17OPO-1-50 S MID-IR (1700 nm) Tunable OPO Source

The range of powers available goes from 410 to 3850 W, covering the majority of applications for cooling electric enclosures in an extremely compact package. Protection against condensateGreat attention is paid to the protection of the electric cabinet against condensate. To that purpose a small stainless steel tank complete with a service discharge pipe and an emergency discharge pipe is provided inside the cooling unit to collect the condensate and to drain it out. Electronic regulation controlAll TEXA air conditioning units are supplied with electronic adjustment as standard. Quick installationInstallation is very quick thanks to the simplicity of the holes to be drilled on the enclosure panel and to the fixing system, whose elements are all included in the cooling unit packaging. They all lend themselves to easy and safe electrical connection by means of rapid connectors which are inserted into the back of the unit. Minimised maintenanceAll the cooling units feature heat exchange surfaces designed to prevent clogging by solid contaminants in the ambient air. They maintain high efficiency even when the environmental conditions are bad, thus reducing maintenance work drastically meaning that the cooling unit can work without a filter on the external air intake. Optimum enclosure protectionThanks to the special internal configuration that keeps the flow of outside air separated and sealed from the inside air, and to the self-adhesive coupling seal, the DEK cooling units allow the enclosure to maintain an IP54 protection level. Safe guarding the environmentGreat attention is paid to limiting the noise level, being one of the most important criteria when designing the DEK cooling units. They are, in fact, designed to minimise disturbance caused by noise to ensure a quiet working place. To protect the environment all the cooling units use the CFC-free, ozonefriendly refrigerant R134a. Supply voltageThe DEK cooling units are available for the main AC supply voltage: 230V single-phase, 400-440V two-phase (in the case of voltage between lines when there is no neutral), 115V single-phase and 400V three-phase, all bifrequency 50-60 Hz. On request and for substantial quantities they can also be available with other voltages not given in the catalogue. PaintingRAL 7035 orange peel effect is the standard colour. Epoxy powder paint is used. On request other colours are available as well as stainless steel versions. KEY FEATURES: Cooling units for roof mounting Cooling capacity from 410 W up to 3850 W Available for different voltages Advantages: quick assembly, reliability and minimised maintenance

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    

OFDR Technology; Spatial Resolution 20 µm; Max. Device Length 20, 40 m; Center Wavelength 1546.69 nm; Wavelength Range 40 nm; Dynamic Range 15, 70 dB The Luna 6415 lightwave component analyzer is a fast and simple-to-use analyzer for passive optical components and modules, extending Luna’s industry-leading optical frequency domain reflectometry (OFDR) platform to manufacturing test and quality control applications. Unlike traditional passive component testers, Luna 6415 measures and analyzes the insertion loss (IL) and return loss (RL) distribution as well as length with a single instrument, working in either reflection or transmission. The Luna 6415 lightwave component analyzer utilizes optical frequency domain reflectometry (OFDR) technology to measure backscattered or transmitted light as a function of distance. The system features extremely high sensitivity, 20 μm spatial sampling resolution and very fast scanning for high test throughput, making it an ideal testing tool for photonic integrated circuits (PICs) and silicon photonics. By integrating both reflection and transmission measurements, Luna 6415 reduces the cost and complexity of test while increasing throughput and provides more complete test coverage of your component. The Luna 6415 lightwave component analyzer further simplifies your manufacturing test with an integrated tunable laser source , automated IL and RL calculations, self-calibration and very high scanning speeds for greater test throughput. Key Features: Return Loss (RL) and Insertion Loss (IL) Analysis Trace Distributed Return Loss (RL) Over Length of Optical Path – Easily Measure Waveguide Scattering Spectral Analysis of Return Loss (RL) and Insertion Loss (IL) Detect and Precisely Locate Reflective Events and Measure Path Length Speed, Resolution and Accuracy for Optimizing Production Test High Spatial Sampling Resolution: 20 μm Measurement Range: 20 m Scan/Acquisition Rate: 6 Hz Maximum Device Length: 20 m (Reflection), 40 m (Transmission) Wavelength Range: 40 nm Center Wavelength: 1546.69 nm Maximum Optical Power: 5 mW Dynamic Range: 70 dB (RL Measurement), 15, 70 dB (IL Measurement, Reflection / Transmission Mode) Return Loss Measurement Sensitivity: -135 dB Measurement Resolution: ±0.1 dB Applications: Spatial RL Testing; Automated Insertion Loss (IL) Test and Analysis; Skew Measurement With Sub-picosecond Resolution; PLCs, Waveguide Devices, AWGs, ROADMs, etc.; Couplers, Switches, Beamsplitters

