EBD SLED Driver Boards

Refractive Index 1.44; 45-60 cps Viscosity at 25°C Norland Optical Adhesive 144 is clear liquid adhesive that will cure when exposed long wavelength ultraviolet light. NOA 144 is recommended for bonding glass to glass. Adhesion is also good to cellulose acetate butyrate. NOA 144 is cured by ultraviolet light between 315 and 395 nm. Peak absorption is 365nm. Full cure requires 6 Joules/cm2. The adhesive exhibits oxygen inhibition and must be cured under an inert atmosphere if used as a coating to assure surface is tack free.Typical Properties of NOA 144 Shore D Hardness 65 Color Clear  Keep NOA 144 in a cool (5-22°C) dark place. If refrigerated, allow the adhesive to come to room temperature before using.

4-16 Channels; Dynamic Range 25 dB; Sampling Rate 100-1,000 Hz; Wavelength Range 1460-1620 nm; Wavelength Accuracy 1, 2 pm; Wavelength Stability 1, 3 pm; Optical Fiber Connectors LC/APC Luna’s HYPERION si255 is an industrial-grade, fan-less fiber optic sensing interrogator. Featuring both static and dynamic full spectrum analysis, Luna’s HYPERION si255 robust, turn-key interrogator provides long-term, reliable and accurate measurements of nearly 1000 of Fiber-Bragg Gratings (FBGs) or extrinsic Fabry-Perot (FP) sensors on 16 parallel, 160 nm wide channels. The si255 interrogator features an all new, high-power, low-noise, ultra-wide swept wavelength laser with guaranteed absolute accuracy on every scan which is realized with Luna’s patented Fiber Fabry-Perot filter and wavelength reference technology. The all new HYPERION platform, on which the si255 is based, features new and groundbreaking capabilities including high-performance on-board DSP and real-time FPGA processing. This enables rapid full-spectrum data acquisition and flexible peak detect algorithms of Fiber Bragg Gratings (FBG), Long Period FBGs (LPG), Fabry-Perot (FP) and Mach-Zehnder (MZ) sensors with low-latency access to data for closed-loop feedback applications. HYPERION static full-spectrum optical interrogators measure the full optical spectrum of the optical sensor signals and can be equipped with a NIST absolute reference cell. The performance of the static interrogator module is characterized by high dynamic range and high absolute wavelength accuracy. The HYPERION platform is now compatible with the ENLIGHT sensing analysis software, which provides a single suite of tools for data acquisition, computation, and analysis of optical sensor networks. More information on the ENLIGHT software can be found in the downloadable datasheet. The HYPERION platform also includes a comprehensive fully supported application programing interface (API) and LabVIEW, Python, Matlab, and C++ examples. Whether an application requires static or dynamic real-time acquisition or periodic monitoring, Luna offers the right instrument for the job. Proven to be an essential element in reliable, long-term sensing measurement installations, Luna’s sensing instruments have been installed in hundreds of challenging applications all over the world, including large-span bridges in China, earthquake monitors in California, oil platforms in Brunei and marine vessels in the North Sea. Key Features: Full Spectrum at 1 kHz With 160 nm on up to 16 Parallel Channels Simultaneously, Eliminating the Need for Optical Switches Dynamic and Absolute Measurements of Fiber Bragg Gratings (FBGs), Long Period FBGs (LPGs), Fabry-Perot (FP) and Mach-Zehnder (MZ) Optical Sensors From Detailed Optical Spectrum Single and Continuous 25 dB Dynamic Range, Available to Each Sensor on Each Channel, Independent of Differential System Losses Modes: Enhanced Visibility (10 Hz), Standard (100 or 1,000 Hz), High Speed (5,000 Hz) Number of Parallel Channels: 4, 8, 16 Wavelength Range: 1500 to 1620 nm Wavelength Accuracy / Stability: 1 pm/1 pm, 2 pm/3 pm Optical Fiber Connectors: LC/APC Data Verification Key Guarantees only Valid Output. Each Data Set is Calibrated and Verified Against any Potential Sources of System Error (Coming Soon) Proven Reliability and Longevity of the Luna Swept Wavelength Source, With Over 100 Million Hours Logged Since 2000 Dimensions: 307 x 274 x 69 mm Applications: Fiber Optic Sensing of – Oil & Gas; Medical Devices; Industrial Measurements; Energy; Structures; Security; Aerospace

