1700-1750 nm; Output Energy ≤50 µJ; Repetition Rate ≤10 kHz; Pulse Width 2-5 ns; Pump Laser and OPO in Single Rugged Housing Our 170P0-1-50-S MID-IR tunable OPO (optical parametric oscillator) source combines pump laser and OPO in a single, rugged housing and generates laser pulses in the mid-infrared (MID-IR) range around 1700 nm – the applications for such wavelengths are mainly in the field of photoacoustic imaging, in addition to gas chromatography and other analysis tasks. The OPO’s wavelength can be tuned in an extended range from 1700 nm to 1750 nm. Other wavelength ranges (e.g. 1500 nm to 2000 nm) are available on demand. Using an electro-optical Q-switch, very short pulses with typical pulse widths of 2 ns to 5 ns are generated. If different wavelengths, repetition rates, pulse energies or pulse widths is what you are looking for, the laser experts at Elforlight (an AMS Company) are happy to specify, design and manufacture your customized OPO solution. Get in touch with us now to discuss your project’s requirements! Key Features: Tunable Wavelength Range: 1700 nm to 1750 nm (1500 nm to 2000 nm on request) Ideal for Cardiovascular Photoacoustic Imaging Pump Laser and OPO in Single Rugged Housing Operation Mode: Pulsed Pulse Width: 2 ns to 5 ns Pulse Repetition Rate: Up to 10 kHz Pulse Energy: 50 µJ @1 kHz, 30 µJ @5 kHz Beam Quality: Close to TEM00, M2 < 1.3. (Capable of Launch into Multimode Optical Fiber) Beam Profile: Circular Triggering: External Laser Pulse Trigger Option (Input Trigger Signal 5 V) Control: RS232 Interface With: Switch Laser On/Off, Set Laser Energy, Enable/Disable Emission Power Supply: 110 VAC to 240 VAC, 50/60 Hz, ~200 W Safety Features: Redundant Interlock, Warning Outputs Applications: Biomedical Photoacoustic Imaging; Gas Chromatography; Other

1940-1960 nm; Fixed or Tunable; Output Energy ≤250 µJ; Repetition Rate ≤5 kHz; Pulse Width 30-50 ns Teem Photonics’ passively and actively Q-switched DPSS lasers with a fixed wavelength of 1.95 µm or a tunable output from 1.94 µm to 1.96 µm delivers single longitudinal mode pulses with up to 250 µJ of energy per pulse. This laser features a pulse duration of 30 ns to 50 ns and a tunable repetition rate of up to 5 kHz. For further technical details please contact the AMS Technologies DPSS laser experts. Key Features: Wavelength: 1.95 µm (Fixed) or 1.94 µm to 1.96 µm (Tunable) Single Longitudinal Mode Energy per Pulse: Up to 250 µJ Pulse Duration (Width): 30 ns to 50 ns Repetition Rate: Tunable up to 5 kHz

Accessories for Mightex collimated LED light sources comprise dedicated focusing modules and interchangeable collimating lenses, lightguide, microscope and fiber-optic adapters, microscope illumination tubes, connector tubes, a thread converter, empty filter/optics holders, a lightguide holder for converting Type-B LCS into Type-B GCS as well as accessories for beam combiners like a push-pull adjustable mount, a 11 mm LCS adapter or connecting plates. Six different ACC-LCS-F-xx focusing modules for collimated LED light sources are available, comprising modules for 11 to 48 mm clear-aperture collimated LED light sources with working distances from 5 to 100 mm. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview” and the downloadable installation drawings. Eight ACC-LCS-C-xx(-B) additional interchangeable collimating lenses for collimated LED light sources are used to produce different beam sizes with the same LED light source base: Four models with clear apertures of 11, 22, 38 and 48 mm as well as four variants for Type-B light sources. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview”. Four different LCS-LGA22-xxx lightguide adapters can be used to couple light from a 22-mm-diameter collimated LED light source into a lightguide. Variants for lightguides with ferrule diameters of 5, 6.35 (1/4”), 7 and 11.1 mm as well as a ferrule length of 15 mm or greater are available. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview” and the downloadable installation drawings. Eight different ACC-BC25-xxx microscope adapters allow to connect LCS collimated LED light sources and beam combiners to microscopes. Single LCS light sources as well as LCS-BC25 beam combiners or WLS sources can be connected to microscopes like Leica DMI, Olympus (IX & BX, other), Zeiss Axioskop, Nikon Eclipse, Eclipse E200 and LV-UEPI/2/A. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview”. A LCS-FPC-ADP-SMA fiber-optic adapter can be used to couple light from a LCS-Series collimated LED light source (22-mm aperture) into a fiber patchcord and accepts SMA connectorized fiber patchcords. Three different ACC-BC25-MIT-xxx microscope illumination tubes allow to couple a beam combiner or LCS-Series collimated LED light source into the infinity optical path of microscopes. The lengths of these microsope illumination tubes are designed for one beam-combiner distance (up to two LCS sources) or two beam-combiner distances (up to four LCS sources). For details, please refer to the downloadable installation drawing. Three different ACC-LCS-xxx connector tubes for LCS-Series collimated LED light sources are available, comprising a male-to-male C-mount connector with inner threads, a female-to-female C-mount connector with outer threads and a 15 mm extension tube for 22 mm clear-aperture LCS-Series light sources. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview” An ACC-LCS-27C adapter is available for converting M27 thread to C-thread. Two different empty filter/optics holders for 22 mm clear-aperture collimated LED light sources are available (ACC-LCS-H-22, ACC-LCS-EH). Both are excitation filter holders for 25.4 mm (1”) diameter filters with up to 5 mm thickness, with ACC-LCS-EH featuring a threaded output end to connect to Mightex LCS-LGA22-xxx lightguide adapters or ACC-BC25-xxx microscope adapters. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview” and the downloadable installation drawing. Mightex’s GCS-LGH-B-0515 lightguide holder is used to replace the collimating lens on a Type-B LCS in order to convert it to a Type-B GCS. This holder is suitable for lightguides with a ferrule diameter of 5 mm (typical 3-mm-core lightguides) and a ferrule length of 15 mm or greater. Mightex’s ACC-LCS-BC25-PPM push-pull mount for multi-wavelength beam combiners is user-adjustable. Currently, Mightex’s multi-wavelength beam combiners can only be used to directly combine 22-mm-diameter collimated LED light sources. For 11-mm-diameter collimated LED light sources, an ACC-BC25-011 mechanical adapter can be used to attach the LED sources to the beam combiners, before the 11-mm-diameter collimated LED sources can be combined. Three different ACC-BC25-CP-01/02/03 connecting plates are available to connect two or more multi-wavelength beam combiners together, with four screws included. For details, please refer to the downloadable “Accessories for Collimated LED Light Sources Overview” and the downloadable product overview.

