Precision Pinhole, Stainless Steel Material MPS1-5

Body Material: 6061-T6 Housing Surface Finish: Black Anodized Pinhole Metal Foil Material: 300 Series Stainless Steel

JCOPTIX precision pinholes suit optical alignment, beam adjustment, imaging, and related applications. Pinhole diameters span 5-2000 μm. The metal foil is installed in an Ø25.4 mm outside-diameter aluminum-alloy housing for convenient compatibility with Ø25.4 mm optomechanics. Unhoused foils are also available for different needs. In spatial filters, the extremely thin pinhole foil is vulnerable to damage at high power. Align at low power before switching to high-power operation. Custom apertures are available alongside standard pinholes; contact support. Stainless-steel precision pinholes. Models: MPS1-5, MPS1-10, MPS1-20, MPS1-30, MPS1-40, MPS1-50, MPS1-70, MPS1-100, MPS1-150, MPS1-200, MPS1-300, MPS1-400, MPS1-500, MPS1-600, MPS1-750, MPS1-1000, MPS1-2000. Black anodizing increases absorption; aperture range 5-2000 μm; 6061-T6 aluminum-alloy housing, standard diameter Ø25.4 mm. JCOPTIX stainless-steel pinholes offer apertures of 5-2000 μm in uncoated stainless-steel foil mounted in Ø25.4 mm outside-diameter aluminum-alloy housings. They conveniently fit JCOPTIX lens mounts or 30 mm cage plates. Their ultrathin foil is vulnerable at high power in spatial filters, so align at low power before switching to high power. Unhoused stainless-steel precision pinholes. Models: MPS1-5-UN, MPS1-10-UN, MPS1-20-UN, MPS1-25-UN, MPS1-30-UN, MPS1-40-UN, MPS1-50-UN, MPS1-70-UN, MPS1-100-UN, MPS1-150-UN, MPS1-200-UN, MPS1-300-UN, MPS1-400-UN, MPS1-500-UN, MPS1-600-UN, MPS1-750-UN, MPS1-1000-UN, MPS1-2000-UN. Black anodizing increases absorption (apertures >50 μm are black); aperture range 5-2000 μm; unmounted foil, outside diameter 9.52 mm. JCOPTIX unhoused stainless-steel pinholes offer apertures of 5-2000 μm in 9.52 mm outside-diameter stainless-steel foil. Foils 30 μm thick, with apertures ≤50 μm, retain the original color on both faces; foils 50 μm thick, with apertures >50 μm, are blackened on both faces. Since the foil is only 30-50 μm thick, handle it carefully with small tweezers or pliers to avoid damage. In spatial filters, the ultrathin pinhole foil is vulnerable at high power; align at low power before switching to high-power operation.

Body Material: 6061-T6 Housing Surface Finish: Black Anodized Pinhole Metal Foil Material: 300 Series Stainless Steel

