ATC-RS-01 Cleaning Tools for Optics

Cleaning Tools for Optics;OPTIPOP;Cassette Grip;Single-Core;Multi-Core;MU;LC;SC;FC;ST;MT;MPO;MTRJ

Refractive Index 1.56; 250 cps Viscosity at 25°C Norland Optical Adhesive 83H ("NOA83H") is a single component liquid adhesive that cures in seconds to a tough, hard polymer when exposed to ultraviolet light. It is recommended as an extremely fast and efficient way to precisely bondoptical components. In addition to UV light, heat can also be usedto cure this one part adhesive.The outstanding characteristic of this material is its extremely fast cure. Thin films can be initially set in under 10 seconds and thick films in 20 seconds using the light sources listed below. It is also extremely stable when not exposed to UV light. NOA 83H will not gel up in dispenser tips or cure before you want it to.Typical Properties of NOA 83H Solids 100% Elongation at Failure 30% Modulus of Elasticity (psi) 160,000 Tensile Strength (psi) 3,500 Hardness - Shore D 85 Shelf life of the liquid is at least 4 months from the date of shipment if stored in a cool (5-22° C), dark place in the original container. If refrigerated, allow the adhesive to come to room temperature prior to use.

Cleaning Tools for Optics;NEOCLEAN;Pen;Single-Core;MU;LC

Cleaning Tools for Optics;OPTIPOP;Cassette Grip;Single-Core;Multi-Core;MU;LC;SC;FC;ST;MT;MPO;MTRJ

Cleaning Tools for Optics;NEOCLEAN;Simple;Single-Core; Multi-Core;MU;LC;SC;FC;ST;MT;MPO;MTRJ

Attachment;POP311/ ATP-3200/ ATP-3000

Fused Silica; Wavelength Range Customer Specified; Finesse Customer Specified; FSR Customer Specified; AR-coated; Dia. 14-203.2 mm; Clear Aperture 4-150 mm LightMachinery’s series of tunable air spaced etalons is manufactured from Fused Silica using the company’s patented fluid jet polishing (FJP) technology – allowing the adjustment of the etalon’s shape and flatness to within a few nanometers. These tunable air spaced etalons are available as 14 mm diameter, 4 mm aperture, single piezo tube (OP-1986) or larger 3-piezo tunable etalons (OP-740xT) with diameters of 50.8 to 203.2 mm and 30 to 150 mm aperture. Wavelength range, finesse, free spectral range (FSR) and design details can be realized based on customer requirements. For the OP-1986 single piezo tube tunable etalon, a dedicated driver and mount Kit (OP-7934) is available that includes everything required to drive the single-tube piezo including power supply, driver with computer interface, cables, connectors and a mount that adapts the single tube piezo etalon to a standard 25.4 mm (1") diameter optical mount – made from Delrin and aluminium. There are a number of ways to tune etalons including tilting the entire etalon, moving the mirrors and changing the index of the medium (pressure, temperature, electrostatic). Tilt tuning is a simple tuning technique. As the etalon is tilted, the FSR changes with the cosine of the angle. Piezo-electric tuning of an air spaced etalon is usually what is meant by the phrase "tunable etalon". This technique can tune the etalon quickly by changing the size of the air gap. By changing the length of the air gap by half the wavelength of the light, the transmission peak moves one full FSR. So, if an etalon is used at 532 nm then only 266 nm of motion is required to tune the etalon. Small piezo elements (like the OP-1986 single piezo tube tunable etalon) can easily move through 10 µm. Larger OP-740xT piezo tunable etalons are made using three piezo elements. Although these etalons are more complex to control, they have the big advantage that the piezo elements can be subtly tuned to eliminate any residual tilt error between the two mirrors and improve the finesse. Etalons are optically transparent, flat components with very precisely parallel reflecting surfaces. While solid etalons consist of solid plates of optical material, air spaced etalons are formed by two mirrors with an air gap between them, reducing the problem of temperature dependence. Due to their construction, air spaced etalons are significantly more complex. The outside surfaces of the end mirrors also need to be wedged and AR-coated to avoid reflections from these surfaces causing additional unwanted etalon effects. Sometimes you need something special – if you are looking for a customized tunable air spaced etalon that exactly meets your specific requirements, please get in touch with the AMS Technologies etalon experts. Our supplier LightMachinery is extremely experienced with specifying, designing and manufacturing custom etalons using the company’s patented fluid jet polishing (FJP) technology. We are looking forward to discussing your customized etalon solution! Fluid jet polishing (FJP) systems use a fine stream of slurry to accurately remove nanometers of material from an optical surface. Many years of refining this computer controlled polishing technology have enabled LightMachinery to use FJP for the adjustment of the shape and flatness of optical components such as etalon mirrors to within a few nanometers as well as the production of very thin components such as wafers and thin etalons that are impossible to accurately polish using conventional technology. Key Features: Piezo Tunable Etalons Etalon Material: Fused Silica (Optical) Gap: Customer Specified 5 µm to >200 mm Gap Adjustment: Tunable From -4 to +12 µm (-30 to 150 V) Maximum Tuning Speed: ~1 KHz For Large Moves, ~10 KHz For Small Moves (One FSR) Wavelength Range: Customer Specified Finesse: Customer Specified Free Spectral Range, FSR: Customer Specified AR-coated: Less Than 0.5% Reflection Diameter: 14 mm (OP-1986), 50.8 to 203.2 mm (2” to 8”, OP-740xT) Clear Aperture: 4 mm (OP-1986), 30 to 150 mm (OP-740xT) Applications: Spectroscopy; Interferometers; Wavelength Measurement; Fine-structural Investigation of Spectral Lines