Accessories for Mightex LED light sources comprise lightguide collimators, dedicated focusing modules for collimated LED light sources, various cables, fiber-optic adapters, microscope illumination tubes, connector tubes for LCS-Series light sources, a thread converter, empty filter/optics holders, a lightguide holder for converting Type-B LCS into Type-B GCS as well as accessories for beam combiners like a push-pull adjustable mount, a 11 mm LCS adapter or connecting plates. Four different lightguide collimators are used to either couple light from free space into a lightguide or collimate light from a lightguide to form a collimated (parallel) optical beam. Lightguide collimators are key components with numerous applications. For example, a lightguide collimator can project light from a lightguide into a uniform spot in free space. High-numerical-aperture aspherical lenses are used for precise collimation and maximum light throughput. The collimators feature adjustable focus from ~100 mm to infinity. Various lightguide ferrule diameters are supported. Customization is available for other ferrule diameters. For further details, please refer to the downloadable datasheet and the downloadable “Accessories for LED Light Sources Overview”. Six different ACC-LCS-F-xx focusing modules for collimated LED light sources are available, comprising modules for 11 to 48 mm clear-aperture collimated LED light sources with working distances from 5 to 100 mm. For details, please refer to the downloadable “Accessories for LED Light Sources Overview” and the downloadable installation drawings. Four different cables are available for FCS-, FFC-, GCS-, WFC- and WLS-Series LED light sources. Some cables feature push-pull connectors and/or are suitable for 4-channel light sources. For details, please refer to the downloadable “Accessories for LED Light Sources Overview”. A LCS-FPC-ADP-SMA fiber-optic adapter can be used to couple light from a LCS-Series collimated LED light source (22-mm aperture) into a fiber patchcord and accepts SMA connectorized fiber patchcords. Three different ACC-BC25-MIT-xxx microscope illumination tubes allow to couple a beam combiner or LCS-Series collimated LED light source into the infinity optical path of microscopes. The lengths of these microsope illumination tubes are designed for one beam-combiner distance (up to two LCS sources) or two beam-combiner distances (up to four LCS sources). For details, please refer to the downloadable installation drawing. Three different ACC-LCS-xxx connector tubes for LCS-Series collimated LED light sources are available, comprising a male-to-male C-mount connector with inner threads, a female-to-female C-mount connector with outer threads and a 15 mm extension tube for 22 mm clear-aperture LCS-Series light sources. For details, please refer to the downloadable “Accessories for LED Light Sources Overview”. An ACC-LCS-27C adapter is available for converting M27 thread to C-thread. Two different empty filter/optics holders for 22 mm clear-aperture collimated LED light sources are available (ACC-LCS-H-22, ACC-LCS-EH). Both are excitation filter holders for 25.4 mm (1”) diameter filters with up to 5 mm thickness, with ACC-LCS-EH featuring a threaded output end to connect to Mightex LCS-LGA22-xxx lightguide adapters or ACC-BC25-xxx microscope adapters. For details, please refer to the downloadable “Accessories for LED Light Sources Overview” and the downloadable installation drawing. Mightex’s GCS-LGH-B-0515 lightguide holder is used to replace the collimating lens on a Type-B LCS in order to convert it to a Type-B GCS. This holder is suitable for lightguides with a ferrule diameter of 5 mm (typical 3-mm-core lightguides) and a ferrule length of 15 mm or greater. Mightex’s ACC-LCS-BC25-PPM push-pull mount for multi-wavelength beam combiners is user-adjustable. Currently, Mightex’s multi-wavelength beam combiners can only be used to directly combine 22-mm-diameter collimated LED light sources. For 11-mm-diameter collimated LED light sources, an ACC-BC25-011 mechanical adapter can be used to attach the LED sources to the beam combiners, before the 11-mm-diameter collimated LED sources can be combined. Three different ACC-BC25-CP-01/02/03 connecting plates are available to connect two or more multi-wavelength beam combiners together, with four screws included. For details, please refer to the downloadable “Accessories for LED Light Sources Overview” and the downloadable product overview.

Accessories for Mightex’s GCS-Series of lightguide-coupled LED light sources comprise an electrical cable (product number ACC-GCS-C05), a heatsink for 3 mm core liquid lightguides (product number ACC-LLG-HS-03), a range of liquid lightguides and lightguide adapters as well as lightguide collimators. Nine different LLG liquid lightguides are available in three wavelength ranges (300 to 650 nm, 340 to 800 nm and 420 to 2000 nm), with 3 or 5 mm core for 5 or 7 mm ferrule diameters respectively, a numerical aperture (NA) of 0.59 and lengths of 1 or 2 m. For details, please refer to the downloadable “Accessories for Lightguide-coupled LED Light Sources Overview” and the downloadable installation drawing. Four different lightguide adapters for Type-A GCS-Series lightguide-coupled LED light sources are available. Each Type-A GCS device comes with a standard lightguide adapter for 5 mm diameter ferrule (A0510). Other adapters (as well as additional standard adapters) can be purchased separately, for lightguides with ferrule diameters of 5, 6, 7 or 8 mm and ferrule lengths of 10 mm or greater. For details, please refer to the downloadable “Accessories for Lightguide-coupled LED Light Sources Overview”. Four different lightguide adapters for Type-B GCS-Series lightguide-coupled LED light sources are available, for lightguides with ferrule diameters of 5, 7, 8 or 10 mm and ferrule lengths of 15 mm or greater. For details, please refer to the downloadable “Accessories for Lightguide-coupled LED Light Sources Overview”. Four different lightguide collimators are used to either couple light from free space into a lightguide or collimate light from a lightguide to form a collimated (parallel) optical beam. Lightguide collimators are key components with numerous applications. For example, a lightguide collimator can project light from a lightguide into a uniform spot in free space.High-numerical-aperture aspherical lenses are used for precise collimation and maximum light throughput. The collimators feature adjustable focus from ~100 mm to infinity. Various lightguide ferrule diameters are supported. Customization is available for other ferrule diameters. For further details, please refer to the downloadable datasheet and the downloadable “Accessories for Lightguide-coupled LED Light Sources Overview”.