Active Area Diameter 0.08-1.1 mm; Responsivity 90- 3,000 kV/W; NEP 10-220 fW/√Hz; Package TO-8, TO-8 Flange, Custom; System Bandwidth 50, 200 MHz Excelitas’ hybrid optical APD receiver modules are comprised of a photodetector (PIN or APD) and a transimpedance amplifier in the same hermetically sealed package. Having both an amplifier and photodetector in the same package allows low-noise pickup from the surrounding environment and reduces parasitic capacitance from interconnect allowing lower-noise operation. The C30950EH is a silicon avalanche photodiode (Si APD) amplifier module with 50 MHz system bandwidth and includes Excelitas’ C30817 silicon avalanche photodiode (APD) . With a useful diameter of 0.8 mm, the C30950EH provides good response between 400 and 1100 nm and is supplied in a modified 12-lead TO-8 package. The C30950EH is the cost-effective, pin-compatible alternative to the C30659 series employing a bipolar amplifier. The C30659 series includes a silicon (Si) or InGaAs avalanche photodiode (APD) with a hybrid preamplifier, in the same hermetically sealed TO-8 package, to allow for ultra-low noise operation, and features an inverting amplifier design with an emitter follower used as an output buffer stage. The Si APDs used in these devices are the same as used in Excelitas’ C30817EH, C30902EH , C30954EH and C30956EH products , while the InGaAs APDs are used in Excelitas’ C30645EH and C30662EH products . These detectors with 50 or 200 MHz system bandwidth provide very good response between 830 and 1550 nm and very fast rise- and fall-times at all wavelengths. The preamplifier section of the module uses a very low-noise GaAs FET front end designed to operate at higher transimpedance than Excelitas’ standard C30950 Series. The C30659-UV-1 includes a UV-enhanced silicon avalanche photodiode (Si APD) providing very good response between 400 nm and 950 nm. The LLAM series of fully RoHS-compliant APD modules features an avalanche photodiode chip, thermoelectric (TE) cooler, and preamplifier, all in a single hermetically-sealed, modified 12-lead TO-66 flange package. The modules are easy to install and offer additional heat sinking. The use of a TE-cooler ensures lower noise and constant responsivity over a +5 to +40 °C ambient temperature range. The LLAM Series modules with 50 or 200 MHz system bandwidth are designed for the detection of high-speed, low-light analog signals. Applications: Laser Range Finder; Video Scanning Imagers; High-speed Analytical Instrumentation; Free-space Communication; UV-VIS-NIR Light Sensing; Distributed Temperature Sensing Part Number Detector Active Diameter Bandwidth Responsivity NEP Output Voltage Swing, 50 Ω Package Download         500 nm 900 nm 1060 nm 1550 nm         C30659-UV-1 UV-Enhanced 1.1 mm 50 MHz 3,000 kV/W - - - 10 fW/√Hz 0.9 V TO-8 Datasheet C30659-900-R5BH C30902 0.5 mm 200 MHz - 400 kV/W - - 40 fW/√Hz 0.9 V TO-8 Datasheet C30659-900-R8AH C30817 0.8 mm 50 MHz - 3,000 kV/W - - 12 fW/√Hz 0.9 V TO-8 Datasheet C30659-1060-R8BH C30954 0.8 mm 200 MHz - 370 kV/W 200 kV/W - 100 fW/√Hz 0.9 V TO-8 Datasheet C30659-1060E-R8BH C30954 0.8 mm 200 MHz - 370 kV/W 200 kV/W - 100 fW/√Hz 0.9 V TO-8 Datasheet C30659-1060-3AH C30956 3 mm 50 MHz - 450  kV/W 280 kV/W - 90 fW/√Hz 0.9 V TO-8 Datasheet C30659-1550-R08BH C30645 0.08 mm 200 MHz - - - 90 kV/W 220 fW/√Hz 0.9 V TO-8 Datasheet C30659-1550E-R08BH C30645 0.08 mm 200 MHz - - - 90 kV/W 220 fW/√Hz 0.9 V TO-8 Datasheet C30659-1550-R2AH C30662 0.2 mm 50 MHz - - - 340 kV/W 130 fW/√Hz 0.9 V TO-8 Datasheet C30659-1550E-R2AH C30662 0.2 mm 50 MHz - - - 340 kV/W 130 fW/√Hz 0.9 V TO-8 Datasheet C30919E C30817 0.8 mm 40 MHz - 1,000 kV/W 250 kV/W - 20 fW/√Hz 0.7 V TO, 1 in - C30950EH C30817 0.8 mm 50 MHz - 560 kV/W 140 kV/W - 27 fW/√Hz 0.7 V TO-8 Datasheet LLAM-1550-R08BH C30645 0.08 mm 200 MHz - - - 90 kV/W 220 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1550E-R08BH C30645 0.08 mm 200 MHz - - - 90 kV/W 220 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1550-R2AH C30662 0.2 mm 50 MHz - - - 340 kV/W 130 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-900-R5BH C30902 0.5 mm 200 MHz - 400 kV/W - - 40 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1550E-R2AH C30662 0.2 mm 50 MHz - - - 340 130 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1060-R8BH C30954 0.8 mm 200 MHz - 370 kV/W 200 kV/W - 50 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1060E-R8BH C30954 0.8 mm 200 MHz - 370 kV/W 200 kV/W - 50 fW/√Hz 0.9 V TO-8 FLANGE Datasheet LLAM-1060-R8BH-FC C30954 0.8 mm 200 MHz - 370 kV/W 200 kV/W - 55 fW/√Hz 0.9 V TO-8 FLANGE+FC Datasheet HUV-1100BGH UV-100 2.5 mm 0.001 MHz - 130 MV/W - - 30 fW/√Hz 5 min CUSTOM - HUV-2000BH UV-215 5.4 mm 0.001 MHz - 130 MV/W - - 70 fW/√Hz 6 min CUSTOM - HeliX-902-200 C30902 0.5 mm 200 MHz - 650 kV/W - - 50 fW/√Hz 1  V CUSTOM - HeliX-954-200 C30954 0.8 mm 150 MHz - 650 kV/W 360 kV/W - 110 fW/√Hz 1  V CUSTOM -

