Lens-Array Homogenizers SLB-PBMLA25S-850-F5

Lens-Array Homogenizers SLB-PBMLA25S-850-F5

Supplier
Sinteclaser
Part Number
SLB-PBMLA25S-850-F5
Category
Optical Lenses
Origin
China

Lens-array homogenizers provide non-collimated homogenization of multimode laser beams into different shapes, for applications such as beam homogenization in medical aesthetics and background-illumination homogenization in machine vision. Our range includes flat microlens arrays and flat cylindrical-lens arrays. A flat microlens array is a flat optical element that uses liquid-crystal-polymer diffractive optics for laser homogenization and beam shaping. It comprises a polymer film and a single N-BK7 window, with an arrayed phase distribution in the film producing the microlens-array function. Output-beam form depends on microlens-unit parameters. Adjusting their phase period and profile flexibly controls output divergence and spot shape for homogenization and shaping into varied shapes and sizes. The device is polarization dependent: right- or left-handed circular input makes light diverge or converge after each lenslet. The divergence or convergence angle follows sinθ=λ/p, where λ is design wavelength and p is the radial phase period of a lenslet. The single-wavelength design has no spherical aberration, and the antireflection-coated input surface gives high transmission and diffraction efficiency. Applications include wavefront sensing, light concentration and beam shaping, with strong potential in optical information processing, optical interconnects, optical computing, image scanners, light-field cameras, medical instruments, 3D imaging and displays. A flat cylindrical-lens array similarly uses liquid-crystal-polymer diffractive optics for one-dimensional beam shaping and homogenization. A polymer film between two N-BK7 windows has a one-dimensional phase array providing cylindrical-lens-array functionality. Modulation depends on incident polarization and cylindrical-lens-unit parameters. Left-handed circular input produces right-handed circular output that first converges and then diverges; right-handed circular input produces diverging left-handed circular output. The divergence or convergence angle follows sinθ=λ/p, where λ is design wavelength and p is the cylindrical-lens-unit phase period. Adjusting this period flexibly controls output divergence for different one-dimensional shaping and homogenization requirements. This is also a single-wavelength design free of spherical aberration with an antireflection-coated input surface for high transmission and diffraction efficiency. It has strong potential for imaging, machine vision and semiconductor laser collimation. Standard microlens arrays have size Ø25.4 mm, lenslet focal lengths of 5 mm or 50 mm, square output beams and operating wavelengths of 532 nm, 633 nm, 850 nm, 915 nm and 976 nm. Custom options include special sizes, operating wavelength, beam divergence and beam profile. Output spot nonuniformity is the RMS energy error over the region above 90% of the normalized spot-energy distribution. Diffraction efficiency is the energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy.

Specification Snapshot
Diffraction Efficiency [Standard microlens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]
>98%
Operating Wavelength [Custom - Microlens Array]
400-1700nm
Diffraction Efficiency [Custom microlens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]
>98%
Diffraction Efficiency [Standard cylindrical-lens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]
>98%
Operating Wavelength [Custom - Cylindrical Lens Array]
400-1700nm
Diffraction Efficiency [Custom cylindrical-lens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]
>98%
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Overview

Lens-array homogenizers provide non-collimated homogenization of multimode laser beams into different shapes, for applications such as beam homogenization in medical aesthetics and background-illumination homogenization in machine vision. Our range includes flat microlens arrays and flat cylindrical-lens arrays. A flat microlens array is a flat optical element that uses liquid-crystal-polymer diffractive optics for laser homogenization and beam shaping. It comprises a polymer film and a single N-BK7 window, with an arrayed phase distribution in the film producing the microlens-array function. Output-beam form depends on microlens-unit parameters. Adjusting their phase period and profile flexibly controls output divergence and spot shape for homogenization and shaping into varied shapes and sizes. The device is polarization dependent: right- or left-handed circular input makes light diverge or converge after each lenslet. The divergence or convergence angle follows sinθ=λ/p, where λ is design wavelength and p is the radial phase period of a lenslet. The single-wavelength design has no spherical aberration, and the antireflection-coated input surface gives high transmission and diffraction efficiency. Applications include wavefront sensing, light concentration and beam shaping, with strong potential in optical information processing, optical interconnects, optical computing, image scanners, light-field cameras, medical instruments, 3D imaging and displays. A flat cylindrical-lens array similarly uses liquid-crystal-polymer diffractive optics for one-dimensional beam shaping and homogenization. A polymer film between two N-BK7 windows has a one-dimensional phase array providing cylindrical-lens-array functionality. Modulation depends on incident polarization and cylindrical-lens-unit parameters. Left-handed circular input produces right-handed circular output that first converges and then diverges; right-handed circular input produces diverging left-handed circular output. The divergence or convergence angle follows sinθ=λ/p, where λ is design wavelength and p is the cylindrical-lens-unit phase period. Adjusting this period flexibly controls output divergence for different one-dimensional shaping and homogenization requirements. This is also a single-wavelength design free of spherical aberration with an antireflection-coated input surface for high transmission and diffraction efficiency. It has strong potential for imaging, machine vision and semiconductor laser collimation. Standard microlens arrays have size Ø25.4 mm, lenslet focal lengths of 5 mm or 50 mm, square output beams and operating wavelengths of 532 nm, 633 nm, 850 nm, 915 nm and 976 nm. Custom options include special sizes, operating wavelength, beam divergence and beam profile. Output spot nonuniformity is the RMS energy error over the region above 90% of the normalized spot-energy distribution. Diffraction efficiency is the energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy.

