Spectroscopy Rail; Collinear Adapter; Lens Options, T-Image Platform Luna’s T-Ray ASR5001 is the first compact pulsed terahertz measurement system that is robust enough to be deployed in an industrial environment and has all of the flexibility provided by Luna’s fiber-coupled sensor heads in a rack mount package. With Luna’s range of accessories and fixturing devices, the T-Ray® 5000 can be configured to fit your specific application. With its exceptionally long high-speed delay, the T-Ray® 5000 is ideally suited for spectroscopic investigations, providing spectral resolution down to 1.5 GHz at 100 Hz. The transmitter (HTS40nm) and receiver (HRS40n1) can be mounted on the T-Ray® ASR5001 spectroscopy rail to perform transmission spectroscopy measurements. A standard mount is provided to hold accessories or standard sample cards. The rail can accommodate lenses up to 150 mm working distance. An iris is provided on the sample holder to block any portions of the beam that may not be going through the sample. Tip-tilt stages provide easy optimization of the beam alignment to ensure maximum bandwidth. Using the T-Ray® 5000 AXA40n1 collinear adapter, transmitter and receiver can be coupled to perform as an integrated collinear reflection transceiver. Alignment pins provide precise positioning. The adapter has two ports for the lens, so it can be assembled as right or left-handed. Reflection measurements are easily acquired because the transmitter and receiver share the same lens. Spatial resolution down to 100 µm has been obtained using this arrangement with a 25.4 mm focal length lens. The transceiver is ideal for reflection tomography. When used with an HTS40nm and an HRS40n1, the assembled collinear transceiver based on ASR5001 or AXA40n1 will provide over 3.5 THz of bandwidth and SNR of 70 dB (ASR5001) or 60 dB (AXA40n1) respectively. The T-Ray® 5000 HTS/HRS Transmitters & Receivers come standard with a 38 mm diameter lens in an adjustable lens tube. In addition to that, Luna offers T-Ray® 5000 lens options ranging from 38.1 mm to 76.2 mm and 152.4 mm in diameter, with focal lengths ranging from 25.4 mm and 76.2 mm to 152.4 mm and 304.8 mm, plus a collimating lens. Here, the “focal length” is the distance from the lens surface to the beam waist. Lens tubes that mount on the transmitter or receiver are also available for 38.1 mm and 76.2 mm lenses. The lenses are manufactured from high-density polyethylene (HDPE) and are manufactured to an aspheric profile for high-quality focusing across a wide range of frequencies. Luna has specifically designed these lenses for use with their fiber-coupled transmitter and receiver sensor heads. When mounted on the front of a transmitter, the lens will provide a collimated or a focused beam. Use relay lenses in conjunction with a collimating lens on the sensor head. The collinear adapter (AXA5001) and the integrated collinear transceiver (HXC50xn) are compatible with 38.1 mm diameter lenses. The T-Ray® 5000 MSL5201 T-Image platform can be positioned for horizontal or vertical scanning. The transmitter and receiver can be configured in transmission or collinear reflection geometry by using the collinear adapter. The MSL5201 can move at speeds up to 150 mm/s and can provide step resolutions below 30 µm. The motors are integrated with the required amplifier and encoder to allow high-quality images to be acquired at speeds up to 1000 pixels/s. The T-Ray® 5000 MSL5201 T-Image platform has an embedded motion controller that is configured by software running on the Terahertz Control Unit. Key Features T-Ray® ASR5001 Spectroscopy Rail: Easy Alignment Without an Optical Table Sample Mounting Fixture With Integrated Iris No Tool Required to Change Lenses Accommodate Various Focal Length Lenses Use to Measure Transmission Spectroscopy Compatible With HTS40nm and HSR40n1 Rail Length: 60 cm Dimensions: 60 x 15.5 x 7.5 cm Weight: 2.0 kg Key Features AXA40n1 Collinear Adapter: Easily Switch to Transceiver Configration Simple Orientation to Target No Tool Required to Change Lenses Expands System Capability Use to Measure Layer Thickness Use to Produce Scanned Images Compatible With HTS40nm and HSR40n1 Variety of Focal Lengths Available Right or Left Handed Operation Polarization Extinction Ratio (PER): >20:1, Horizontal Beam Diameter: 38 mm Available Lens Focal Length: 25 mm, 75 mm, 150 mm, Collimating Lens Mounting Hardware: ¼-20 Threaded Mounting Holes Dimensions: 70 x 64 x 70 mm Weight: 320 g Key Features T-Ray® 5000 Lens Options: Low Loss Simple Alignment No Tool Required for Installation Compatible With Transmitter or Receiver Compatible With Collinear Adapter Lens Diameter: 38.1 mm, 76.1 mm, 152.4 mm Lens Focal Length: 25.4 mm, 76.2 mm, 152.4 mm, 304.8 mm Adjustable Lens Tubes Available for 38.1 mm, 76.1 mm Diameter Lenses Key Features T-Ray® 5000 MSL5201 T-Image Platform: Fiber-coupled to Allow Easy Movement Image Resolution to 100 µm Perfect for Field Work Built to Operate Upright or Prone Easy to Use Imaging Software Available Transmission or Reflection Images Multiple Lens Configurations Available Scan range: 30 cm Minimum Step: <30 µm Focal Lengths: 25 mm, 75 mm, 150 mm Power Supply Voltage Requirements: 110/240 VAC Dimensions: 660 mm x 699 mm x 330 mm Weight: 21.3 kg Applications: Time Domain Spectroscopy; Time Domain Reflection Tomography; Defect Detection; Basis Weight Measurement; System Optimization & Verification; Reaction Kinetics Monitoring; Medical & Biological Research; Nondestructive Materials Inspection; Package Inspection; Semiconductor Wafer Inspection; Remote Threat Detection; Homeland Security

DGD Range 0-200, 0-44 ps; DGD Resolution 0.2 ps; Single Band C, L, O, Dual Band CL; Max. IL 3.5 dB; Max. PDL 0.3 dB; RL >50 dB Polarization mode dispersion (PMD) can seriously degrade the quality of high-speed fiber-optic data transmission. High-speed transceivers must meet stringent standards for PMD tolerance. General Photonics’ DGD-1000 PMD Source/Emulator accurately and repeatably generates both high and low values of differential group delay (DGD) or first-order PMD. Both the DGD and PDL are very stable over time and wavelength within the performance band. The DGD-1000 PMD source/emulator is available in different versions to accommodate the need for different wavelengths and DGD ranges. Key Features: Generates Differential Group Delay DGD up to 400 ps DGD Range: 0 to 200 ps, 0 to 400 ps DGD Resolution: 0.2 ps DGD Change Rate: Up to 64 ps/s Wavelength Range Single Band: C Band, L Band or O Band Wavelength Range Dual Band: CL Bands Insertion Loss (IL): ≤3.5 dB Very Low Insertion Loss (IL) Variation Over DGD Range: 0.1 dB typ. Very Low Polarization Dependent Loss (PDL) Over DGD Generation Range: 0.3 dB max., 0.1 dB typ. Return Loss: >50 dB Slow SOP Variation: <1 rad/min Small DGD Variation Over Time: <0.1 ps Over 8 Hours Extended Version Can Cover up to 600 ps as Special Order Applications: System PMD Tolerance Testing; 1st Order PMD Performance Simulation

