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DOE_Special-Patterns (Special Patterns)
LD Collimators & Diffractive Optics: Pattern-Generator

Diffractive Optical Element (DOE)

Description:

LD Collimators & Diffractive Optics: Beam-shaping-Optics

Beam shaping optics in terms of diffractive optics involve the use of precisely engineered microstructures to control and shape light beams for a variety of advanced applications, leveraging the principles of diffraction to achieve high precision and flexibility.

LD Collimators & Diffractive Optics: Beam-Splitter

A beam splitter in the context of diffractive optics is a device that utilizes diffractive elements to divide a beam of light into two or more separate beams. Unlike traditional beam splitters that use partial reflection and transmission through materials like glass, diffractive beam splitters rely on the principles of diffraction and interference to achieve the splitting.

LD Collimators & Diffractive Optics: Pattern-Generator

Diffractive pattern generators stand out due to several unique characteristics that distinguish them from other optical technologies. One of their most significant advantages is their ability to precisely control light at a microscopic level. The microstructures on the diffractive optical elements (DOEs) are meticulously designed to manipulate the phase and amplitude of light waves, enabling the creation of highly accurate and complex light patterns. This level of precision is challenging to achieve with traditional optical components. Another key feature is the high degree of customization and versatility they offer. By designing specific patterns into the DOE, manufacturers can tailor the light output to meet various application needs. Whether producing simple shapes like lines and circles or more intricate designs for holography and 3D imaging, the versatility of these generators makes them suitable for a wide range of uses. Diffractive optics pattern generators are also known for their efficiency and compactness. Compared to conventional optics that rely on refraction and reflection, diffractive optics can achieve similar or superior performance with much thinner and lighter components. This efficiency leads to more compact and lightweight designs, which are particularly advantageous in portable devices and systems where space and weight are critical factors. The ability to produce light patterns with very high resolution and uniformity is another hallmark of diffractive optics pattern generators. This quality is essential in applications like laser projection and optical metrology, where clarity and consistency of the light pattern are paramount. Additionally, these generators can be designed to work with specific wavelengths of light, including visible, ultraviolet, and infrared. This wavelength versatility allows for their use in a wide range of scientific and industrial applications, from microscopy to laser cutting and medical imaging. Diffractive optics pattern generators are highly compatible with modern laser and photonic technologies. They can be integrated into existing systems to enhance performance and functionality, such as improving beam shaping in laser machining or enhancing image quality in projection systems. The robustness and durability of these generators are notable as well. The microstructures on DOEs are typically etched or printed onto durable materials, making them robust and long-lasting. This durability is especially beneficial in industrial environments where equipment must withstand harsh conditions. Finally, while the initial design and fabrication of DOEs can be complex, the production process can be highly cost-effective, especially for large quantities. Once a DOE design is finalized, it can be replicated with high precision at a relatively low cost, making it an economical choice for mass production. In summary, diffractive optics pattern generators are distinguished by their precision, versatility, efficiency, high-quality output, wavelength adaptability, ease of integration, robustness, and cost-effectiveness. These attributes make them a preferred choice in various advanced optical applications, from industrial manufacturing to cutting-edge scientific research.

This article refers to: DOE_Special-Patterns (Special Patterns) (LD Collimators & Diffractive Optics: Pattern-Generator ) - Special Patterns

DOE Item # Description Design Wavelength Pattern Size @ 100 mm Distance (@ Design Wavelength) Pattern Angles (@ Design Wavelength) Optimum Wavelength Range Image
FDE-R256 Square Grid 51 x 51 Lines 660 nm Width: 39 mm
Height: 39 mm
Diagonal: 55 mm
Line Spacing: 0.77 mm
Width: 22°
Height: 22°
Diagonal: 31°
Angle betw. Lines: 0.44°
530 – 660 nm Grid 51x51 Picture.jpg
FDE-R259 5 Rings 645 nm Width: 51 mm
Line Spacing: 5.1 mm
Width: 29°
Line Spacing: 2.8°
530 – 700 nm Five Circles Picture.jpg
FDE-R269 10 Rings 515 nm Width: 96.2 mm
Line Spacing: 4.8 mm
Width: 51.4°
Line Spacing: 2.6°
488 – 532 nm Ten Circles.jpg
FDE-R285 Hexagon 780 nm Width: 13.1 mm Width: 7.5° 520 – 800 nm Hexagon.jpg
FDE-R354 Square Grid 10×10 Lines 658 nm Width: 72.8 mm
Height: 72.8 mm
Diagonal: 102.9 mm
Line Spacing: 8.1 mm
Width: 40.0°
Height: 40.0°
Diagonal: 51.4°
Angle betw. Lines: 4°
620 – 680 nm Square Grid.jpg
FDE-R396 21×11 Hexagonal Array 660 nm* Width: 61.1 mm
Height: 35.3 mm
Diagonal: 70.5 mm
Dot Spacing: 3.5 mm
Width: 34.0°
Height: 20.0°
Diagonal: 38.8°
Angle betw. Dots: 2.0°
600 – 730 nm
FDE-R397 11×10 Hexagonal Array 660 nm* Width: 44.4 mm
Height: 46.2 mm
Diagonal: 64.1 mm
Dot Spacing: 5.1 mm
Width: 25.1°
Height: 26.0°
Diagonal: 35.5°
Angle betw. Dots: 2.9°
600 – 730 nm
FDE-R399 5 Rings 450 nm Width: 51 mm
Line Spacing: 7.3 mm
Width: 40°
Line Spacing: 4.0°
400 – 500 nm

 

*Large-angle pattern that due to its symmetry properties is subject to geometrical distortion, if the DOE is used at laser wavelengths significantly different (Δλ > 50nm) from the design wavelength.

 
  • Pattern-Generator

Downloads

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FDE-R256 (Square Grid 51 x 51 Lines, 660nm)

431 KB
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FDE-R259 (5 Rings, 645nm)

385 KB
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FDE-R269 (10 Rings, 515nm)

400 KB
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FDE-R285 (Hexagon, 780nm)

363 KB
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FDE-R354 (Square Grid 10 x 10 Lines, 658nm)

277 KB
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FDE-R396 (21 x 11 Dots Hexagonal Array, 660nm)

275 KB
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FDE-R397 (11 x 10 Dots Hexagonal Array, 660nm)

258 KB
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FDE-R399 (5 Rings, 450nm)

237 KB
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