Single Channel; Fiber Type Step Index Multi Mode; Core Size 200 to 600 µm; Flange Options Bolt, Conflat & ISO Klein Flange; Connector Type SMA905 Fiberguide’s VFT series of fiber vacuum pressure feedthroughs is designed to allow optical fibers to penetrate a pressure vessel without compromising the integrity of the vacuum. The VFT series can be configured as stand-alone feedthroughs or integrated into cable assemblies as needed. The VFT series of vacuum feedthroughs are ideal for laser power delivery or optical sensing applications that must be conducted in a pressure or vacuum chamber. Optional specifications for the VFT series of vacuum feedthroughs are pigtail or bundle configurations, alternate connectors or fiber types as well as variants for high or low temperature. Key Features: Fiber Type: Step Index Multimode Core Sizes: 200, 400, 600 µm Wavelengths: 190 to 1250 (High OH), 300 to 2400 nm (Low OH ) Numerical Aperture (NA): 0.22 Connector Options: SMA905 Flange Options: Bolt Style, ConFlat Flange, ISO Klein Flange (KF) Bulkhead Temperature Range: -40 to +125 °C Vacuum Rating: 1 x 10-9 Torr Applications: Laser Power Delivery or Optical Sensing in a Pressure or Vacuum Chamber

1260-1650 nm; IL 0.05 dB; PMD 0.05 ps; AL <0.01, <0.05 dB; RL >65 dB; Max. Rise & Fall Time 30 µs General Photonics’ MPC all fiber polarization controller module is packaged in a low-profile, 16 mm high enclosure, suitable for system integration and mounting on a PCB. The module’s low height is especially advantageous for integration in test equipment, fiber sensors, fiber lasers and optical network modules. Available with three (-3x) and four channels (-4x), the MPC polarization controller module features an all-fiber design with inherently low loss, minimal activation loss and minimal back reflection. A special athermal design leads to stable operation over a wide range of temperatures (-25 to +80 °C). Combined with General Photonics’ miniature piezo driver card, it can be controlled either by a digital or analog signal to obtain any desired polarization output from an arbitrary input polarization state. Key Features: OEM Packaging All-fiber Design Low Intrinsic Insertion Loss: 0.05 dB Low Back Reflection – Return Loss: >65 dB Fast Response – Maximum Rise and Fall Time: 30 µs Operating Wavelength Range: 1260 to 1650 nm Maximum Activation Loss (AL): 0.01, 0.05 dB Polarization Mode Dispersion (PMD): 0.05 ps Compact Size – Dimensions: 65.5/83 x 20.3 x 16 mm Applications: Polarization Stabilization; Compensate PMD in Fiber Sensing Systems; Polarization Demultiplexing; Fiber Sensor; Fiber Laser; Testing Equipment

Output Current LD 0.25-1.5 A; Output Current TEC ±4 A; Chassis Mount; Compatible with Butterfly Type 1 & Type 2 Lasers; Current Stability <0.1%   Maiman Electronics’ SF8XXX series of laser diode drivers and TEC temperature controllers are suitable for driving fiber coupled laser diodes in a butterfly package with 10 or 14 pins. SF8XXX series drivers are available with pinouts for Type 1 (Pump) or Type 2 (Telecom, SF8XXX-T) butterfly laser diodes. The SF8XXX drivers include highly stable (±0.01 A) current sources for the laser diode and a thermoelectric Peltier cooler (TEC). The integrated temperature controller keeps the temperature on the Peltier element with high precision within ±0,01 °C. The laser diode driver circuit of the SF8XXX series is a non-isolated low drop-out (LDO) regulator with constant current output, producing current with high stability and low ripple. The TEC driver circuit is a non-isolated DC/DC