520 to 660 nm; Optical Power 0.5 to 30 mW; CW to 2 kHz; Connector Type Super/Angled NTT-FC/PC, SC, ST, Universal OZ Optics’ FODL series of visible fiber optic fault locators launches 635 nm visible laser diode light into the fiber. When light encounters a break or sharp bend, it scatters, and the scattered light can be observed emerging from the cable. Fault locators can locate breaks in short patchcords, which an OTDR cannot detect due to its operating dead zone. A fault locator is also much less expensive than an OTDR. However, they are not recommended for use with dark-colored or armored cables. Another use for fault locators is to check connector quality – inside the connector ferrule, poor gluing or dirt may create a micro bend in the fiber producing excess insertion or return losses and maybe resulting in premature failure of the connector. Launching visible light through the fiber, so that it emerges from the connector in question, the distortion appears as a series of rings superimposed on a normal output. Fault locators are available in bench-top, pocket and pen format. Pocket size fault locators can be operated in either CW or pulse modulation mode. Pen size fault locators are CW only. High power versions, available as bench-top units, are also CW only. Key Features: Pen, Pocket and Bench-top Versions Available High Visibility (up to 6 km with a 1 mW, 635 nm Source) Higher Output up to 30 mW, Non-contact Style Power Versions Available Continuous Light or Pulse Modulation Power Supply Alkaline Batteries or AC/DC Adapter Carrying Pouch with Belt Clip for Pocket-size Version 1.25 mm and 2.5 mm ID Universal Connector Receptacles Available Applications: Single Mode and Multi Mode Fiber Testing; Fiber Identifier Applications; Locating Breaks and Bends in Fibers and Connectors; Identifying Fibers and Tracing Optical Signals by Using Modulated Signals; Optimizing Splices

Wavelength 215-401 nm; ISO/IEC 17025:2017 Accredited; NIST traceable calibration The ILT770 is a compact, handheld UV light meter that’s loaded with features. It’s designed for use in a phototherapy booth and comes with built-in data storage, a rechargeable lithium ION battery, and a user-friendly display that shows both numerical and graphical readings. This allows for easy analysis of the system and generation of reports. The units of readout include both Irradiance in W/cm2 and dose in J/cm2, with auto-ranging capabilities (uw/cm2, mW/cm2 uJ/cm2, mJ/cm2, J/cm2 etc). The ILT770 UV light meter is available in five standard configurations: ILT770-UV: 215-350 nm ILT770-NB: 249-259 nm ILT770-NBUVB311: 275-325 nm ILT770-UVA-350: 315-390 nm ILT770-UVA-1: 326-401 nm Each package includes an ILT770 light meter, a UV sensor (options include UVC, Narrow band UVC, Narrow band UVB, UVA or UVA-1), a NIST traceable – ISO17025 accredited calibration with certificate, a storage case, a USB cable, PC software for downloading stored readings, and a 1-year warranty. This is a comprehensive solution for your UV measurement needs. Key features: SO/IEC 17025:2017 Accredited, NIST traceable calibration for results you can trust Measures irradiance and dose Graphical display with data analysis Affordable Stores readings that can be downloaded to a PC Compact, portable ergonomic design Rechargeable battery Create reports with downloaded data Easy-to-use interface Made in the USA BNC connector locks sensor in place Linear over 4 decades of light levels Applications: Validation of UV disinfection systems; testing of UVA and narrow-band UVB sources, e.g. for skin treatment

Measurement Range: > 10 Decades 100 fA - 1 mA - (1 n/Wcm2 to 10 W/cm2); Datalogging Memory 16,380 total light level readings; Operating Temperature -40 - +85°C The ILT2400 stands out as the market’s most advanced hand-held light/lux meter and optometer. It comes equipped with ILT’s Accuspan software, which automatically sets the averaging while swiftly measuring over eight decades of light intensities. The built-in software enables customers to capture a peak as brief as 100μS and store up to 16 readings per second. The color display is versatile, functioning in both landscape and portrait modes. ILT, based in Peabody, MA, USA, manufactures the ILT2400 and its software. This allows ILT to quickly configure and customize components to meet the needs of customers and OEMs. The ILT2400 optical measurement systems package includes an ILT2400 device, carrying case, software, and a detector/filter/optic and calibration configured to the customer’s needs. The ILT2400 optical measurement systems enable direct reading in the relevant empirical units, including lux, foot-candles, candela, lumens, watts, W/cm2, cd/m2, foot-lamberts, nits, etc. The ILT2400 and its software are compatible with most computers running Windows 7 and Windows 8. Key features: Research Quality at a Hand-held Price 8 Decade Dynamic Range of Optical Analysis Meter & Sensors with NIST Traceable ISO17025 Accredited Calibration Hand-held, Compact, Ergonomic Design Brilliant 4.3” Touch Screen Display 90° Screen Rotation for Landscape and Portrait Viewing ILT’s Accuspan: Auto-ranging with Smart Averaging Built-in Rechargeable Battery Lasts Up to 8 Hours Backwards Compatible with ILT1700 Sensors Measurement Speeds Up to 100 μSeconds Includes DataLight III comprehensive software package for both Mac and PC Made in the USA Applications: Audience Scanning Laser Safety, General Purpose Light Measurements, Research, Sterilization/UVGI, Solar Measurements, Photoresist/Lithography, Optical Radiation Hazard, Phototherapy, Photo-Degradation, PPF & PPFD Plant Studies, and more.

Measurement Range 100 fA - 1 mA; Reverse Bias 2 Voltages/Selectable; Operating Temperature -40 - +85 °C; Calibrated Irradiance 0 - 40 °C The ILT5000 radiometer is the ILT1700 for the 21st Century! Improvements on the industry standard ILT1700 include rapid optical measurements (1-100hz), a broader dynamic range (100fA to 1mA), Datalight III for PC and Mac, plus built-in wireless, data storage, and rechargeable batteries. The ILT5000 is backwards compatible with the ILT1700 sensor configurations, as well as all of ILT's sensor accessories including filters, optics, integrating spheres and ISO/IEC 17025:2017 Accredited/NIST traceable calibrations. ILT manufactures the ILT5000 and DataLight III radiometer in the USA at our Peabody, MA facility which allows us to rapidly customize system components to meet the needs of our customers and OEMs. ILT5000 optical measurement systems typically consist of the ILT5000 light meter, a sensor, filter, optic and calibration to allow direct reading in the appropriate empirical units including lux, foot-candles, candela, lumens, watts, W/cm2, cd/m2, foot-lamberts, nits, etc. Measurement systems: The ILT5000 meter requires a sensor to measure light. Sensors are available to measure from 185 nm out to 40 micron and are supported with a vast array of accessory including bandpass filter, cosine receptors, integrating sphere, and numerous types of calibration. Key Features: Measurement Range: Over 10 Decades 100 fA - 1 mA- (1 n/Wcm2 to 10 W/cm2) Datalogging Memory: Can store 16,380 total light level readings or 8,190 light level with real time stamp (At one reading per minute, this equates to 11.3 days (real time stamp off) or 5.6 days of logging with time stamp on) Built-in Wi-Fi Operating Temperature: -40 to 85° C (Calibrated Irradiance: 0-50° C) USB: USB2, Including Power, for Single and Multiple Systems USB Current Draw: 500 mA max., 250 mA typical Size: 1-3/5" H x 5" W x 7" L Input Connector: D-Sub and SMA CE Certified: No rf noise Calibration: NIST Traceable/ISO 17025 4 - 20 mA output Sample rate up to 100 Hz, programmable Auto-range, Auto-dark, Auto-sample with user control options Built-in rechargeable battery pack "Set it & Forget it" remote data logging Continuous multi-system monitoring Backward compatible with the ILT1700 SED detector/filter/optics Labview compatible NIST Traceable / ISO/IEC 17025:2017 Accredited calibration and certificate Includes DataLight III comprehensive software package for both Mac and PC Comes with ILT's DataLight III Software includedDataLight is all about supplying fast, reliable light measurement data to you computer for analysis. Our extensive light measurement software package is available for Windows PC, Tablet and MAC computers. DataLight III includes our "set it and forget it" remote internal data storage app., an improved All-in-One meters app for control and transmission of data using a mini USB cable or wireless data transmission, as well as a full API and command line interface for user programming and customization. Applications: Radiometry, Photometry, Reasearch, UVGI- Sterilization, Solar, Photoresist, Optical Radiation Hazard, Phototherapy, Photo-degradation, Plant Growth and more