266, 355, 532, 1064 nm; Output Energy >1, >10, >25 µJ; Repetition Rate >70, 100, 150 kHz; Peak Power >6, >15, >38 kW; Pulse Width <0.65, <0.17 ns Teem Photonics’ ANx PicoOne and PicoMega amplified DPSS laser series is based on a microchip seeder and an efficient MOFA (Master Oscillator Fiber Amplifier) amplification stage. These lasers produce 650 or even 170 ps pulses at frequencies in excess of 100 kHz with a peak power exceeding 38 kW at 1064 nm. The laser operates with a single emission frequency. The Passively Q-switched (PQS) microchip laser technology and fiber amplification brought together with this laser series offers full control over the pulse energy (or peak power) while leaving unchanged the pulse width and pulse shape. Other seeders may also be used if different characteristics are required. The ANP-20E PicoOne amplified laser produces pulses of 1064 nm light with a nearly Gaussian beam output and an average power reaching 1.75 W, while the ANG-10E PicoOne amplified laser produces pulses of 532 nm light with an average power reaching 700 mW. Variants with 355 nm and 266 nm output are available on request, please contact AMS Technologies for detailed performance. Using the same platform as the PicoOne Series, the ANG-150P-000 PicoMega amplified laser brings passive Q-switching to a new realm. It generates ultra-short pulses (down to 120 ps) at repetition rates reaching 150 kHz. From LIDAR to high-throughput processing – in applications where ultra-short pulse width is a “must”, the PicoMega laser has a low cost of ownership compared to more complex ps lasers. It can be used as a seeder in applications where still higher power is needed. Key Features: Wavelengths: 266, 355, 532, 1064 nm Ultra-short Pulses, Pulse Width Down to Below 170 ps @100 kHz Peak Power: Up to >38 kW at 1064 nm (>15 kW at 532 nm) Excellent Beam Quality: Beam Profile Gaussian TEM00, M²<1.2, <1.3 Efficient, Air-cooled Sealed Package, Long Life Output Energy: >1 µJ, >10 µJ, >25 µJ Repetition Rate:  Up to 150 kHz  Applications: Micromachining; Material Processing; Selective Ablation of µm to nm Scale Layers; PCB Repair; Seeder for High-power Amplification; Instrumentation and LIDAR; (Time Gated) Raman Spectroscopy; Supercontinuum Generation; Ranging; Biophotonics; Dense Tissue Ablation

1527-1610 nm; Output Power 13-27 dBm; Termination Receptacle Style, FC/PC, FC/APC, ST, SC, SCA, LC, MU; C, C+L Band; Spectrum Flatness 1.0-2.0 dB OZ Optics’ ASE (Amplified Spontaneous Emission) broadband low coherence light sources are ideal instruments for optical component spectral measurement and system compliance testing in manufacturing and R&D environments. The new generation of ASE sources have no high-frequency ripples, which makes them very useful for sensor interrogation applications. ASE broadband light sources are available to cover the C-band, L-band, or both the C & L bands together. These are available with either a flattened spectral output for demanding applications, or a non-flattened response for less demanding or cost-sensitive applications. A range of output powers are available. The output light is accessed via a female fiber connector receptacle on the front panel. A variety of standard connector types are available. Custom connectors can also be accommodated. ASE broadband light sources are available in bench-top, rackmount or OEM module form factors. The basic version of the source features a built-in microprocessor for applications that require output power adjustment. RS-232 and USB interfaces are included, with the addition of a GPIB interface offered as an option. Key Features: High Output Power: 13 dBm (20 mW) to 27 dBm (500 mW) Wide Spectral Bandwidth Operating Wavelength Range (Typ.): 1527 to 1610 nm (Unflattened), 1531 to 1607 nm (Flattened) Spectrum Flatness (Typ.): 1.0 to 2.0 dB Covers C Band, L Band, or Both High Power Stability: 0.02 dB (1 h) Un-polarized Output Light Minimum Output Isolation: 45 dB Minimum Return Loss: 55 dB Termination: Receptacle Style, FC/PC, FC/APC, ST, SC, SCA, LC, MU Interfaces: RS232 and USB, GPIB Optional High Performance-to-cost Ratio Optional Built-in Attenuator and Optical Power Monitor Custom Design Flexibility Operating Temperature Range: 0 to +40°C Applications: Optical Component Testing; Telecom System Compliance Testing; EDFA Gain Spectrum Measurements; Optical Fiber Sensors and Sensing Systems; WDM by Spectral Slicing; Biomedical Imaging; Coherent Communication Systems