converter, producing low current ripple. Additional features of the SF8XXX series include an adjustable TEC output current limit and an integrated self-adjusting PID controller, providing optimal temperature regulation. All SF8XXX can be controlled by analog signal or digital signals and switches on the board. The SF8xxx series drivers are housed in a 61 × 101.6 mm enclosure with aluminium base plate to aid thermal dissipation from the laser diode. SF8xxx series drivers can be mounted on any surface that is thermally conductive enough to dissipate the laser diode’s power loss. The laser diode mount is located on the board – either with landing pads for soldering a butterfly laser diode directly into driver board or with an integrated mounting Azimuth socket for butterfly packaged devices (-ZIF types). Key Features: All-in-One Current Source, Temperature Controller and Mount (ZIF-10/ZIF 14 types with Azimuth ZIF Socket) for Butterfly Laser Diodes Compatible with Type 1 Butterfly 10-pin, Type 1 / Type 2 Butterfly 14-pin Laser Diode (Depending on Model) Low Laser Diode Current Ripple: ≤10 µA Laser Diode Current Stability <0.1% Integrated PID Controller, Does Not Require Setup Soft-Start Current Ramp, Current Limit, Temperature Limit for Laser Diode Protection Free Software NTC Thermistor Input Analog Control Signal / RS-232 Possibility to Calibrate Current Within 5% Applications: Supplying Laser Diodes in Butterfly Package; Laser Pumping; Laser Spectroscopy; Laboratory Test Set-ups

400-1700 nm; Power 1.5-30 mW; Bandwidth 3-160 nm; Current 60-600 mA; Beam Shape Gaussian, Flat Top; Package TO-9, TO-56, 5-BTF, 14-BTF, TOSA; Cooled or Uncooled; With or Without Monitor Photodiode With the EXS series, EXALOS offers a wide variety of standard superluminescent light emitting diode (SLED or SLD) modules covering near-infrared and RGB (red, green, blue) ranges. EXS series SLED modules are available at different wavelengths ranging from 400 to 1700 nm, with different output power and bandwidth values.EXALOS’ high-performance SLEDs come in various packages including cooled 14-pin dual-in-line (DIL) and butterfly package, cooled and uncooled 5-pin butterfly packages or low-cost uncooled TOSA and TO-56 packages.In addition to the standard product range, EXALOS can also offer SLED devices with custom optical performance and custom housing or fibers. Please contact the AMS Technologies SLED experts to discuss your custom SLED module solution tailored to your project’s requirements.Key Features: Wavelength Range: 400 to 1700 nm Power: 1.5 to 30 mW Bandwidth: 3 to 160 nm Current: 60 to 600 mA Beam Shape: Gaussian, Flat Top Package: TO-9, TO-56, 5-BTF, 14-BTF, TOSA Cooled or Uncooled Versions With or Without Monitor Photodiode Wavelength Power Bandwidth Current Spectral Shape Cooled Package Type MPD (y/n) Fiber Type Part Number 405 nm 10 mW 4 nm 110 mA Gaussian no TO-56 no none EXS210015-02 405 nm 2 mW 3 nm 100 mA Gaussian yes 14-BTF no SMF EXS210084-01 450 nm 10 mW 5 nm 180 mA Gaussian no TO-56 no none EXS210014-01 450 nm 5 mW 6 nm 160 mA Gaussian yes 14-BTF no SMF EXS210099-03 510 nm 6 mW 10 nm 600 mA Gaussian no TO-9 no none EXS210115-00 510 nm 1,5 mW 10 nm 500 mA Gaussian yes 14-BTF no SMF EXS210118-01 635 nm 10 mW 6 nm 60 mA Gaussian no TO-56 no none EXS210105-02 635 nm 10 mW 5 nm 60 mA Gaussian no TO-56 no none EXS210131-01 635 nm 3 mW 6 nm 60 mA Gaussian yes 14-BTF no SMF EXS210098-01 650 nm 4 mW 10 nm 100 mA Gaussian no TO-56 yes none EXS210035-02 650 nm 3 mW 6 nm 100 mA Gaussian yes 14-BTF yes SMF EXS210033-03 650 nm 10 mW 6 nm 60 mA Gaussian no TO-56 yes none EXS210030-03 650 nm 3 mW 6 nm 100 mA Gaussian yes 14-BTF yes PMF EXS210144-01 750 nm 5 mW 20 nm 150 mA Gaussian yes 14-BTF yes SMF EXS210025-01 750 nm 2 mW 20 nm 140 mA Gaussian no TOSA yes SMF EXS210065-01 750 nm 15 mW 20 nm 140 mA Gaussian no TO-56 yes none EXS210017-01 790 nm 5 mW 20 nm 120 mA Gaussian yes 14-BTF yes SMF EXS210060-01 