Wavelength 420-520 nm; Band Irradiance Range .08 to 8000 µW/cm2/nm; Irradiance Range 3 to 300,000 µW/cm2; Current Range 1 nA to 1.65 uA The ILT750 Bili Light Meter is available in two configurations: ILT750 Bili Light Meter – 470 nm ILT750 Bili454 Light Meter – 454 nm, direct substitute for the Ohmeda Light Meter   The ILT750 Bili Light Meter is a comprehensive solution for measuring light in neonatal jaundice treatment systems. This bilirubin light meter eliminates the need for manual recording and calculation of multiple measurements to obtain your irradiance value. Simply move the ILT750 detector over the blanket or under the light source and let the meter calculate for you. Key features: Dual units with a wide sensitivity range: from .08 to 8000 µW/cm2/nm, and 3.0 to 300,000 µW/cm2 User-friendly device 3-digit display resolution Peak response at 470 nm, aligning with the bilirubin action spectrum Calibration that is ISO/IEC 17025:2017 Accredited and NIST Traceable Sensor corrected for cosine for accurate spatial response Measures Band Irradiance (µW/cm2/nm) or Irradiance (W/cm2) Compatible with traditional and LED sources Suitable for bili blankets, pads, or overhead lamps Housing that is easy to clean Compact and ergonomic design that is easy to hold Powered by AA batteries Made in the USA   The ILT750-BILI454 Light Meter serves as a direct substitute for the Ohmeda light meter, designed to test both traditional and LED blue light sources from GE, which are used in the treatment of neonatal jaundice. The advanced capabilities of the ILT model remove the need for manual calculations or note-taking. Simply move the detector across the blanket or beneath the light source, and the meter will handle the calculations for you. After rigorous design and testing, the ILT750-BILI454 meter can read within a few percentage points of the discontinued Ohmeda Biliblanket II Blue light meter. This meter is versatile and can be used not only on the blanket but also on all GE lighting systems, including: GE Giraffe Systems GE Lullaby Systems GE BiliSoft Systems Traditional GE Blue light systems Key features: Measures within a few percentages of the discontinued Ohmeda meter Features a large, easy-to-read OLED display Calibrated at 454 nm using a GE LED light source Can verify and average irradiance values across the entire treatment area in less than a minute Calibration is ISO/IEC 17025:2017 Accredited and NIST Traceable Allows selection of units (µW/cm2/nm or W/cm2) Designed with an easy-to-hold, lightweight, and ergonomic design that’s easy to clean Custom filter matching is designed into the device Made in the USA Applications: testing of GE traditional and LED blue light sources for treatment of infant jaundice

Wavelength 215-475 nm; Range 4.5 decade (mW/cm2 to 40W/cm2); Temperature 0-75 °C (internal case temperature) The ILT800 CureRight is a UV curing radiometer that is packed with features, offering unparalleled flexibility and capabilities not found in any other system. Its adaptability enables the device to measure lights used for UV curing and a variety of other applications such as sterilization/disinfection, lithography, and more. The system is designed with the diverse needs of its users in mind and can be tailored to fit your specific environment. The ILT800 CureRight series validates and measures all kinds of UV curing methods and sources, including conveyor, belt, oven, flood, area, spot, fiber optic, collimated beam, side cure, 180° curing, 3D printing, pulsed and traditional UV lamps, and UV/VIS LEDs & light sources. The ILT CureRight is available in five standard configurations: ILT800-UVA: 315 - 390 nm ILT800-BAV: 275 - 475 nm ILT800-UV: 250 - 400 nm ILT800-CUV: 215 - 350 nm ILT800-UVF (UV LED): 360 - 400 nm Flat, (275 - 450 nm) Contact us for OEM / Custom Filtration The ILT800 CureRight UV radiometer system surpasses competitors with features like standard profiling and programmable settings such as measurement modes (auto/manual/live), minimum light level threshold, and lamp-to-lamp measurement interval (delay). The system also boasts a unique user interface that places the input sensor and optic, device controls, and the readout display all on one side, facilitating simultaneous measurement, monitoring, and analysis of measurement data. The ILT800 UV radiometer allows users to track their curing processes over time by allowing them to store, download, and view both current and all previously saved readings on the device’s integrated OLED display. This built-in data storage and review feature enables users to quickly identify changes that have occurred over time. It also helps users to easily spot potential issues in their systems such as dirty lamps and reflectors, lamp/reflector misalignment, declining lamp output, failed lamps, and power supply problems, among others. Additional benefits include the ability to download the results to a computer for more detailed analysis. With ILT’s proprietary DataLight CureRight software interface, users can download and view their data, as well as generate spreadsheets and reports using their own analysis tools. To further enhance the data storage and capabilities, ILT introduced an advanced sorting feature called Device ID, a feature not found in any other UV curing light meter. Device ID allows users to program up to 20 unique system/light source name tags. Device ID enables users to view and export all saved data for each curing station or light source into separate files, clearly identified with the Device ID. It’s like having the functionality of multiple meters in a single device. The ILT800’s spectral filtration was designed to match the photoinitiators’ response to UV light, which is directly related to its absorption and is highly wavelength selective. Most lamps emit broadband UV/VIS/IR, and the lamp’s output may not change evenly across all wavelengths. The ILT800 filters were designed to monitor changes in output in the areas that affect absorption, and consequently, the effectiveness of the curing. Whether you’re using a low-output fluorescent source for sterilization, high-intensity mercury or xenon lamps for curing, or narrow-band LEDs for photolithography, there’s a version of the ILT800 tailored for your needs. Filtration options covering UVC to UV-VIS Filtration to ensure a process match Measures only the light that effects the cure Applications: low-output fluorescent sources for sterilization, high-intensity mercury or xenon lamps for curing, narrow-band LEDs for photolithography

OSNR Range 5-38 dB; 1529-1561.5 nm; Min. Optical Input Power -10 dBm, Min. Optical Output Power +8 dBm; Channel Spacing 50-400 GHz OZ Optics' iOSNRG-1000-TUN intelligent optical signal-to-noise ratio generator (iOSNRG) has been designed to allow users to inject a programmable level of noise into an optical signal, creating a precisely defined signal-to-noise ratio. All iOSNRG settings can be controlled automatically with the user-friendly touch panel or computer interface. With a built-in bandwidth-adjustable tunable filter, the wavelength can be selected to be any channel within the ITU 50G Grid or any other ITU Grid. The output power level is user programmable, making the iOSNRG-1000-TUN an ideal instrument for doing OSNR measurements in data communication systems. The instrument comes with GPIB, USB, and Ethernet interfaces, allowing it to be controlled by a computer, for automated testing of systems or devices. Key Features: User Selectable Optical Signal-to-noise Ratio (OSNR) and Power Level Built-in Tunable Filter with Adjustable Bandwidth Stand-alone Device with Touchscreen Control for Local Operation GPIB, USB, and Ethernet Interfaces for Computer Control Optical Port for Connecting External Optical Spectrum Analyzer Provision for External Filter Direct Output from Tunable Filter or with EDFA Amplification Supports 50G/100G/200G/400G Applications OSNR Range: 5 dB to 38 dB OSNR Setting Accuracy: ±0.5 dB Optical Input Power: >-10 dBm Optical Output Power:: ≥+8 (dBm) Wavelength: 1529 nm to 1561.5 nm Channel Spacing: 50/100/200/400 GHz Fiber Core/Cladding: 9/125 μm Supply Voltage: 110–220 VAC, 47-63 Hz Max. Electrical Power: 80 W Dimensions1: 390x344x86 mm Weight: 7.5 kg Applications: Fiber Optic Network Testing; Bit Error Rate (BER )Testing; Eye Diagram Quality Testing; DWDM Network Testing; Submarine Network Testing