1529-1562 nm; Output Power 13 dBm; Termination Receptacle Style, FC/PC, FC/APC, ST, SC, SCA, LC, MU, None; C Band; Spectrum Flatness <±0.5 dB OZ Optics’ ASE-11 (Amplified Spontaneous Emission) broadband low-coherence light source is an ideal instrument for optical component spectral measurement and system compliance testing in manufacturing and R&D environments. The ASE-11 source comes with a flat spectrum with peak-to-peak ripples less than 1 dB over 1529 nm to 1562 nm, which makes it very useful for optical signal-to-noise ratio and sensor interrogation applications. The unit comes with a nominal 13 dBm output power and it is provided with an internal or external monitor port. The output light is accessed via a pigtailed 9/125 μm single mode fiber. A variety of standard connector types are available. Custom connectors can also be accommodated. The unit is packaged in a low-profile OEM box with built-in driver. Key Features: High Output Power: 13 dBm Flat Spectral Bandwidth With Ripple <±0.5 dB Operating Wavelength Range: 1529 to 1562 nm Covers C-band Spectrum Flatness: <±0.5 dB High Power Stability: 0.02 dB (1 h) Un-polarized Output Light High Performance-to-cost Ratio Optional Built-in Attenuator Pump TEC and Current Driver Included Output Isolation: 45 dB Return Loss: 55 dB Termination: Receptacle Style, FC/PC, FC/APC, ST, SC, SCA, LC, MU, None Internal or External Monitor Port Operating Temperature Range: 0 to +40°C Dimensions: 200 x 200 x 50 mm Applications: OSNR Measurement; Optical Components Testing; Telecom System Compliance Testing; Optical Fiber Sensors and Sensing Systems; WDM; Biomedical Imaging; Coherent Communication Systems

1528-1610 nm; Output Power ≥7-≥13 dBm; Termination SMF-28e Fiber Pigtail; C, C+L Band; Spectrum Flatness ≤2 dB; Output Connector: FC/PC, FC/UPC, FC/APC LightComm Technology’s ASE-C/CL ASE broadband light sources are available in desktop or miniature size module form factors. These light sources provide broadband spectra covering C band as well as C+L band with high stability and high output power. Key Features: Broadband Spectrum Output, Covering C band or C+L Band Operating Wavelength: 1528 to 1610 nm High Output Power: ≥7 to ≥13 dBm Spectrum Flatness: ≤2 dB (With GFF) Spectrum Density: ≥16 to ≥20 dBm/nm Spectrum Density Stability: ≤±0.5 dBm/nm (15 min) High Output Power Stability: ≤±0.02 dB (15 min), ≤±0.05 dB (8 h) Fiber Pigtail: Single Mode SMF-28e Output Connector: FC/PC, FC/UPC, FC/APC Operating Temperature: 0 to +40°C Power Supply: 230/110 VAC, 20 W (Desktop) Dimensions: 260x240x113 mm (Desktop), 90x70x16 mm (Mini Module) Applications: Fiber Grating; DWDM Filters; CWDM Filters; AWG Test and Manufacturing; Passive Fiber Optical Components Test; Optical Fiber Gyro and Fiber Sensors

Deuterium-Halogen; 200-2500 nm; Stability <1 mAU; Drift <0.25%/h; Optical Power 0.2, 7 µW; Power Supply 12 VDC, 450 mA Get the best of two worlds with Avantes’ AvaLight-DHc full range light source. It has both a deuterium light source and a halogen light source, providing you with adequate light between 200 and 2500 nm for nearly all absorbance chemistry applications. Deuterium emits light between 200 and 550 nm, whereas halogen emits light of up to 2500 nm. Coupling to the rest of your spectroscopy system is easy with the SMA connector. This light source is recommended in settings with large fiber cables or direct-attachment to a cuvette holder such as the CUV-DA, due to its relatively low output energy. The integrated TTL-shutter makes saving a dark measurement very simple in combination with AvaSoft (extra IC-DB26-2 needed). Optionally, the AvaLight-DHc is available in a rack-mountable version, to be used in the 19” rack or the 9.5” desktop system. A direct-attach cuvette holder CUV-DA is available for fluorescence or absorbance measurements. Key Features: Combined Deuterium-Halogen Light Source Integrated TTL-Shutter Wavelength Range: 200 to 2500 nm Stability: <1 mAU Warm-up Time: 1, 8 min Drift: <0.25%/h Optical Power (in 600 µm Fiber): 0.2, 7 µW Lamp Lifetime: 1000, 2000 h Temperature Range: 5 to 35 °C Power Supply: 12 VDC, 450 mA Dimensions: 175 x 110 x 44 mm Applications: Nearly All Absorbance Chemistry Applications