JCOPTIX precision pinholes suit optical alignment, beam adjustment, imaging, and related applications. Pinhole diameters span 5-2000 μm. The metal foil is installed in an Ø25.4 mm outside-diameter aluminum-alloy housing for convenient compatibility with Ø25.4 mm optomechanics. Unhoused foils are also available for different needs. In spatial filters, the extremely thin pinhole foil is vulnerable to damage at high power. Align at low power before switching to high-power operation. Custom apertures are available alongside standard pinholes; contact support. Stainless-steel precision pinholes. Models: MPS1-5, MPS1-10, MPS1-20, MPS1-30, MPS1-40, MPS1-50, MPS1-70, MPS1-100, MPS1-150, MPS1-200, MPS1-300, MPS1-400, MPS1-500, MPS1-600, MPS1-750, MPS1-1000, MPS1-2000. Black anodizing increases absorption; aperture range 5-2000 μm; 6061-T6 aluminum-alloy housing, standard diameter Ø25.4 mm. JCOPTIX stainless-steel pinholes offer apertures of 5-2000 μm in uncoated stainless-steel foil mounted in Ø25.4 mm outside-diameter aluminum-alloy housings. They conveniently fit JCOPTIX lens mounts or 30 mm cage plates. Their ultrathin foil is vulnerable at high power in spatial filters, so align at low power before switching to high power. Unhoused stainless-steel precision pinholes. Models: MPS1-5-UN, MPS1-10-UN, MPS1-20-UN, MPS1-25-UN, MPS1-30-UN, MPS1-40-UN, MPS1-50-UN, MPS1-70-UN, MPS1-100-UN, MPS1-150-UN, MPS1-200-UN, MPS1-300-UN, MPS1-400-UN, MPS1-500-UN, MPS1-600-UN, MPS1-750-UN, MPS1-1000-UN, MPS1-2000-UN. Black anodizing increases absorption (apertures >50 μm are black); aperture range 5-2000 μm; unmounted foil, outside diameter 9.52 mm. JCOPTIX unhoused stainless-steel pinholes offer apertures of 5-2000 μm in 9.52 mm outside-diameter stainless-steel foil. Foils 30 μm thick, with apertures ≤50 μm, retain the original color on both faces; foils 50 μm thick, with apertures >50 μm, are blackened on both faces. Since the foil is only 30-50 μm thick, handle it carefully with small tweezers or pliers to avoid damage. In spatial filters, the ultrathin pinhole foil is vulnerable at high power; align at low power before switching to high-power operation.

Body Material: 6061-T6 Housing Surface Finish: Black Anodized Pinhole Metal Foil Material: 300 Series Stainless Steel

JCOPTIX precision pinholes suit optical alignment, beam adjustment, imaging, and related applications. Pinhole diameters span 5-2000 μm. The metal foil is installed in an Ø25.4 mm outside-diameter aluminum-alloy housing for convenient compatibility with Ø25.4 mm optomechanics. Unhoused foils are also available for different needs. In spatial filters, the extremely thin pinhole foil is vulnerable to damage at high power. Align at low power before switching to high-power operation. Custom apertures are available alongside standard pinholes; contact support. Stainless-steel precision pinholes. Models: MPS1-5, MPS1-10, MPS1-20, MPS1-30, MPS1-40, MPS1-50, MPS1-70, MPS1-100, MPS1-150, MPS1-200, MPS1-300, MPS1-400, MPS1-500, MPS1-600, MPS1-750, MPS1-1000, MPS1-2000. Black anodizing increases absorption; aperture range 5-2000 μm; 6061-T6 aluminum-alloy housing, standard diameter Ø25.4 mm. JCOPTIX stainless-steel pinholes offer apertures of 5-2000 μm in uncoated stainless-steel foil mounted in Ø25.4 mm outside-diameter aluminum-alloy housings. They conveniently fit JCOPTIX lens mounts or 30 mm cage plates. Their ultrathin foil is vulnerable at high power in spatial filters, so align at low power before switching to high power. Unhoused stainless-steel precision pinholes. Models: MPS1-5-UN, MPS1-10-UN, MPS1-20-UN, MPS1-25-UN, MPS1-30-UN, MPS1-40-UN, MPS1-50-UN, MPS1-70-UN, MPS1-100-UN, MPS1-150-UN, MPS1-200-UN, MPS1-300-UN, MPS1-400-UN, MPS1-500-UN, MPS1-600-UN, MPS1-750-UN, MPS1-1000-UN, MPS1-2000-UN. Black anodizing increases absorption (apertures >50 μm are black); aperture range 5-2000 μm; unmounted foil, outside diameter 9.52 mm. JCOPTIX unhoused stainless-steel pinholes offer apertures of 5-2000 μm in 9.52 mm outside-diameter stainless-steel foil. Foils 30 μm thick, with apertures ≤50 μm, retain the original color on both faces; foils 50 μm thick, with apertures >50 μm, are blackened on both faces. Since the foil is only 30-50 μm thick, handle it carefully with small tweezers or pliers to avoid damage. In spatial filters, the ultrathin pinhole foil is vulnerable at high power; align at low power before switching to high-power operation.