1270-1610 nm; Wavelength Resolution 1.6 pm; Loss Measurement Dynamic Range 60, 80 dB; Loss Measurement Resolution ±0.002, ±0.05 dB; Laser Sweep Rate 70 nm/s; Measurement Time 12, 55 s; Maximum Device Length 75, 150 m Luna’s LCA 500 lightwave component analyzers are fast and accurate systems that are ideal for production test and quality control. The LCA 500 series provides the high throughput and connectivity needed for the manufacturing floor while delivering the extremely high resolution and sensitivity that is critical when testing and validating modern photonic devices and network subsystems. The LCA 500 lightwave component analyzers provide single-scan measurements for testing a wide range of passive components from couplers to Optical Fibers and everything in between (Fiber Bragg Gratings, arrayed waveguide gratings, free-space filters, tunable devices, amplifiers, etc.). Key Features: Single Scan Measurement of Insertion Loss (IL), Return Loss (RL) and Polarization Dependent Loss (PDL) High Resolution: 1.6 pm High Sensitivity: 80 dB Dynamic Range Integrated Tunable Light Source – No External Tunable Laser Needed Measure in Transmission or Reflection Compatible With C and L Band (LCA 500) or O Band (LCA 513) Complete Full-band Measurement Scan in Less Than 3 s User-friendly Interface Wavelength Range: 1270 to 1610 nm Wavelength Resolution: 1.6 pm Loss Measurement Dynamic Range: 60, 80 dB Loss Measurement Resolution: ±0.002, ±0.05 dB Laser Sweep Rate: 70 nm/s, 1 Hz Measurement Time: 12, 55 s Maximum Device Length: 75 m (Reflection), 150 m (Transmission) Applications: Testing of Passive Components like DWDMs, AWGs, Filters, Switches, Waveguide Gratings, Modulators, Couplers, etc.; High-resolution Measurements for Planar Light Circuits (PLCs) and Silicon Photonic Devices; Manufacturing Test and Quality Control; Flexible Tunable Laser Source splitters

Laser Diode Current 0-500 mA; LD Compliance Voltage 0.0-8.0 V; TEC Current 0-1 A; TEC Voltage Range ±8.00 V; Photodiode Current 0-3600 μA; Setpoint Resolution 0.1 mA; Setpoint Accuracy ±0.05% OZ Optics’ LDA-100 low cost, compact and standalone laser diode analyzer provides quick and versatile laser diode characterization and parametric analysis. The unit features a high-resolution LIV (light, current, voltage) measurement system, providing all main laser diode parameters including threshold current and slope efficiency. The setup and measurement takes only a few seconds. The measured parameters are displayed on a color touch screen, and the data can be downloaded to any host computer for further processing and analysis through a built-in USB interface. The unit features a built-in smart driver that will automatically detect the laser diode pinout. The user can select to operate the laser diode under test in either auto-current or auto-power control modes. The integrated TEC controller maintains your diode at its operating temperature, ensuring accurate and repeatable measurements. The smart laser diode analyzer comes with multiple features for safe and accurate measurements. These features include current limit protection, automatic pinout detection, sensor range checks and manager passcode level to prevent any accidental changes of the preset settings that could otherwise harm the laser diode under test, or invalidate the results. External interlocks can be connected to disable the laser diode in response to safety concern situations. Each unit is provided as a set that includes all required accessories for direct plug-and-play operation. The kit includes a calibrated optical power meter head and a thermally controlled laser diode holder for 5.6 mm package laser diodes (holders for 3.8 mm and 9 mm packages are offered separately). A simple sliding mechanism allows easy laser diode replacement. Special laser diode adapters can be customized upon request for any laser diode package. Key Features: Integrated Temperature Controller Compact Plug-and-Play Laser Diode Analyzer Fast and Accurate LIV (Light, Current, Voltage) Curve Generation With 0.1 mA Resolution Setpoint Resolution: 0.1 mA Setpoint Accuracy: ±0.05% Laser Diode Compliance Voltage: 0.0 V to 8.0 V Laser Diode Drive Current up to 500 mA Photodiode Current Range: 0 μA to 3600 μA Photodiode Current Resolution: 0.1 μA 15-bit Power Resolution 3 W Output TEC Temperature Controller Max. TEC Current: 1 A TEC Voltage Range: ±8.00 V Temperature Control Range: +10°C to +50°C Password Protection, Hardware Interlock and Overcurrent Shut-off Circuitry for Safety Built-in Smart Driver for Diode Pinout Auto Detection and Temperature Control Touchscreen Control and Accompanying Windows Software Operating Rel. Humidity: <85%, Non-condensing Dimensions Analyzer: 110 x 63 x 30 mm Dimensions Analyzer + Accessories: 110 x 115 x 45 mm Weight Analyzer: 300 g Weight Analyzer + Accessories: 1000 g Applications: Laser Diode Characterization; Laser Diode Quality Control; Laser Source Calibration

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

Zero Dead Zone; 1270-1610 nm; Resolution 10-250 µm; Scan Time 0.4-16 s; Max. Device Length 30-2,000 m; Dynamic Range 60, 80 dB; Backscatter-level Sensitivity -130 dB OBR 4600 optical backscatter reflectometers are part of Luna’s award-winning OBR Optical Backscatter Reflectometer product line. Designed for component testing, short run network testing and troubleshooting, the OBR 4600 reflectometers enable ultra-high resolution reflectometry with backscatter level sensitivity. The OBR 4600 reflectometers feature spatial resolution as fine as 10 µm, no dead zone and an extremely low noise floor. The OBR 4600 comes with an extensive range of options including a strain and temperature sensing package with maximum sensor lengths up to 2 km. To increase the functionality of their OBR 4600 optical backscatter reflectometer, users can add the following options: Spot Scan Option: Allows the user to narrow the scan range to 1 to 2 m area within the network under test. This reduces the time required to scan and also allows the user to focus exclusively on the area of interest. Hard Shell Carrying Case Option: The OBR 4600 can be provided with a hard shell carrying case for applications that require portability or exposure to more rugged environments. 2 km Sensing Length Option: The OBR 4600 range can be extended up to 2 km with a 3 mm spatial resolution and no dead zone. Software Development Kit Option: A selection of DLL files can be provided to allow users to customize their own test equipment user interface with the OBR 4600 operation. Lightpath Analysis Software Option: Allows the user to program a go/no go check based on a pre-selected characterization of a component or network. This option is ideal for testing and can reduce a complicated analysis to a simple pass/fail end of line production test. Distributed Temperature and Strain Sensing Package: This option allows the user to make strain or temperature measurements using sensors made with standard unaltered fiber optic cable that does not require fiber bragg gratings. The distributed sensing option can provide sub-cm spatial resolution with sensors up to 2 km. Key Features: “Zero Dead Zone” Reflectometers Measure Insertion Loss (IL), Return Loss (RL), Distributed Loss, Distance, Polarization States, Phase Derivative and Group Delay Easily Locate, Identify and Troubleshoot Macro-bends, Splices, Connectors and Breaks Dual Display With Intuitive User Interface Allows to Simultaneously Determine Fault Location and Fault Magnitude and Perform Fault or Component Characterization Highlight Selected Sections of the Scan and Perform an Analysis in the Frequency Domain User-selectable Scanning Wavelength Range and Centerpoint Fast Scanning: Measure 30 m with 10 μm Sampling Resolution in <7 s Continuous High-speed Scanning: 1 m Segments at up to 3 Hz Optional Spot Scanning Feature Extended Range Option Provides 2 km Range With no Dead Zone Wavelength Range: 1270 to 1610 nm Maximum Wavelength Resolution: 0.02 pm Maximum Device Length: 30 to 2,000 m Sampling Resolution: 10 to 250 µm Scan Time: 0.4 to 16 s Measurement Rate in Spot Scan Mode: 0.15 to 3.7 Hz Dynamic Range: 60, 80 dB Backscatter-level Sensitivity: -130 dB High-resolution C and L Band (OBR 4600) or O Band (OBR 4613) Capability Applications: Easily Locate, Identify and Troubleshoot Macro-bends, Splices, Connectors and Breaks; Locate Insertion Loss (IL) Points at Every Point in the Network or Assembly – Eliminate Cutbacks; Test and Troubleshoot Short-run Networks (up to 2 km); Unprecedented Visibility into Miniaturized Components