653-1120 nm; Spectral Width 2-10 nm; Output Power 1-19 W (CW), 1.8-90 W (Pulsed); Threshold Current ≤500-3000 mA; Slope Efficiency 0.6-1.0 W/A; Forward Current 1,6-100 A Toptica egleyard’s BAL series of multi mode laser diodes are high brightness, broad area laser (BAL) diodes operating multi mode spatially and longitudinally. Within the BAL series, wavelengths between 653 and 1,120 nm are available with output powers between 1 and 19 W in cw mode or even up to 90 W in pulse mode. Its high pulse energy and fast rise time makes the BAL series of multi mode laser diodes the laser source of choice for high resolution sensing applications under harsh environmental conditions. Stripe widths from 100 to 400 µm are available to optimize beam structure and power for the application. Toptica eagleyard’s hermetically sealed TO packages as well as C-mount or fiber pigtailed flat packages make such laser diodes ideally suited for applications with either demanding size restrictions or with preferred fiber pigtail handling. The output power of the fiber of a cost efficient pigtailed single emitter starts at 1 W and reaches up to 90 W peak in pulsed mode. Key Features: Broad Area, Edge Emitting Laser Diodes Broad Wavelength Range: 653 to 1,120 nm High Output Power: 1 to 19 W (CW) and 1.8 to 90 W (Pulsed) Hermetically Sealed Fast/Slow Axis Collimation Typ. Spectral Width: 2 to 10 nm Stripe Width: 100 to 400 µm Cavity Length: 1 to 4 mm Beam Divergence: Parallel (Slow Axis) 1.5° to 10° (FWHM), Perpendicular (Fast Axis) 0.6° to 30° (FWHM) Extreme Operating Temperature Range: -60 to +90 °C Packages: C-Mount, 9 mm TO TO with Thread, Integrated FAC/SAC, Flatpack With Window   Product Wavelength Output Power Operational Mode Package Specifics Downloads BAL-0653-01000-1510-CMT02-0000 653 nm 1 W CW C-Mount 2 mm Powerful, High Brightness, Longitudinally Multi Mode Datasheet BAL-0670-00001-1510-SOT23-0010 670 nm 1.5 W Pulsed TO-Can 9 mm Suitable for Harsh Environments Datasheet BAL-0670-00004-1510-SOT23-0010 670 nm 4 W Pulsed TO-Can 9 mm Suitable for Harsh Environments Datasheet BAL-0670-00010-1510-SOT23-0016 670 nm 10 W Pulsed TO-Can 9 mm Suitable for Harsh Environments Datasheet BAL-0808-00005-2013-SOT12-0010 808 nm 6 W Pulsed TO-Can 9 mm Suitable for Harsh Environments Datasheet BAL-0808-08000-4020-CMT04-0000 808 nm 8 W CW C-Mount 4 mm Suitable for Harsh Environments Datasheet BAL-0808-00020-4020-FLW01-0010 808 nm 20 W Pulsed Flatpack With Window Suitable for Harsh Environments Datasheet BAL-0808-00025-2013-SOT23-0016 808 nm 25 W Pulsed TO-Can 9 mm Suitable for Harsh Environments Datasheet BAL-0905-00010-1040-TOE02-0010 905 nm 12 W Pulsed TO With Thread Suitable for Harsh Environments Datasheet BAL-0905-00050-1040-TOE22-0010 905 nm 50 W Pulsed TO With Thread Suitable for Harsh Environments Datasheet BAL-0905-00090-1040-TOE22-0010 905 nm 90 W Pulsed TO With Thread Suitable for Harsh Environments Datasheet BAL-0980-08000-4020-CMT04-0000 980 nm 8 W CW C-Mount 4 mm Suitable for Harsh Environments Datasheet BAL-1064-08000-4020-CMT04-0000 1064 nm 8 W CW C-Mount 4 mm Suitable for Harsh Environments Datasheet   Applications: Time-of-Flight LIDAR; Laser Sensing in Missiles; Laser Ignitors of Optopyro Elements for Satellites or Launchers; Active Protection Systems; Material Processing; Medical; Solid-state Laser Pumping

1526-1563 nm; Output Power ≤17 dBm; Termination SM Fiber Pigtail, FC/APC Connector; Spectrum Flatness 1 dB Typ.; Full Temperature Power Stability ≤5% Beogold Technology's BG-ASE low-coherence broadband ASE (amplified spontaneous emission) light source is designed for industrial manufacturing and laboratory R&D applications. BG-ASE’s unique ATC and APC circuit control technology ensures very stable output power. The flattened ASE light source features high output power, low polarization and wide spectral width. The device is small and of high stability and reliability. With 5 VDC power supply and upper computer software, the user can read and set the module parameters via R232 communication serial port in real time. Module and benchtop structures are available for different needs. Key Features: Operating Wavelength Range: 1526 nm to 1563 nm Excellent Spectrum Flatness: 1 dB Typical (@ Room Temperature) Small Output Ripple High Adjustable Output Power: ≤17 dBm High Output Power Stability: ≤0.03 dB (Short Term), ≤0.2 dB (Long Term) Full Temperature Power Stability: ≤5% High Reliability Module and Benchtop Structures Available Customized Output Power and Configuration Operating Temperature Range: -45 °C to +85 °C Fiber Connector: SM Fiber Pigtail (Module), FC/APC or Customized (Benchtop) Communication Interface: RS232 (Module), RS232 Console or RJ45 (Benchtop) Power Supply: 5 VDC (Module), 220 VAC (Benchtop) Dimensions: 90 x 70 x 15 mm (Module), 260.6 x 162.8 x 76 mm (Benchtop) Applications: Fiber Optic Sensing; Component Test and Measurement; Medical and Biological Imaging; Fiber Optic Telecommunication

Signal/Idler Degeneracy Wavelength 1550 ±0.7² nm; Photon Pairs Bandwith FWHM 3 nm @ -3 dB Spectral Brightness; Noise Suppression >75 dB; Fidelity >98% OZ Optics' advanced entangled photon sources harness the high optical confinement within a periodically poled nonlinear waveguide (PPNW) to achieve exceptional efficiency and produce plentiful photon pairs. Utilizing spontaneous parametric down-conversion (SPDC) within a periodically poled lithium niobate (PPLN) type-2 waveguide, situated within a fiber-based Sagnac loop, photons are generated. The thermal stabilization of the PPNW ensures maintenance of the ideal phase matching condition. Following the creation of photon pairs, pump photons and associated fluorescence noise are efficiently filtered out from the remaining pairs using a built-in set of optical filters. This remarkable stability is attained through the self-compensation effect of an all-in-fiber Sagnac interferometer, complemented by a single-frequency external cavity laser operating at 775 nm with an ultra-narrow linewidth. Consequently, bright, high-performance, and low-noise entangled photon sources operating at room temperature are realized. The resulting polarization-entangled photon pairs are generated within a narrow spectral bandwidth of just a few nanometers in the C Band, with a center wavelength of 1550 nm. Key features: Highest counts/coincidence rate available in the market High Heralding efficiency and excellent fidelity Turn-key, highly stable, room temperature operation Rugged, alignment free, proprietary design Built-in noise-suppression filters Built-in stable pump laser with variable attenuator Customizable Applications: Quantum key distribution, quantum computing and information processing, quantum LIDAR, subsystem integrable for quantum communication  