PM or SM Splitters/Combiners; 1550 nm, Other; Splitting Ratio 50/50-90/10; PDL ±0.25 dB; Directivity >50 dB OZ Optics’ fiber optic beamsplitters are used to divide light from one fiber into two or more fibers. Light from an input fiber is first collimated, then sent through a beam-splitting optic to divide it into two. The resultant output beams are then focused back into the output fibers. Both 1xN and 2xN splitters can be constructed in this fashion with as many as eight or more outputs, with both low return losses and low insertion losses. Standard parts available in this series are FOBS-12P (1x2) and FOBS-22P (2x2) pigtail-style splitters, FOBS-12 (1x2) and FOBS-22 (2x2) receptacle-style splitters, as well as LDBS-12P (pigtail-style) and LDBS-1 (receptacle-style) laser diode to fiber splitters, and finally ULBS-12P (pigtail-style) and ULBS-1 (receptacle-style) laser to fiber splitters This design is extremely flexible, allowing to use different fiber types on different ports, and different beamsplitter optics inside. Custom designs combining circulators, polarizing splitters and non-polarizing splitters in the same package are routinely manufactured. Splitters can be made with either fibers permanently attached to each port (pigtail style) or with receptacles on each port that one can plug your fiber into (receptacle style). OZ Optics can also build source to fiber couplers with built-in beamsplitters for either laser or laser diode sources. Contact AMS Technologies for details. If size is a concern, we recommend that you consider OZ Optics’ miniature line of splitters. Within OZ Optics’ series of beamsplitters and combiners, the two most common types of splitters offered are polarizing beamsplitters and polarization maintaining (PM) beamsplitters. Polarizing beamsplitters split incoming light into two orthogonal states. They can also be used to combine the light from two fibers into a single output fiber. When used as a beam combiner, each input signal will transmit along a different output polarization axis. PM splitters use a partially reflecting mirror to transmit a portion of the light from the input fiber to the main output fiber and reflect the remainder of the light to the second output fiber. All ports made using polarization maintaining fiber are aligned so that polarized light aligned parallel to the stress rods on the input fiber emerges from the output fibers in the same manner, maintaining the polarization state to a high degree. Splitters that only split off a small portion of the input light are commonly known as taps and often used for power monitoring applications. For a very cost-effective alternative configuration, combining the functions of a tap and monitor photodiode in a single unit, we invite you to review OZ Optics’ OPM series of inline optical taps and monitors. Key Features: High Power Handling High Extinction Ratio Highly Modular and Flexible Design Wide Wavelength Range Bi-directional Broadband Performance Custom Designs Welcomed Mode-independent Behavior in Multi Mode (MM) Fiber Applications Splitting Ratio: 50/50 Standard, Custom Split Ratios 50/50 to 95/5 Available on Request Splitting Ratio Tolerance: ±3% (50/50 Splitters), ±2% (90/10 Splitters) Central Wavelength: 1550 nm Standard, Other Wavelengths on Request Bandwidth: ±1.5% of Central Wavelength Wavelength Dependent Loss (WDL): 0.1 dB (1520-1570 nm) Polarization Extinction Ratio: 20 dB Min., 23 dB Typ. (630-1600 nm), 17 dB Min., 20 dB Typ. (400-630 nm) Polarization Dependent Loss (PDL): ±0.25 dB Directivity: >50 dB Return Loss (RL): 30 dB to 60 dB Insertion Loss (IL): <0.5 dB to <1.0 dB Power Handling: >1 W (+30 dBm) Operating Temperature Range: 0°C to +70°C Applications: EDFA Amplifier; Raman Amplifier Combiner; Polarization Mode Dispersion Compensation; Polarization Extinction Ratio (PER) Measurements; Fiber Optic Sensors; Coherent Communication Systems; Quantum Cryptography; Return Loss (RL) Measurement