Portable & Rugged; 1270-1610 nm; Resolution 80-200 µm; Measurement Time 10 s; Measurement Length Modes 10,50,100 m; Dynamic Range 15 (IL), 70 (RL) dB; RL Measurement Sensitivity -129 dB Luna’s OBR 6200 series of optical backscatter reflectometers are portable and rugged ultra-high resolution reflectometers with backscatter-level sensitivity for testing short networks deployed in aerospace, naval, data center and industrial applications. Troubleshoot fiber assemblies in the field to easily locate optical loss events with sub-millimeter resolution. Learn more about highest-resolution OTDR measurements available in the downloadable data sheet. The OBR 6200 series utilizes optical frequency domain reflectometry (OFDR) technology to measure distributed return loss (RL) and insertion loss (IL) with high precision and dynamic range. The systems easily locate optical loss events with sub-millimeter spatial resolution. OBR 6200 optical backscatter reflectometers are rugged battery-powered integrated systems with an intuitive touchscreen user interface, making them ideal for field maintenance applications. The user interface includes screen modes for interactive RL and IL measurement as well as automatic event detection. Key Features: Fully Portable and Rugged Optical Backscatter Reflectometers Track and Analyze Return Loss (RL) and Insertion Loss (IL) Versus Length Spatial Sampling Resolution: Down to 80 μm Detect and Precisely Locate Reflective Events Measure Optical Path Length With High Precision Automatic Event Detection One or Two Optical Channels Available With IP65 and MIL-STD Certifications Measurement Length Modes: 10, 50, 100 m Sampling Resolution: 80 to 200 µm Length Measurement Accuracy: <1 to <4 mm Wavelength Scan Range: 4 to 10 nm Center Wavelength: 1546.7 nm Measurement Time: 10 s Dynamic Range: 70 dB (RL Measurement), 15 dB (IL Measurement) Return Loss Measurement Sensitivity: -129 dB Measurement Resolution: ±0.1 dB Applications: Troubleshoot Fiber Assemblies in the Field; Precisely Locate Insertion Loss (IL) Sites, High-RL (Return Loss) Connections, Fiber Breaks, etc.; Maintain Avionics, Aerospace, Naval and Industrial Networks; Verify Fiber Lengths of Data Center Interconnects; Troubleshoot Fiber Optic Sensing Systems

1260-1620 nm; 8-40 Channels; PDL Measurement Range 0-20 dB; PDL Resolution 0.01 dB; IL Measurement Range 0-60 dB; IL Resolution 0.002 dB; Optical Power Range -60-8 dBm; Optical Power Accuracy ±0.5 dB General Photonics’ OCA-1000 is a multi-channel optical component analyzer that simultaneously measures insertion loss (IL), polarization dependent loss (PDL), and optical power (P) on multiple optical paths. The measurement is based on the Mueller Matrix method, which offers fast characterization of wavelength dependent optical parameters that are critical in today’s optical communication systems. The OCA-1000 base model can have up to eight channels. Custom 8- or 16-channel expansion units can be added to increase the system capacity to up to 40 channels. The instrument comes with a control program with built-in functions to display measured power, IL, and PDL vs. wavelength or to monitor the time variation of power/IL for all channels simultaneously to determine their stability. For AWG characterization, the data analysis software also calculates passband center wavelength, bandwidth, and flatness as well as inter-channel crosstalk (from adjacent and nonadjacent channels). The OCA-1000 optical component analyzer is an ideal solution for easy, accurate characterization of components and modules with multiple outputs, including DWDMs, ROADMs, AWGs and PLCs. It can be used with various tunable lasers , such as those from Keysight or Santec. This flexibility makes full use of existing laser resources and reduces the cost of making such measurements. Its rapid measurement reduces the time required to characterize devices with large numbers of ports, enabling higher production throughput. Key Features: Wide Wavelength Range: 1260 to 1360 nm (O-Band), 1480 to 1620 nm (C- & L-Bands) Number of Channels: 8 to 40 PDL Measurement Range: 0 to 20 dB High Polarization Dependent Loss (PDL) Accuracy: ±(0.02 + 2% of PDL) dB @PDL<10dB, ±(0.02 + 5% of PDL) dB @10<PDL<20dB PDL Resolution: 0.01 dB Insertion Loss (IL) Measurement Range: 0 to 55 dB, 0 to 60 dB IL Resolution: 0.002 dB Optical Power Range: -60 to 8 dBm Optical Power Accuracy: ±0.5 dB High Channel-to-channel Uniformity User-friendly Control Software Integration Time of Power Meter: 0.5 to 1,000 ms Dimensions: 19”-Rack-Mountable Enclosure, 1 U, 305 mm Depth Applications: PDL or IL vs. Wavelength Measurement; IL or Power vs. Time Measurement; DWDM Component Passband Characterization: Center Frequency, BW, Ripple, Noise Floor; Fiber Optic Component Characterization; Network Component Characterization (e.g. DWDM, ROADM); Planar Lightwave Circuits (PLC); Photonic Integrated Circuits (PIC)

1310, 1550 nm; Dynamic Range >80 dB; Scan Range 600 mm; Spatial Resolution 10-25 µm; RL Range 10-90 dB; Sweep Speed 20 mm/s General Photonics’ OCDR-1000 is an optical coherence domain reflectometer designed to obtain space-resolved reflection information inside a fiber optical component, such as a photonic integrated circuit (PIC), for diagnosing quality or design issues. It is based on a polarization optimized white light interferometer proprietary to General Photonics. The OCDR-1000 optical coherence domain reflectometer performs the functions of the discontinued Agilent 8504B Reflectometer – and more – but with better polarization management, spatial resolution and accuracy; larger scan range and dynamic range; and smaller size and weight. The OCR-1000 is a low-cost alternative to OFDR technology, with a much higher dynamic range that avoids the masking of small reflection peaks by the large reflections typical of the input surface of an optical device. The OCDR-1000 optical coherence domain reflectometer can measure devices with a length of up to 600 mm. A set of length-matching delay modules is available to match the pigtail lengths of the devices to be measured and place the measurement span in the region of interest. With a reflection dynamic range of over 80 dB and a spatial resolution down to 10 µm, this instrument helps engineers and researchers see the inside of an optical device to precisely identify defects and their locations. Key Features: Dynamic Range: >80 dB Scan Range: 600 mm (400 mm in Fiber) Spatial Resolution: 10 to 25 μm Operating Wavelengths: 1310, 1550 nm, Others on Request Return Loss (RL) Range: 10 to 90 dB Sweep Speed: 20 mm/s Compact & Lightweight Built-in Light Source Average Light Source Power: >-3 dBm Performs Functions of Discontinued Agilent 8504B Reflectometer - and More Dimensions: 89 x 356 x 356 mm Applications: Optical Characterization of Photonic Integrated Circuits, Fiber Optic Components; Accurate Measurement of Return Loss, Distributed Reflectivity