500 to 1000 nm; Refractive Index Accuracy ±0.0001; Spatial Resolution 500 nm; Fiber Type SM, MM, PM, Other; Fiber Diameter 40 to 400 µm Interfiber Analysis’ IFA-100 multi-wavelength interferometric optical fiber analyzer can measure the refractive index profile of an optical fiber without the need for a cleave at wavelengths from 375 to 2000 nm. By scanning the fiber from the side, the IFA-100 unit allows for scanning and measuring the optical refractive index profile (RIP) along the fiber’s length with sub-micron spatial resolution. The measurement is independent of cumbersome fiber preparation like cleaving and allows for measuring the evolution of the refractive index profile over a given length of fiber. The equipment uses a broadband light source and can determine the refractive index profile at any wavelength between visible and near infrared. The refractive index or index of refraction (IOR) is a property of any material. For optically transmitting materials, such as for fibers and waveguides, it is reflected in the reduced speed of light when travelling through any media other than vacuum. Fibers and waveguides use a distribution of the IOR within their cross section to guide and reflect light, and knowledge of this distribution allows many other critical performance parameters to be calculated, such as mode fields, group and phase propagation constants and fiber dispersion. Based on Interfiber Analysis’ IFA-100 multi-wavelength interferometric optical fiber analyzer, AMS Technologies offers refractive index measurement services for product development, incoming inspection and forensic analysis on optical fibers. Key Features: Multi-wavelength: 500 to 1000 nm No Cleave Required Sub-µm Spatial Resolution: About 500 nm Applicable to Any Fiber Type Fast Measurement Refractive Index Accuracy: ±0.0001 Fiber Diameter: 40 to 400 µm Fiber Material: Silica Glass, Non-silica Glass, Plastic Concentricity Error Measurement: ±200 nm Core Non-circularity Error Measurement: ± 0.4% Fiber Type: Single Mode (SM), Multi Mode (MM), Polarization Maintaining PM), Micro-Structured (PCF), Multicore, Rare-earth, Cladding-pumped, Large Mode Area (LMA), Low Bend Loss, High-Δ, etc. Applications: Measuring Splices, Tapers or Couplers of Any Fiber Type; Test and Measurement; Telecommunication; Lasers

Cartridge;NEOCLEAN;Consumable