Soft-Edge Gradient Type: Gaussian, Sinusoidal, Sawtooth, Random Discrete, Super-Gaussian, etc. Substrate Material: Fused Silica, Silicon, Germanium Optical performance: Central Region Transmittance >92%

Definition: soft-edge apertures suppress diffraction. Unlike sharp-edged hard apertures providing '******' light blocking (source masking retained), they gradually modulate intensity at the beam edge to smooth energy distribution. Their core role is to eliminate Fresnel fringes from hard truncation, improve output uniformity, and enhance beam quality; see the output illustration. Key parameters: 1. Operating band spans 193 nm UV to 10.6 μm far IR for various lasers. 3. Clear apertures range from 3 mm-100 mm, with custom circular, square, rectangular, annular, or other shapes. 6. Processing precision: micrometer microstructure resolution with controlled soft-edge profile errors. Working principle: sharp hard apertures cause strong Fresnel diffraction, nonuniform far-field intensity, and pronounced diffraction rings that impair beam quality. Soft edges provide gradual transmission transitions, using structures such as serrated apertures or blind-spot glass apertures. The smooth transition breaks the periodic boundary conditions described at hard edges and greatly weakens diffraction modulation. The smoothed field suppresses diffraction artifacts and outputs a soft-edged, uniform-energy spot for high-power lasers and precision inspection paths. Manufacturing/customization: independently developed soft-edge apertures use the company's precision micro/nano-optical processes. An integrated in-house lithography/dry-etching platform and engineers in optical design, micro/nanofabrication, and precision inspection provide control of core manufacturing. Rectangular, serrated, randomly discrete, and other special structures can be made independently, with individual solutions tailored to gradual transmission, edge-diffraction suppression, and smooth shaping. To address hard-edge fringes, energetic edge stray light, ragged spot edges, and uneven fields, the company considers equipment aperture sizes, uniformity specifications, and beam-path layout constraints. It iteratively optimizes transition microstructures and edge attenuation slopes to maximize smoothness and diffraction suppression. High-transmission fused-silica substrates can receive antireflection or laser-damage-resistant coatings, improving transmission and damage tolerance; the source states spectral coverage from UV and visible through near/far IR. All parameters can be customized, including clear shape/dimensions, aperture, gradient profile, and attenuation slope. This serves precision beam purification in laser systems, inspection instruments, imaging, and research optical paths. Flexible delivery covers small university/research prototypes with special structures or nonstandard gradients, advanced development, and stable high-volume supply to laser/equipment manufacturers. The mature in-house line provides consistent microstructures, stable gradients, and improved stray-light suppression. Dedicated engineers give one-to-one support for integration, setup, optimization/calibration, and after-sales corrections. The company presents itself as a domestic independent supplier for precise soft-edge control and diffraction suppression. Contact it for custom work and professional, efficient technical/product support. Additional parameters: 2. Gradient types include Gaussian, sinusoidal, serrated, random discrete, and super-Gaussian profiles. 4. Substrates include fused silica, silicon, germanium, and other high-performance optical materials. 5. Central transmission >92%, low wavefront distortion, and high laser-damage threshold. Image captions: soft-edge aperture output; product photograph; soft-edge result; circular-aperture result; circular soft-edge aperture.

Sizes: 3-350mm Clear Aperture: central 90% of diameter Flatness: 1/10th wave

Sizes: 3-350mm Clear Aperture: central 90% of diameter Flatness: 1/10th wave Angle Tolerance: 3 arcsec Surface Quality: 20-10 scratch-dig Shapes: Right angle, Penta, Dove, Porro, Rhomboid,Coner cube, Equilateral,right angle roof and special shapes Material:Optical glasses and Fused Silica