Attenuation Range 50 dB; Output Power Control ±0.1 dB; Min. Insertion Loss 1 dB, Input Power -10-+25 dBm; Polarization Dependence ±0.1 dB OZ Optics has successfully combined its expertise in variable attenuators with its optical power monitor technology to develop the OPR series of optical power regulators. These systems allow to maintain the output optical power from a fiber optic system at a constant level, countering changes caused by PDL, reduced amplifier gain, or other sources. The optical power regulators use the output from an optical power monitor as feedback to control an attenuator. Simple controls allow the user to enable or disable the feedback circuit, monitor the signal intensity, and control the output power through the fiber. The systems can maintain output power levels constant to better than ±0.1 dB, with millisecond response speed. Optical power regulators are used wherever one has an unstable output from an optical fiber and one needs a more stable signal. They are ideal for power stabilization in DWDM networks, where changes in power can produce transmission errors. The complete unit is available either as a miniature module that can be integrated into other devices, a stand-alone module for testing, or as a rack mountable unit for optical networks. Contact AMS Technologies for further information. Key Features: Controls Output Power to ±0.1 dB Dynamic Attenuation Range: 50 dB Millisecond Response Speed Single- and Multi-channel Versions Single Mode (SM) and Polarization Maintaining (PM) Fiber Versions OEM, Rack Mountable, and Stand-alone Versions Typ. Minimum Insertion Loss (IL): 1 dB Input Power Range: -20 dBm to +25 dBm Wavelength Dependent Response: ±0.25 dB (1510 nm to 1610 nm, Responses for Regulators for Other Wavelengths Will Vary) Polarization Dependence: ±0.1 dB Applications: Power Stabilization in DWDM Networks; Signal Conditioning in Test Equipment

Single-scan, All-parameter Measurement; 1270-1610 nm; Wavelength Resolution 1.6 pm; Loss Measurement Dynamic Range 60, 80 dB; Loss Measurement Resolution ±0.002, ±0.05 dB Luna’s OVA 5000 Optical Vector Analyzer™ is the fastest, most accurate and economical tool for loss, dispersion and polarization measurements of modern optical networking equipment – and the only instrument on the market that is capable of full and complete all-parameter linear characterization of single-mode optical components in a single scan. The OVA 5000 provides comprehensive component characterization of dispersion compensation modules, AWGs, Fiber Bragg Gratings and many other optical devices. The OVA 5000 uses an interferometric method to directly measure the linear transfer function (Jones Matrix) and simultaneously measure its four complex elements at every wavelength. From this data, all standard linear parameter measurements can be extracted with the highest dynamic range and accuracy available. The result is an extremely fast, high-resolution and accurate device characterization that is ideal for silicon photonics and other integrated photonics devices. The OVA 5000 simultaneously performs these optical component characterizations every 3 seconds: Insertion Loss (IL) Return Loss (RL) Dependent Loss (PDL) Phase Response Group Delay (GD) Chromatic Dispersion (CD) Polarization Mode Dispersion (PMD) / Second Order PMD Min/Max Loss Due to Polarization Impulse Response Jones Matrix Elements Phase Ripple – Linear and Quadratic With the optical frequency domain reflectometer (OFDR) option, the OVA 5000 optical vector analyzer can also operate as a high-resolution reflectometer , delivering reflectometer measurements with 20 μm sampling resolution, “zero dead zone” and high sensitivity (>95 dB). An optional polarization analysis software add-on allows the OVA 5000 to measure, calculate and display the response of an optical component to simulated input polarization states, eliminating the tedious and difficult task of polarization alignment. Key Features: Single Measurement, All-parameter Analysis of Devices up to 150 m in Length Full Characterization of Passive Devices in Under 3 s Complete Polarization Response Simultaneously Measure Complete Range of Parameters in One Single Scan: IL, RL, PDL, PMD, Second Order PMD, CD, GD, OTD Response, Jones Matrix Elements, Optical Phase Response High-Resolution C and L Band (OVA 5000) or O Band (OVA 5013) Capability Fast and Averaging Modes Real-time Measurements User-friendly Interface Wavelength Range: 1270 to 1610 nm Wavelength Resolution: 1.6 pm Loss Measurement Dynamic Range: 60, 80 dB Loss Measurement Resolution: ±0.002, ±0.05 dB Applications: Analyze Planar Light Circuits and Silicon Photonic Devices; Characterize Optical Fiber Components; Measure Both Spectral Response and Time Delay Response; Improve Device Simulations and Models With Complete Transfer Function

PDL Dynamic Range 0.1-20 dB; PDL Resolution 0.1 dB; C-, L-Band; Max. IL 2 dB; PDL Switching Time ≤5 ms; Residual PDM <0.1 ps; RL >50 dB High-speed fiber optic transceivers, including those deploying coherent detection technology for 40 Gbit/s and 100 Gbit/s data transmission, must meet stringent PDL (polarization dependent loss) tolerance specifications. In addition, the PDL tracking speed and response time of the PDL mitigation algorithm of a coherent detection receiver must be quantified. General Photonics’ PDLE-101 PDL emulator is specially designed for such PDL-related tests. This PDL source/ emulator can generate individual PDL values between 0 and 20 dB, with a resolution of 0.1 dB for PDL tolerance testing. It can also generate variable PDL with user defined range, waveform, and speed for PDL tracking speed and recovery time tests. The PDLE-101 PDL emulator can be controlled via the front panel keypad or by remote control via USB, RS-232, GPIB, or Ethernet interfaces. The residual PMD of the unit is less than 0.1 ps. Key Features: High PDL (Polarization Dependent Loss) Resolution: 0.1 dB Wide PDL Dynamic Range: 0.1 to 20 dB High Speed, PDL Switching Time: 5 ms max., 1 ms typ. PDL Waveforms: Sine, Square, Triangle Random PDL Generation Wavelength Range: C-Band or L-Band Max. Insertion Loss (IL): 2 dB @ PDL = 0, Excluding Connectors Low Residual PMD: <0.1 ps @ PDL = 0 Return Loss: >50 dB Fiber Type: SMF-28 Fiber Connector Type: FC/PC, FC/APC, SC/PC, SC/APC Optical Power Handling: 500 mW Applications: PDL Tolerance Test; PDL Tracking Speed and Recovery Time Tests; PDL Emulation; Code Development for PDL Compensation in Coherent Systems; System PDL Response Test

PMD Range 1st Order 0-91, 0.36-182.4 ps, 2nd Order 2,000, 8,100 ps²; PMD Switching Time 1 ms; C-, L-Band; IL 5.0, 5.5 dB; PDL 0.45, 0.5 dB; RL 50 dB General Photonics’ PMD-1000 is a flexible, digital PMD (polarization mode dispersion) source that deterministically generates precise 1st order PMD up to 180 ps and 2nd order PMD up to 8,100 ps2. Its quasi-continuous operation mode enables independent generation of first order and wavelength-independent second order PMD for uniform coverage of the PMD space. The PMD-1000 uses high-speed ternary magneto optic crystals to generate PMD. The PMD switching time is as short as one millisecond, making the PMD-1000 the fastest PMD generator on the market. Its automatic polarization controller combined with before and after polarimeters enhances the instrument’s flexibility. For example, if the polarization controller is used to align and maintain the input SOP (state of polarization) at 45° from the principal axis of the DGD (differential group delay) element, the instrument creates the worst-case first order PMD effect. Alternatively, the controller can adjust and maintain the input SOP using the feedback from the rear polarimeter to either minimize or maximize the output DOP (degree of polarization) for each PMD setting. Minimizing the output DOP enables testing of the worst-case total PMD effect, while maximizing the DOP turns the PMD-1000 into a PMD compensator, allowing the user to obtain optimized PMD values for PMD compensation. The PMD-1000 can also perform PMD emulation by generating statistical PMD distributions. Finally, the system’s polarization controller and polarimeters enable variable rate scrambling and deterministic polarization control functions, including trace generation and polarization stabilization at any SOP. General Photonics’ PMD-1000 makes your PMD-related systems testing simple, fast and professional. Key Features: All Digital Design – No Motors High-speed PMD Switching: 1 ms 1st and 2nd Order PMD Source/Emulator 1st Order PMD Range: 0 to 91 ps, 0.36 to 182.4 ps 2nd Order PMD Range: 2,000, 8,100 ps² Polarization Scrambling Automatic Polarization Alignment PMD Compensation Operating Wavelength Range: C-Band or L-Band Insertion Loss (IL): 5.0, 5.5 dB Input Power Range: -10 to 10 dBm Return Loss ((RL): 50 dB Polarization Dependent Loss (PDL): 0.45, 0.5 dB typ. SOP Tracking Speed: 10 π/s DOP Accuracy: ±2% Optical Power Handling: 300 mW min. Applications: Verifying System PMD Tolerance; Stress Test of PMD Compensation Circuits; PMDC Optimization; Calibration Source for PMD Instruments; System PMD Emulation