Signal/Idler Degeneracy Wavelength 1550 ±0.6² nm; Photon Pairs Bandwith FWHM 80 nm @ -3 dB Spectral Brightness; Noise Suppression >75 dB; Fidelity >98% OZ Optics' advanced entangled photon sources leverage the high optical confinement within a periodically poled nonlinear waveguide (PPNW) to achieve remarkable efficiency and a rich abundance of photon pairs. These photons are produced through spontaneous parametric down-conversion (SPDC) within a periodically poled lithium niobate (PPLN) type-2 waveguide, nestled within a fiber-based Sagnac loop. Ensuring optimal phase matching, the PPNW is thermally stabilized. Upon photon pair creation, any residual pump photons and associated fluorescence noise are meticulously filtered out by an integrated set of optical filters. Exceptional stability is realized through the self-compensation effect of an all-in-fiber Sagnac interferometer, complemented by a single-frequency external cavity laser operating at 775 nm with an ultra-narrow linewidth. Consequently, these entangled photon sources deliver bright, high-performance outputs with minimal noise, operating comfortably at room temperature. The resulting polarization-entangled photon pairs exhibit a narrow spectral bandwidth of just a few nanometers in the C Band, centered at 1550 nm. Key features: Highest counts/coincidence rate available in the market High Heralding efficiency and excellent fidelity Turn-key, highly stable, room temperature operation Rugged, alignment free, proprietary design Built-in noise-suppression filters Built-in stable pump laser with variable attenuator Customizable Applications: Quantum key distribution, quantum computing and information processing, quantum LIDAR, subsystem integrable for quantum communication  

1045 nm; Repetition Rate 15-40 MHz; Pulse Width <80 fs; Average Output Power >2 W; Peak Power >1 MW Litilit’s Biolit 2 is a compact, air-cooled femtosecond fiber laser for biophotonics, designed with multiphoton microscopy and other nonlinear optics applications in mind. The industrial-grade device is exceptionally robust, affordable and maintenance-free. Clean pulses lead to sharp images : A combination of very short (typ. 60 fs) and clean pulses, high beam quality and lower repetition rate – compared to solid-state siblings – enables unparalleled multiphoton imaging while preserving the object. Key Features: Robust and Stable Very Short and Clean Pulses Maintenance-free & Turn-key Integrated Tunable Dispersion Pre-compensation: -5,000 fs² to +1,000 fs² Passively Air-cooled Central Wavelength: 1045 ±5 nm Average Power: >20 W Pulse Duration: <80 fs (60 fs Typ.) Pulse Strehl Ratio: >0.9 Flexible Pulse Repetition Rate, Optimized for Multiphoton Microscopy: 15, 20, 30 or 40 MHz Peak Power: >1 MW (@20 MHz) Beam Quality: M²<1.2 Beam Circularity: >0.9 Beam Diameter: 1.5 ±0.5 mm Beam Pointing: <50 µrad pk-to-pk Pulse Energy Stability (RMS): <1% Laser Control Interface: CAN, USB Power Stability (RMS): <1.0% Power Supply: 100 to 240 VAC, 47 to 63 Hz, 300 W Cooling Laser Head: Air (Passive) Cooling Control Unit: Forced Air (Fans) Operating Temperature: +15 to +35°C Dimensions Laser Head: 266 x 190 x 112 mm Dimensions Control Unit: 449 x 370 x 140 mm Applications: Multiphoton Microscopy; Photopolymerization; Ophthalmology; OPO Pumping

Wavelength 795-1927nm; Power 5-40 W; Fiber Core Diameter 105-1000 µm Applications: Pumping Rb Vapor, Spin Exchange Optical Pumping (SEOP); Pumping DPSSL; Fiber-Coupled Module for Pumping DPSSL; Fiber Lasers; Surgery, Fat Reduction, Materials Processing; Skin Rejuvenation; Varicose Vein Treatment; Fiber-Coupled Module for Varicose Vein Treatment; Pumping Er:YAG Lasers; Wavelength Stabilized Diode Laser for Pumping Er:YAG Crystal; Fiber-Coupled Module for Medical Applications; Aesthetics; Illumination; Nerve Stimulation. Item number Series Wavelength Power Fiber Core Diameter  Additional Information Applications Downloads 6109-0000 BrightLock® Ultra-50 795 nm 25 W 1000 µm Spectrally Narrowed Pumping Rb Vapor, Spin Exchange Optical Pumping (SEOP) Datasheet 6008-1118 BrightLock® Ultra-50 808.5 nm 30 W 400 µm Wavelength Stabilized Pumping DPSSL Datasheet 6108-0007 BrightLock® Ultra-50 880 nm 40 W 400 µm Wavelength Stabilized Pumping DPSSL Datasheet 6108-0000 BrightLase® Ultra-50 888 nm 40 W 400 µm Medica Options Fiber-Coupled Module for Pumping DPSSL Datasheet 6107-0000 BrightLock® Ultra-50 976 nm 25 W 200 µm Wavelength Stabilized Pumping DPSSL and Fiber Lasers Datasheet 6019-0007 BrightLase® Ultra-50 1064 nm 35 W 400 µm Medica Options Surgery, Fat Reduction, Materials Processing Datasheet 6119-0000 BrightLase® Ultra-50 1410 nm 5 W 105 µm Medica Options Skin Rejuvenation Datasheet 6018-M003 BrightLase® Ultra-50 1470 nm 12 W 200 µm Medica Options Surgery, Varicose Vein Treatment Datasheet 6015-0007 BrightLase® Ultra-50 1470 nm 17 W 400 µm Medica Options Fiber-Coupled Module for Varicose Vein Treatment Datasheet 6015-0010 BrightLase® Ultra-50 1470 nm 8 W 105 µm Medica Options Pumping Er:YAG Lasers Datasheet 6115-0000 BrightLock® Ultra-50 1532 nm 15 W 400 µm Wavelength Stabilized Wavelength Stabilized Diode Laser for Pumping Er:YAG Crystal Datasheet 6015-M100 BrightLase® Ultra-50 1532 nm 15 W 300 µm Medica Options Fiber-Coupled Module for Medical Applications Datasheet 6014-M002 BrightLase® Ultra-50 1540 nm 12 W 105 µm Medica Options Aesthetics, Skin Rejuvenation Datasheet 6014-M001 BrightLase® Ultra-50 1550 nm 15 W 400 µm Medica Options Illumination, Skin Rejuvenation, Surgery Datasheet 6014-0017 BrightLase® Ultra-50 1875 nm 5 W 400 µm Medica Options Surgery, Nerve Stimulation Datasheet 6014-0019 BrightLock® Ultra-50 1908 nm 6 W 400 µm Wavelength Stabilized Wavelength Stabilized Diode Laser for Pumping Ho:YAG Crystals Datasheet 6010-M006 BrightLase® Ultra-50 1927 nm 2.5 W 105 µm Medica Options Skin Rejuvenation Datasheet

