Newport MKS Half Wave Plate, Multiple-Order, Quartz, 12.7 mm Diameter, 413 nm 05RP12-41

Description
The 05RP12-41 Multiple-Order Half 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 rotate the direction of polarization and the amount of polarization rotation is twice the amount of the waveplate rotation. This 1/2 inch (12.7 mm) diameter wave plate is 1 mm thick and has λ/2 (180°) retardation. It is antireflection coated to maximize transmission at 413 nm. When using multiple-order waveplates, 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 0.0015λ/°C, compared to 0.0001λ/°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 05RP12-41 Multiple-Order Half 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 rotate the direction of polarization and the amount of polarization rotation is twice the amount of the waveplate rotation. This 1/2 inch (12.7 mm) diameter wave plate is 1 mm thick and has λ/2 (180°) retardation. It is antireflection coated to maximize transmission at 413 nm. When using multiple-order waveplates, 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 0.0015λ/°C, compared to 0.0001λ/°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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Half Wave Plate, Multiple-Order, Quartz, 12.7 mm Diameter, 413 nm - 05RP12-41 - Newport MKS
Irvine, CA, United States
Half Wave Plate, Multiple-Order, Quartz, 12.7 mm Diameter, 413 nm
05RP12-41
Half Wave Plate, Multiple-Order, Quartz, 12.7 mm Diameter, 413 nm 05RP12-41
The 05RP12-41 Multiple-Order Half 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 rotate the direction of polarization and the amount of polarization rotation is twice the amount of the waveplate rotation. This 1/2 inch (12.7 mm) diameter wave plate is 1 mm thick and has λ/2 (180°) retardation. It is antireflection coated to maximize transmission at 413 nm. When using multiple-order waveplates, 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 0.0015λ/°C, compared to 0.0001λ/°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 05RP12-41 Multiple-Order Half 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 rotate the direction of polarization and the amount of polarization rotation is twice the amount of the waveplate rotation. This 1/2 inch (12.7 mm) diameter wave plate is 1 mm thick and has λ/2 (180°) retardation. It is antireflection coated to maximize transmission at 413 nm. When using multiple-order waveplates, 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 0.0015λ/°C, compared to 0.0001λ/°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 05RP12-41
Product Name Half Wave Plate, Multiple-Order, Quartz, 12.7 mm Diameter, 413 nm
Material Quartz
Surface Quality 10-5 Scratch / Dig
Wavelength Range 413 nm (4130 Å)
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