790 nm 15 mW 20 nm 120 mA Gaussian no TO-56 yes none EXS210067-03 800 nm 10 mW 40 nm 160 mA Flat top yes 14-BTF yes SMF EXS210111-01 820 nm 2 mW 25 nm 120 mA Gaussian no TOSA yes SMF EXS210036-01 820 nm 3 mW 25 nm 120 mA Gaussian no 5-BTF no SMF EXS210119-01 820 nm 15 mW 25 nm 120 mA Gaussian no TO-56 yes none EXS210086-01 830 nm 12 mW 20 nm 200 mA Gaussian yes 14-BTF yes SMF EXS210005-02 840 nm 15 mW 48 nm 180 mA Flat top yes 14-BTF yes SMF EXS210090-01 840 nm 2 mW 50 nm 150 mA Flat top no TOSA yes SMF EXS210037-01 840 nm 10 mW 50 nm 150 mA Flat top no TO-56 yes none EXS210040-01 840 nm 10 mW 46 nm 160 mA Flat top yes 14-BTF yes SMF EXS210006-03 840 nm 6 mW 40 nm 120 mA Flat top yes 14-BTF yes SMF EXS210106-01 840 nm 6 mW 50 nm 120 mA Flat top yes 14-BTF yes SMF EXS210022-03 850 nm 5 mW 35 nm 250 mA Gaussian yes 14-BTF no SMF EXS210031-02 850 nm 5 mW 55 nm 150 mA Flat top yes 14-BTF yes SMF EXS210068-02 880 nm 5 mW 65 nm 200 mA Flat top yes 14-BTF yes SMF EXS210018-01 880 nm 12 mW 70 nm 200 mA Flat top yes 14-BTF yes SMF EXS210088-02 910 nm 15 mW 40 nm 200 mA Gaussian yes 14-BTF yes SMF EXS210120-01 1050 nm 10 mW 70 nm 200 mA Flat top yes 14-BTF yes SMF EXS210009-01 1050 nm 20 mW 60 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210063-02 1060 nm 20 mW 70 nm 350 mA Flat top yes 14-BTF yes SMF EXS210010-01 1070 nm 10 mW 90 nm 300 mA Flat top yes 14-BTF yes SMF EXS210007-01 1230 nm 10 mW 45 nm 400 mA Gaussian yes 14-BTF yes SMF EXS210079-01 1270 nm 25 mW 30 nm 450 mA Gaussian yes 14-BTF yes SMF ESL2720-2113 1280 nm 8 mW 80 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210049-02 1290 nm 2 mW 60 nm 200 mA Gaussian yes 14-BTF yes SMF EXS210034-02 1300 nm 6 mW 120 nm 450 mA Flat top yes 14-BTF yes SMF EXS210057-01 1300 nm 20 mW 50 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210076-02 1300 nm 15 mW 70 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210046-02 1300 nm 10 mW 110 nm 500 mA Flat top yes 14-BTF yes SMF EXS210045-02 1300 nm 10 mW 40 nm 250 mA Gaussian yes 14-BTF yes PMF EXS210072-01 1300 nm 10 mW 40 nm 250 mA Gaussian yes 14-BTF yes SMF EXS210032-02 1300 nm 12 mW 40 nm 200 mA Gaussian no TO-56 yes none EXS210041-02 1300 nm 3 mW 40 nm 200 mA Gaussian no TOSA no SMF EXS210028-02 1310 nm 30 mW 60 nm 600 mA Gaussian yes 14-BTF yes SMF EXS210047-02 1310 nm 30 mW 60 nm 600 mA Gaussian yes 14-BTF yes PMF EXS210087-01 1310 nm 20 mW 90 nm 600 mA Flat top yes 14-BTF yes SMF EXS210074-02 1350 nm 25 mW 50 nm 400 mA Gaussian yes 14-BTF yes SMF EXS210020-01 1380 nm 10 mW 40 nm 250 mA Gaussian yes 14-BTF yes SMF ESL1410-2113 1450 nm 5 mW 80 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210103-01 1480 nm 15 mW 40 nm 450 mA Gaussian yes 14-BTF yes SMF ESL4820-2113 1520 nm 8 mW 60 nm 250 mA Gaussian yes 14-BTF yes SMF EXS210038-01 1520 nm 2 mW 60 nm 200 mA Gaussian no TOSA no SMF EXS210029-01 1520 nm 6 mW 60 nm 200 mA Gaussian no TO-56 no none EXS210042-01 1530 nm 2 mW 100 nm 550 mA Gaussian yes 14-BTF yes SMF EXS210095-01 1550 nm 30 mW 40 nm 500 mA Gaussian yes 14-BTF yes SMF EXS210073-01 1550 nm 12 mW 40 nm 250 mA Gaussian yes 14-BTF yes PMF EXS210094-01 1550 nm 12 mW 40 nm 300 mA Gaussian yes 14-BTF yes PMF EXS210070-01 1550 nm 15 mW 45 nm 300 mA Gaussian yes 14-BTF yes SMF EXS210069-01 1550 nm 20 mW 60 nm 500 mA Flat top yes 14-BTF yes SMF EXS210059-01 1550 nm 6 mW 60 nm 200 mA Gaussian no TO-56 no none EXS210085-01 1550 nm 5 mW 60 nm 250 mA Gaussian yes 14-BTF yes SMF EXS210019-03 1550 nm 2 mW 60 nm 200 mA Gaussian no TOSA yes SMF EXS210071-02 1550 nm 15 mW 90 nm 600 mA Gaussian yes 14-BTF yes SMF EXS210108-01 1550 nm 10 mW 90 nm 600 mA Gaussian yes 14-BTF yes SMF EXS210048-03 1550 nm 10 mW 60 nm 300 mA Flat top yes 14-BTF yes SMF EXS210054-01 1550 nm 4 mW 150 nm 350 mA Flat top yes 14-BTF yes SMF EXS210066-02 1570 nm 10 mW 65 nm 250 mA Flat top yes 14-BTF yes SMF EXS210055-01 1580 nm 20 mW 60 nm 500 mA Flat top yes 14-BTF yes SMF EXS210062-01