2.

Phase retardation plates - waveplates for the IR range, polarization rotators, Faraday isolators are available on request.
Fonctionnalités
  • Waveplates are made from excellent quality laser grade Crystalline Quartz material
Name RetardationRetardation OrderLongueur d'onde, nm Prix Quantité

2-CPW-LO-L/2-0266

λ/2LO266
162,50 $US

2-CPW-LO-L/2-0343

λ/2LO343
162,50 $US

2-CPW-LO-L/2-0355

λ/2LO355
162,50 $US

2-CPW-LO-L/2-0400

λ/2LO400
162,50 $US

2-CPW-LO-L/2-0473

λ/2LO473
162,50 $US

2-CPW-LO-L/2-0515

λ/2LO515
162,50 $US

2-CPW-LO-L/2-0532

λ/2LO532
162,50 $US

2-CPW-LO-L/2-0589

λ/2LO589
162,50 $US

2-CPW-LO-L/2-0633

λ/2LO633
162,50 $US

2-CPW-LO-L/2-0780

λ/2LO780
162,50 $US

2-CPW-LO-L/2-0800

λ/2LO800
162,50 $US

2-CPW-LO-L/2-0852

λ/2LO852
162,50 $US

2-CPW-LO-L/2-0940

λ/2LO940
162,50 $US

2-CPW-LO-L/2-0980

λ/2LO980
162,50 $US

2-CPW-LO-L/2-1030

λ/2LO1030
162,50 $US

2-CPW-LO-L/2-1064

λ/2LO1064
162,50 $US

2-CPW-LO-L/2-1122

λ/2LO1122
162,50 $US

2-CPW-LO-L/2-1319

λ/2LO1319
162,50 $US

2-CPW-LO-L/2-1550

λ/2LO1550
162,50 $US

2-CPW-LO-L/4-0266

λ/4LO266
162,50 $US

2-CPW-LO-L/4-0343

λ/4LO343
162,50 $US

2-CPW-LO-L/4-0355

λ/4LO355
162,50 $US

2-CPW-LO-L/4-0400

λ/4LO400
162,50 $US

2-CPW-LO-L/4-0473

λ/4LO473
162,50 $US

2-CPW-LO-L/4-0515

λ/4LO515
162,50 $US

2-CPW-LO-L/4-0532

λ/4LO532
162,50 $US

2-CPW-LO-L/4-0589

λ/4LO589
162,50 $US

2-CPW-LO-L/4-0633

λ/4LO633
162,50 $US

2-CPW-LO-L/4-0780

λ/4LO780
162,50 $US

2-CPW-LO-L/4-0800

λ/4LO800
162,50 $US

2-CPW-LO-L/4-0852

λ/4LO852
162,50 $US

2-CPW-LO-L/4-0940

λ/4LO940
162,50 $US

2-CPW-LO-L/4-0980

λ/4LO980
162,50 $US

2-CPW-LO-L/4-1030

λ/4LO1030
162,50 $US

2-CPW-LO-L/4-1064

λ/4LO1064
162,50 $US

2-CPW-LO-L/4-1122

λ/4LO1122
162,50 $US

2-CPW-LO-L/4-1319

λ/4LO1319
162,50 $US

2-CPW-LO-L/4-1550

λ/4LO1550
162,50 $US

2-CPW-ZO-L/2-0266

λ/2ZO266
312,00 $US

2-CPW-ZO-L/2-0343

λ/2ZO343
312,00 $US

2-CPW-ZO-L/2-0355

λ/2ZO355
312,00 $US

2-CPW-ZO-L/2-0400

λ/2ZO400
312,00 $US

2-CPW-ZO-L/2-0473

λ/2ZO473
312,00 $US

2-CPW-ZO-L/2-0515

λ/2ZO515
312,00 $US

2-CPW-ZO-L/2-0532

λ/2ZO532
312,00 $US

2-CPW-ZO-L/2-0589

λ/2ZO589
312,00 $US

2-CPW-ZO-L/2-0633

λ/2ZO633
312,00 $US

2-CPW-ZO-L/2-0780

λ/2ZO780
312,00 $US

2-CPW-ZO-L/2-0800

λ/2ZO800
312,00 $US

2-CPW-ZO-L/2-0852

λ/2ZO852
312,00 $US

2-CPW-ZO-L/2-0940

λ/2ZO940
312,00 $US

2-CPW-ZO-L/2-0980

λ/2ZO980
312,00 $US

2-CPW-ZO-L/2-1030

λ/2ZO1030
312,00 $US

2-CPW-ZO-L/2-1064

λ/2ZO1064
312,00 $US

2-CPW-ZO-L/2-1122

λ/2ZO1122
312,00 $US

2-CPW-ZO-L/2-1319

λ/2ZO1319
312,00 $US

2-CPW-ZO-L/2-1550

λ/2ZO1550
312,00 $US

2-CPW-ZO-L/4-0266

λ/4ZO266
312,00 $US

2-CPW-ZO-L/4-0343

λ/4ZO343
312,00 $US

2-CPW-ZO-L/4-0355

λ/4ZO355
312,00 $US

2-CPW-ZO-L/4-0400

λ/4ZO400
312,00 $US

2-CPW-ZO-L/4-0473

λ/4ZO473
312,00 $US

2-CPW-ZO-L/4-0515

λ/4ZO515
312,00 $US

2-CPW-ZO-L/4-0532

λ/4ZO532
312,00 $US

2-CPW-ZO-L/4-0589

λ/4ZO589
312,00 $US

2-CPW-ZO-L/4-0633

λ/4ZO633
312,00 $US

2-CPW-ZO-L/4-0780

λ/4ZO780
312,00 $US

2-CPW-ZO-L/4-0800

λ/4ZO800
312,00 $US

2-CPW-ZO-L/4-0852

λ/4ZO852
312,00 $US

2-CPW-ZO-L/4-0940

λ/4ZO940
312,00 $US

2-CPW-ZO-L/4-0980

λ/4ZO980
312,00 $US

2-CPW-ZO-L/4-1030

λ/4ZO1030
312,00 $US

2-CPW-ZO-L/4-1064

λ/4ZO1064
312,00 $US

2-CPW-ZO-L/4-1122

λ/4ZO1122
312,00 $US

2-CPW-ZO-L/4-1319

λ/4ZO1319
312,00 $US

2-CPW-ZO-L/4-1550

λ/4ZO1550
312,00 $US
OU