Tunable Pulse-width Compression & Spectral Bandwidth Expansion; 1020-1050 nm; Input Peak Power 39.6-43.8 kW; Output Peak Power 95.4-105.5 kW; Pulse-width Compression Factor >3 OZ Optics’ PWC pulse compressor and peak-field booster is a compact device that utilizes nonlinear effects from an optical fiber to surpass peak electric field limitations from an ultrafast optical source. After fixing the device to the output of the source, only minor adjustments are needed to increase the peak electric field by a factor of more than two. The pulse exiting this device contains more frequency content than the optical source and has a shorter pulse duration. Key Features: Higher Output Peak Field Easy Installation and Alignment Compact and Lightweight Platform Rugged and Fiber-based Design Tunable Pulse-width Compression Tunable Spectral Bandwidth Expansion Wavelength: 1020 nm, 1035 nm, 1050 nm Input Peak Power: 39.6 kW, 41.7 kW, 43.8 kW Output Peak Power: 95.4 kW, 100.5 kW, 105.5kW Pulse-width Compression Factor: >3 Operating Temperature Range: +15°C to +25°C Dimensions: 5 x 4.5 x 3.5 cm Weight: <0.3 kg Applications: THz Generation and Detection; Optical Microscopy; Nonlinear Optics

Horizontal PER <20:1; Beam Diameter 20, 38, 40 mm; Lens 25,75,150 mm, Collimating; Min. Layer Thickness 10-50 µm; Single High-flex Umbilical Luna’s T-Ray® 5000 measurement system is one of the fastest terahertz systems available on the market. Luna’s broad range of T-Gauge® sensor heads and gauges are paired with the T-Ray® 5000 Intelligent Terahertz Control Unit to create a complete system. Transmitter and receiver are securely mounted inside the online sensor head’s sealed metal housing. The umbilical for the transceiver, containing the electrical and optical connections, is constructed with high flex rated electrical cable to allow for continuous scanning. When connected to a T-Ray® 5000 Control Unit, the online sensor heads will provide excellent waveform response, capable of providing detailed reflection measurement of layered surfaces or products. The T-Gauge® HXC50yn is a high-performance online sensor head with full transceiver functionality and takes the robustness of the T-Ray® 5000 terahertz system to a new level with the ability to operate in industrial environments. Reflection measurement of thickness, multi-layer thickness, and basis weight are easily acquired. A variety of lenses are available to adjust the measurement spot size and working distance. The “y” and “n” in the model number correspond to the focal length of the lens, and the type of terahertz transmitter, respectively – “y” = 4 for 75 mm lens and 5 for 150mm lens, “n” = 1 for a type 1 transmitter and 2 for a type 2 transmitter. The T-Gauge® HXC51yn online sensor head adds functionality to the standard online sensor head with a virtual reference surface (VRS). Reflection measurement of thickness, multi-layer thickness, basis weight, and density are easily acquired. The VRS enables non-contact, calibration-less caliper thickness measurement as well as basis weight and density without reducing the open separation between the sensor and the product. The T-Gauge® HXP51y2 online EPG sensor head allows measurement of thinner layers than the standard HXC50yn online sensor head. With higher bandwidth and higher signal to noise, the EPG opens new applications to terahertz process control. Coatings on metal or composite substrates and free standing films can be measured down to 10 µm (0.5 mil). The T-Gauge® HSC50yn compact industrial sensor is designed for industrial applications that require a smaller footprint, a lighter weight or two output beams. These capabilities are met by the HSC50yn, which capitalizes on the new single fiber lighter weight umbilical, and a more compact design, to allow robot mounting. With proper attention to the configuration, it can be used to inspect two points on the same object. In the case of small diameter tubing, this can even be used to measure four orthogonal points at the same time. The T-Gauge® SCS500n explosion-proof thickness measurement system takes the robustness of the T-Ray® 5000 to a new level with the ability to operate in flammable atmospheres, such as paint booths or coating facilities. Designed to be robot mountable and intrinsically safe, the T-Gauge® SCS500n Online Sensor Solution CID1 SCS500n is optimized for use in spray booth applications but can be used in other applications as well. The working distance of the sensor head is fixed at 115 mm, but other working distances may be available upon request. The T-Ray® 5000 LSG500n line scan gauge (LSG) provides a handheld solution for high-speed scanning of a line 50 mm or 75mm in length. The line scan image is displayed on the screen of the handheld tool and can be analyzed by dedicated software for specific applications. Current software solutions can provide layer thickness measurements, detection of voids, or alignment of body panels with measurement of the vertical and horizontal offset between them. The T-Ray® 5000 SPG500n single point thickness measurement gauge allows direct measurement of multiple layer objects with the press of a button. The modular nature of the measurement tool allows either straight-on or right-angle measurement tips. By using pulse time-of-flight (ToF) to make its measurements, the SPG500n has greater insensitivity to environmental and material variations that can lead to calibration inaccuracies, as well as operator inconsistencies. The measurement is fundamentally non-contact, but for hand-held use, a measurement tip is used to aid the user in positioning the object at the focus of the THz beam. Key Features: Full Transceiver Functionality, No Need for Separate Transmitter and Receiver Collinear Design Two Measurement Ports With Potential to Use Both Ports at Once (HSC50yn) Cost-effective Plastic Lens TPX Lens for Low Loss (HXP51y2) Solvent Resistant Lens (SCS500n) Hardened Case for Industrial Environment, Tolerant to Dirt and Dust in the Factory Capable of Being Cleaned Safe in Explosive Environments (SCS500n) Single High-flex Umbilical, Long Umbilical Life in Scanner or Robot Simple Orientation to Target Variety of Focal Lengths Available: 25 mm (not All Models), 75 mm, 150 mm, Collimating Lens Polarization Extinction Ratio (PER): >20:1, Horizontal Beam Diameter: 38 mm (HXC51yn), 40 mm (HXC50yn, HSC50yn), 20 mm (HXP51y2) Sweep Rate: ≤8/s (LSG500n) Pointing Lasers to Guide Tool Alignment (LSG500n) Gauge Direction: 0°, 90° (SPG500n) Min. Layer Thickness: 50 µm (LSG500n), 10 µm (HXP51y2, Single Layer), 25 µm (HXP51y2, Buried Layer) Passline Tolerance: ±2 mm (HXP51y2, 150 mm Lens) Inexpensive to Replace if Damaged Extended Lifetime Replace Multiple Sensors Supports VRS Functionality (HXC51yn) Compatible With Various Motion Options Improve Product Quality by Optimizing Production Increases Product Gap for Density Measurements Operating Temperature Range: 0°C to +50°C Mounting Hardware: ¼-20 Threaded Mounting Holes Dimensions: 250 x 150 x 150 mm (LSG500n), 128 x 66 x 178 mm (HXC50yn, HXC51yn), 128 x 66 x 178 mm (HXP51y2), 76 x 67 x 152 mm (HSC50yn), 64 x 76 x 267 mm (SPG500n) Weight: 1.6 kg (HXC50yn, HXP51y2), 1.8 kg (HXC51yn), 1.1 kg (HSC50yn), 1 kg (LSG500n); 2 kg (SPG500n) Applications: Measure Layer Thickness; Produce Scanned Images; Industrial Process Control like Commercial Roofing, Foam Density, Adhesive Foams, Paint or Coating Thickness, Plastic Extrusion, Asphalt Shingles; Nondestructive Materials Inspection Applications like Aircraft Coatings, Packaged Goods, Radomes, Spacecraft, Pipeline Repairs, Void Detection, Subsurface Defects or Inclusions, Art Conservation; Converting Applications like Paper Coating, Multilayer Films, Tires; Terahertz Line Scan Imaging

