Newport MKS Quarter Wave Plate, Multiple-Order, Quartz, 25.4 mm Diameter, 1064 nm 10RP14-34

Description
The 10RP14-34 Multiple-Order Quarter Wave Plate is a crystal quartz optic designed to differentially retard the phase of a polarized beam. With the proper phase shift, this waveplate can be used to convert linear polarization into circular polarization. This 1 inch (25.4 mm) diameter wave plate is 1 mm thick and has λ/4 (90°) retardation. It is antireflection coated to maximize transmission at 1064 nm. When using multiple-order wave plates, several items should be considered. A wave plate of practical thickness produces a multiple of λ/4 or λ/2 retardation. Higher orders cause retardation to vary dramatically with wavelength. Wave plates are sensitive to temperature changes. A typical multiple-order wave plate has a temperature coefficient of 0.0015 λ/°C, compared to 0.000 1λ/°C for a zero-order wave plate, so tighter temperature control will be required. Precise adjustment of retardation is possible by tilting the wave plate. Tilting about the slow axis increases retardation, while tilting about the fast axis reduces retardation.
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Description
The 10RP14-34 Multiple-Order Quarter Wave Plate is a crystal quartz optic designed to differentially retard the phase of a polarized beam. With the proper phase shift, this waveplate can be used to convert linear polarization into circular polarization. This 1 inch (25.4 mm) diameter wave plate is 1 mm thick and has λ/4 (90°) retardation. It is antireflection coated to maximize transmission at 1064 nm. When using multiple-order wave plates, several items should be considered. A wave plate of practical thickness produces a multiple of λ/4 or λ/2 retardation. Higher orders cause retardation to vary dramatically with wavelength. Wave plates are sensitive to temperature changes. A typical multiple-order wave plate has a temperature coefficient of 0.0015 λ/°C, compared to 0.000 1λ/°C for a zero-order wave plate, so tighter temperature control will be required. Precise adjustment of retardation is possible by tilting the wave plate. Tilting about the slow axis increases retardation, while tilting about the fast axis reduces retardation.
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Quarter Wave Plate, Multiple-Order, Quartz, 25.4 mm Diameter, 1064 nm - 10RP14-34 - Newport MKS
Irvine, CA, United States
Quarter Wave Plate, Multiple-Order, Quartz, 25.4 mm Diameter, 1064 nm
10RP14-34
Quarter Wave Plate, Multiple-Order, Quartz, 25.4 mm Diameter, 1064 nm 10RP14-34
The 10RP14-34 Multiple-Order Quarter Wave Plate is a crystal quartz optic designed to differentially retard the phase of a polarized beam. With the proper phase shift, this waveplate can be used to convert linear polarization into circular polarization. This 1 inch (25.4 mm) diameter wave plate is 1 mm thick and has λ/4 (90°) retardation. It is antireflection coated to maximize transmission at 1064 nm. When using multiple-order wave plates, several items should be considered. A wave plate of practical thickness produces a multiple of λ/4 or λ/2 retardation. Higher orders cause retardation to vary dramatically with wavelength. Wave plates are sensitive to temperature changes. A typical multiple-order wave plate has a temperature coefficient of 0.0015 λ/°C, compared to 0.000 1λ/°C for a zero-order wave plate, so tighter temperature control will be required. Precise adjustment of retardation is possible by tilting the wave plate. Tilting about the slow axis increases retardation, while tilting about the fast axis reduces retardation.

The 10RP14-34 Multiple-Order Quarter Wave Plate is a crystal quartz optic designed to differentially retard the phase of a polarized beam. With the proper phase shift, this waveplate can be used to convert linear polarization into circular polarization. This 1 inch (25.4 mm) diameter wave plate is 1 mm thick and has λ/4 (90°) retardation. It is antireflection coated to maximize transmission at 1064 nm. When using multiple-order wave plates, several items should be considered. A wave plate of practical thickness produces a multiple of λ/4 or λ/2 retardation. Higher orders cause retardation to vary dramatically with wavelength. Wave plates are sensitive to temperature changes. A typical multiple-order wave plate has a temperature coefficient of 0.0015 λ/°C, compared to 0.000 1λ/°C for a zero-order wave plate, so tighter temperature control will be required. Precise adjustment of retardation is possible by tilting the wave plate. Tilting about the slow axis increases retardation, while tilting about the fast axis reduces retardation.

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Technical Specifications

  Newport MKS
Product Category Waveplates and Retardation Plates
Product Number 10RP14-34
Product Name Quarter Wave Plate, Multiple-Order, Quartz, 25.4 mm Diameter, 1064 nm
Material Quartz
Surface Quality 10-5 Scratch / Dig
Wavelength Range 1064 nm (10640 Å)
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