Specifications

ParameterValue
Operating Wavelength [Standard Product - Microlens Array]532,633,850,915,976nm
Element Dimensions and Mounting (Side Length or Diameter Specification) [Standard Product - Microlens Array]Ø25.4x1.6 mm, compatible with 1-inch optic mounts
Clear Aperture Dimension [Standard Product - Microlens Array]Ø21.5 mm
Input Beam Quality Requirements [Standard Product - Microlens Array]Multimode
Input Beam Polarization State Requirements [Standard Product - Microlens Array]None
Focal Length [Standard Product - Microlens Array]5mm,50mm
Output Spot Shape [Standard Product - Microlens Array]Square
Output Spot Nonuniformity [Standard microlens array; RMS energy error over the region above 90% of the normalized spot-energy distribution]<10%
Transmittance [Standard Product - Microlens Array ;400-450 nm]>85%
Transmittance [Standard Product - Microlens Array ;450-1700 nm]>96%
Reflectance Ravg [Standard Product - Microlens Array ;0° Angle of Incidence]Ravg <0.5%(0° Angle of Incidence )
Diffraction Efficiency [Standard microlens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]>98%
Operating Wavelength [Custom - Microlens Array]400-1700nm
Element Dimensions and Mounting (Side Length or Diameter Specification) [Custom - Microlens Array]3-160 mm (side length or diameter specification)
Clear Aperture Dimension [Custom - Microlens Array]≤ substrate inscribed-circle diameter x90%
Input Beam Quality Requirements [Custom - Microlens Array]Multimode
Input Beam Polarization State Requirements [Custom - Microlens Array]None
Output Spot Shape [Custom - Microlens Array]Arbitrary shapes such as squares, triangles and regular hexagons; shapes allowing dense tiling are best
Output Spot Nonuniformity [Custom microlens array; RMS energy error over the region above 90% of the normalized spot-energy distribution]<10%
Transmittance [Custom - Microlens Array ;400-450 nm]>85%
Transmittance [Custom - Microlens Array ;450-1700 nm]>96%
Reflectance Ravg [Custom - Microlens Array ;0° Angle of Incidence]Ravg <0.5%(0° Angle of Incidence )
Diffraction Efficiency [Custom microlens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]>98%
Operating Wavelength [Standard Product - Cylindrical Lens Array]520,650,915,940,976nm
Element Dimensions and Mounting (Side Length or Diameter Specification) [Standard Product - Cylindrical Lens Array]Ø25.4x3.2 mm, compatible with 1-inch optic mounts
Clear Aperture Dimension [Standard Product - Cylindrical Lens Array]Ø21.5 mm
Input Beam Quality Requirements [Standard Product - Cylindrical Lens Array]Multimode
Input Beam Polarization State Requirements [Standard Product - Cylindrical Lens Array]None
Focal Length [Standard Product - Cylindrical Lens Array]5mm,50mm
Output Spot Shape [Standard Product - Cylindrical Lens Array]Line-Shaped
Output Spot Nonuniformity [Standard cylindrical-lens array; RMS energy error over the region above 90% of the normalized spot-energy distribution]<10%
Transmittance [Standard Product - Cylindrical Lens Array ;400-450 nm]>85%
Transmittance [Standard Product - Cylindrical Lens Array ;450-1700 nm]>96%
Reflectance Ravg [Standard Product - Cylindrical Lens Array ;0° Angle of Incidence]Ravg <0.5%(0° Angle of Incidence )
Diffraction Efficiency [Standard cylindrical-lens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]>98%
Operating Wavelength [Custom - Cylindrical Lens Array]400-1700nm
Element Dimensions and Mounting (Side Length or Diameter Specification) [Custom - Cylindrical Lens Array]3-160mm (side length or diameter specification)
Clear Aperture Dimension [Custom - Cylindrical Lens Array]≤ substrate inscribed-circle diameter x90%
Input Beam Quality Requirements [Custom - Cylindrical Lens Array]Multimode
Input Beam Polarization State Requirements [Custom - Cylindrical Lens Array]None
Output Spot Shape [Custom - Cylindrical Lens Array]Line-Shaped
Output Spot Nonuniformity [Custom cylindrical-lens array; RMS energy error over the region above 90% of the normalized spot-energy distribution]<10%
Transmittance [Custom - Cylindrical Lens Array ;400-450 nm]>85%
Transmittance [Custom - Cylindrical Lens Array ;450-1700 nm]>96%
Reflectance Ravg [Custom - Cylindrical Lens Array ;0° Angle of Incidence]Ravg <0.5%(0° Angle of Incidence )
Diffraction Efficiency [Custom cylindrical-lens array; energy in the region above 90% of the normalized spot-energy distribution divided by all output optical energy]>98%

Key Features

Flat, compact structure for easy integration Transmissive homogenization for high energy utilization Continuous phase and high fill factor for high diffraction efficiency and effective homogenization Flexible customization with selectable homogenized shape and adjustable divergence Better suited to non-collimated homogenization of multimode lasers

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Supplier Information

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Sinteclaser
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Wuhan Sintec Optoelectronics Technology Co., Ltd. is a high-tech enterprise and a specialized and sophisticated 'Little Giant' enterprise at the upstream of the domestic laser industry chain. The company focuses on the R&D, manufacturing, sales and service of lasers and laser accessories. Its main products include femtosecond lasers, picosecond lasers, acousto-optic modulators, optical components, etc., widely used in laser equipment manufacturing, scientific research and other fields. Located in Wuhan Optical Valley, with a modern industrial park, the company provides one-stop personalized services for the laser industry, with customers all over China and products exported overseas.

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