Horizontal PER <20:1; Beam Diameter 38 mm; SNR 37-94.5 dB; Lens 25,75,150 mm, Collimating; Hot Swappable Luna’s T-Ray® 5000 is the first compact pulsed terahertz measurement system that is robust enough to be deployed in an industrial environment. With Luna’s T-Ray® 5000 HTS/HRS transmitters and receivers, the T-Ray® 5000 can be configured to fit your specific application. Operating in either reflection or transmission mode, the fiber-coupled transmitter/receiver heads deliver a picosecond duration time-domain terahertz pulse, allowing high speed, scanned images to be easily produced. Coupled with an HRS40n1 receiver, the transmitters provide bandwidth above 3.5 THz and signal to noise ratio above 70 dB (HTS40n1/2) or 55 dB (HTS40n3) The T-Ray® 5000 HTS40n1 Transmitter Type 1 provides high output power with high spectral bandwidth. The enhanced low frequencies provide higher material penetration for imaging voids and disbonds in high-frequency scattering media. By maximizing low-frequency power, the HTS40n1 is ideal for applications where high material penetration is required for imaging, particularly in scattering or absorbing materials. The T-Ray® 5000 HTS40n2 Transmitter Type 2 balances high output power with high spectral bandwidth and minimizes features following the pulse to allow high quality images and detection of multiple layers in reflection with less need for post processing of the waveform. By balancing bandwidth and power, the HTS40n2 is ideal for applications where both high-resolution imaging and broad spectral range are desired. The T-Ray® 5000 HTS40n3 Transmitter Type 3 provides uniform signal to noise over an extended range for high-resolution spectroscopy, while minimizing waveform distortions after the pulse to allow high resolution temporal measurement of layer thicknesses without the need for post processing of the waveform. By providing a uniform signal to noise over a broad bandwidth, the HTS40n3 is ideal for applications where both high resolution and broad spectral range are desired. The T-Ray® 5000 HRS40n1 Receiver provides high spectral bandwidth when coupled with any of the HTS40nm transmitters. The HRS40n1 provides bandwidth over 3.5 THz and signal to noise ratio above 70 dB. By embedding amplification close to the signal source, the receiver is able to produce high signal to noise, and eliminate the need for a lock-in amplifier. Key Features: Fiber-coupled to Allow Easy Movement Ultra-broadband Measurement Transmitted or Reflected Data Collection Mates With Collinear Adapter (AXA40n1) High Signal to Noise Ratio (SNR): 37 dB (@3.0 THz) to 94.5 dB (@0.1 THz), Typ., 1 min Average Polarization Extinction Ratio (PER): <20:1, Horizontal Beam Diameter: 38 mm Hot-swappable With Other Transmitters/Receivers Low Noise to Enable Rapid Data Collection Adjustable Lens Tube for Focusing Multiple Lenses Available: 25 mm, 75 mm, 150 mm, Collimating Lens Mounting Hardware: ¼-20 Threaded Mounting Holes Dimensions: 190.5 x 190.5 x 381 mm (HTS40n Transmitters), 70 x 64 x 70 mm (HRS40n1 Receiver) Weight: 275 g Applications: Terahertz Time Domain Spectroscopy; Gas, Liquid and Solid Spectroscopy; Nondestructive Materials Inspection; Package Inspection; Polymorph Discrimination; Semiconductor Wafer Inspection; Reaction Kinetics Monitoring; Medical and Biological Imaging Research; Sub-surface Corrosion Detection; Remote Threat Detection; Explosive Detection; Homeland Security; Converting Applications like Paper Coating, Multilayer Films, Tires

1, 2 Channels; Dynamic Range 16 Bit; Sampling Rate 100, 1,000 Hz; Max. Measurement Range 12-100 mm; 6 High-speed Encoder Inputs Luna’s T-Ray® 5000 measurement systems are amongst the fastest terahertz systems available on the market, with measured data processed within the control unit at a rate of up to 1 kHz. T-Ray® 5000 intelligent terahertz control units (TCUs) are the hearts of the system, monitoring and controlling all aspects of THz generation and detection. The TCU is paired with one of a variety of T-Gauge® Sensor heads to create a complete system. The data generated by the T-Gauge® sensor heads and processed by the T-Ray® 5000 control units enable multiple measurements of a product simultaneously. One T-Gauge® sensor can measure the basis weight, caliper thickness, multi-layer thicknesses, density and moisture content of a sample in a single pass. Attached to a separate transmitter and receiver, the T-Ray® 5000 control units can perform spectroscopic measurements as well as transmission and reflection imaging. The T-Ray® 5000 TCU52nm terahertz control unit monitors and controls all aspects of THz generation and detection, precisely delivering controlled optical signals to the terahertz transmitters and receivers, or the T-Gauge® Sensor Heads, enabling them to generate and receive terahertz signals. The T-Ray® 5000 TCU54nm dual channel control unit is the same size, shape and weight as the single channel unit (TCU52nm), but with the added benefit of being able to control two terahertz sensors for multi-sensor applications. The T-Ray® 5000 control units and accessories are linked with robust connection points and interfaces appropriate for industrial environments. Adequate connections are provided to allow seamless integration with most QC systems or experimental applications. The industry-standard interface connections make integration with the T-Gauge® Sensor straightforward. Key Features: Compact Enclosure One (TCU52nm) or Two (TCU54nm) Reflection Sensors Mates to Fiber coupled Sensor Head Lightweight Umbilical, Single Fiber to Each Head (TCU54nm) Integrated Data Processor Standard Monitor and USB Connections Digital Inputs Available for Measurement Control Easy to Install Integrates with Web Scanners and Robots Provides Measurements in Engineering Units Does Not Require Specialty Monitor or Keyboard Triggers for Bin Boundaries or Data Tagging Maximum Measurement Range: 12, 25, 50, 100 mm Measurement Rate: 100 Hz, 1000 Hz External Monitor Connection: VGA USB Ports: 4 Ethernet Ports: 3 Digital Interface: 16 Inputs & Outputs High-speed Encoder Inputs: 6 A/D Converter Dynamic Range: 16 Bit Power Supply: 110/240 VAC, <4 A Operating Temperature Range: 0°C to +50°C Dimensions: 445 mm x 546 mm x 191 mm Weight: 18.2 kg Applications: Industrial Process Control Like Commercial Roofing, Foam Density, Coating Thickness, Plastic Extrusion, Asphalt Shingles; Nondestructive Materials Inspection Like Aircraft, Packaged Goods; Radome Inspection, Spacecraft, Pipeline Repairs; Converting Applications Like Paper Coating, Multilayer Films, Tires, Top and Bottom Balance of Steel Cord Tire Play (TCU54nm); Scientific Applications Like Terahertz Imaging (Transmission and Reflection), Time Domain Spectroscopy; Thickness Measurement of Material Opaque to THz; Differential Measurement as Coatings or Layers Are Applied (TCU54nm); OD and ID Measurement of Large Diameter Pipe (TCU54nm); Four Point Measurement of Small Diameter Tubing (TCU54nm); Two Point Calender Control