Wavelength 888-1908 nm; Power 40-350 W; Fiber Core Diameter 400-800 µm Applications: Pumping DPSSL; Resonant Pumping; High Power Diode Laser for Lung and Liver Surgery; Fiber-Coupled Diode Laser for BPH (Benign Prostate Hyper-Growth) Surgery; Wavelength Locked Diode Laser for Pumping Er:YAG; Fiber-Coupled Bar-Based Modules; Fiber-Coupled Module for Transparent Plastic Welding; Wavelength Locked Diode Laser for Pumping Ho:YAG. Item number Series Wavelength Power Fiber Core Diameter  Additional Information Applications Downloads 6508-0001 BrightLock® Ultra-500 880 nm 350 W 800 µm Wavelength Stabilized Pumping DPSSL, Resonant Pumping Datasheet 6408-0004 BrightLase® Ultra-500 888 nm 250 W 400 µm Medica Options Pumping DPSSL, Resonant Pumping Datasheet 6413-M200 BrightLase® Ultra-500 1318 nm 150 W 600 µm Medica Options High Power Diode Laser for Lung and Liver Surgery Datasheet 6414-0001 BrightLase® Ultra-500 1470 nm 100 W 400 µm Medica Options Fiber-Coupled Diode Laser for BPH (Benign Prostate Hyper-Growth) Surgery Datasheet 6515-0000 BrightLock® Ultra-500 1532 nm 90 W 400 µm Wavelength Stabilized Wavelength Locked Diode Laser for Pumping Er:YAG Datasheet 6415-0002 BrightLase® Ultra-500 1540 nm 150 W 600 µm Medica Options Fiber-Coupled Bar-Based Modules Datasheet 6417-0001 BrightLase® Ultra-500 1710 nm 60 W 400 µm Fiber-Coupled Module with Options Fiber-Coupled Module for Transparent Plastic Welding Datasheet 6519-0004 BrightLock® Ultra-500 1908 nm 60 W 600 µm Fiber-Coupled Module with Options Wavelength Locked Diode Laser for Pumping Ho:YAG Datasheet 6519-0002 BrightLock® Ultra-500 1908 nm 40 W 600 µm Wavelength Stabilized Wavelength Locked Diode Laser for Pumping Ho:YAG Datasheet

Wavelength 795-1470nm; Power 25-120 W; Fiber Core Diameter 200-1000 µApplications: Pumping Rb Vapor; Spin Exchange Optical Pumping; Pumping DPSSL; Resonant Pumping; Pumping Fiber Lasers; Fat Reduction; Surgery; Materials Processing; Diode Laser for Pain Relief and Wound Healing; Fiber-Coupled Bar-based Modules; Pumping Er:YAG Lasers; BPH Treatment; Diode Laser for Transparent Plastic Welding. Item number Series Wavelength Power Fiber Core Diameter  Additional Information Applications Downloads 6307-0002 BrightLock®Ultra-100 795 nm 75 W 1000 µm Wavelength Stabilized Pumping Rb Vapor, Spin Exchange Optical Pumping Datasheet 6308-0005 BrightLock®Ultra-100 880 nm 120 W 400 µm Wavelength Stabilized Pumping DPSSL, Resonant Pumping Datasheet 6208-0006 BrightLase® Ultra-100 888 nm  100 W 400 µm  Fiber-coupled Module Pumping DPSSL Datasheet 6309-0004 BrightLock®Ultra-100  976 nm 75 W 200 µm Wavelength Stabilized Pumping DPSSL, Pumping Fiber Lasers Datasheet 6309-0001 BrightLock®Ultra-100  976 nm 120 W 400 µm Wavelength Stabilized Pumping DPSSL, Pumping Fiber Lasers Datasheet 6210-0007 BrightLase® Ultra-100 1064 nm 120 W 400 µm Fiber-coupled Module Fat Reduction, Surgery, Materials Processing Datasheet 6212-M002 BrightLase® Ultra-100 1270 nm 40 W 400 µm Medica Features Diode Laser for Pain Relief and Wound Healing Datasheet 6213-M002 BrightLase® Ultra-100 1320 nm 45 W 400 µm Medica Features Fiber-Coupled Bar-based Modules Datasheet 6214-M002 BrightLase® Ultra-100 1470 nm 45 W 400 µm Medica Features Fiber-Coupled Bar-based Modules Datasheet 6214-0011 BrightLase® Ultra-100 1470 nm 18 W 105 µm Fiber-Pigtailed Module Pumping Er:YAG Lasers Datasheet 6214-0002 BrightLase® Ultra-100 1470 nm 45 W 400 µm Medica Features Surgery, BPH Treatment Datasheet 6315-0003 BrightLock®Ultra-100 1532 nm 25 W 200 µm Wavelength Stabilized   Datasheet 6315-0002 BrightLock®Ultra-100  1532 nm 40 W 400 µm Wavelength Stabilized   Datasheet 6217-0003 BrightLase® Ultra-100 1710 nm 30 W 400 µm Optional Aiming Beam Diode Laser for Transparent Plastic Welding Datasheet

1040 nm; Pulse Energy 5->35 nJ; Pulse Repetition Frequency 100 MHz; Pulse Duration <150 fs; Output Power ≤0.5 ->3.5 W Chromacity 1040 is a reliable, fixed wavelength, femtosecond laser source for two-photon microscopy that delivers ultrashort pulses with high average powers in the near-IR. Chromacity’s fiber-based femtosecond laser source allows to exploit the well-known advantages of Yb-doped fibers as gain media, while delivering high quality and high-power ultrashort pulses. The 1040 nm femtosecond laser is ideal for multiphoton excitation (MPE) by coupling into microscope systems, empowering users to produce clear and high-resolution images, as a result of its excellent beam quality, ultrafast pulses and high average power levels. Learn how the femtosecond laser source is ideal for two-photon microscopy. The Chromacity 1040 femtosecond laser is engineered with a custom-designed and temperature-controlled baseplate, providing an unprecedented level of ruggedness and reliability for this type of laser architecture. The Chromacity 1040 is the next generation in femtosecond laser systems, which no longer need hours in set-up time. The light emitted from the laser originates from a single mode fiber, ensuring superior beam quality. This laser source does not require water cooling and comes with a simple user interface, making it one of the easiest laser sources to operate. Key Features: Compact Laser Housing Air-cooled Operation Intuitive Web Browser Interface Power-efficient Laser Cavity (Low Power Consumption) Low-, Mid-, and High-Power-Versions Available Output Power: ≤0.5 W (Low-Power), 2.5 W (Mid-Power), >3.5 W (High-Power) Wavelength: 1030 nm (Low-Power, 1040 nm (Mid-Power, High-Power) Pulse Duration: <150 fs (Chirped Output Pulse Option Available) Pulse Energy: 5 nJ (Low-Power), 25 nJ (Mid-Power), >35 nJ (High-Power) Pulse Repetition Frequency: 100 MHz (Other Repetition Frequencies Available) Beam Parameters: Free Space, M2 <1.2, Linearly Polarized, Divergence <2 mrad TEM00 Beam Ideal for Coupling into a Range of Microscopes Beam Diameter: 0.5 mm to 1.2 mm Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Cooling: Air-cooled Electrical: 110-240 VAC, 50-60 Hz, 80 W Dimensions 1040 Module: 426 mm x 250 mm x 108 mm (LxWxH) Dimensions Control Unit: 483 mm x 285 mm x 88 mm (LxWxH, 19’’ 2U Rack-mount) Applications: SHG and Multi-photon Microscopy; Light Sheet Microscopy; Optogenetics Imaging Experiments; Pump Source for Non-linear Optics (OPOs, SHG); THz Generation; Supercontinuum Generation; Time Resolved Experiments (e.g. TCSPC/FLIM)

1280 nm; Pulse Energy 300 pJ; Repetition Rate 100 MHz; Pulse Duration 80 fs; Output Power ≤30 mW The Chromacity 1280 femtosecond laser generates femtosecond pulses, with a fiber delivery output, to drive advances in test and measurement applications within the semiconductor industry. While operating at 1280 nm, Chromacity’s ultrafast laser can also generate 80 fs pulses across the 1250 nm to 1310 nm wavelength range, and combined with excellent beam quality, the Chromacity 1280 has scope to broaden fundamental research and material characterization capabilities. The 1280 nm laser inherits Chromacity’s novel laser design architecture and patented manufacturing expertise to develop a high-performance and truly stable light source, which is operationally ready with minimal set-up time. Within the range of typical applications for this laser, laser scanning and optoelectronic imaging of integrated circuits is crucial towards optimal semiconductor failure analysis, at a time when the industry faces global chip shortages. With seamless integration into Laser Assisted Device Alteration (LADA) platforms, Chromacity’s robust 1280 nm laser source can help determine soft defect localization, using near-IR microscopy techniques including (2P-LADA). Further applications include Two-Photon Laser Assisted Device Alteration (2P-LADA), a high-resolution imaging technique which exploits two-photon absorption (TPA) to deliver precise three-dimensional localization of the photocarriers, injected by the TPA process, to accurately locate and characterize failures, with optimum spatial and temporal performance. Similarly, the Two-Photon Optical Beam Induced Current (TOBIC) technique is another laser-scanning method for imaging integrated circuits. This technique uses ultrashort-pulse lasers to induce a photocurrent which is subsequently mapped to generate an image. TOBIC imaging occurs around 1250 nm to 1550 nm, where the beam is easily transmitted through the silicon band gap. Key Features: Fiber Output Compact Laser Housing Air-cooled Operation Intuitive Web Browser Interface Remote Installation Capability Output Power: Up to 30 mW From Fiber-coupled Output Peak Power: 4kW Wavelength: 1280 nm Spectral Bandwidth: 80 nm Pulse Duration: 80 fs Pulse Energy: 300 pJ Repetition Rate: Locked to 100 MHz Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Cooling: Air-cooled Electrical: 110-240 VAC, 50-60 Hz, 80 W Dimensions 1280 Module: 614 mm x 304 mm x 96 mm (LxWxH) Applications: Two-photon Laser-assisted Device Alteration (2p LADA) in Silicon Integrated Circuits; Two-photon Optical Beam Induced Current (TOBIC); Material Characterization; Fundamental Research; Interrogating Photonics Integrated Circuits (PIC)

520 nm; Pulse Energy 20 nJ; Pulse Repetition Frequency 100 MHz; Pulse Duration <150 fs; Output Power ≤2 W Chromacity 520 is a robust and reliable 520 nm fixed wavelength femtosecond laser source for biomedical imaging and semiconductor applications that delivers ultrashort-pulses with high average powers in the green. Pumped by high-quality pulses from Chromacity’s 1040 nm laser Chromacity1040, second-harmonic light at 520 nm is efficiently generated with sub-150-fs pulse durations. This second harmonic generation (SHG) module can be coupled with the Chromacity 1040 to generate up to 2 W of average power. The compact housing enables simple system integration, and a fiber delivery option is also available. The Chromacity 520 laser source does not require water cooling and comes with a simple user interface, making it one of the easiest and affordable laser sources to operate. Remote installation can be provided. Tailored to your needs: The Chromacity 520 is engineered with a custom-designed and temperature-controlled baseplate, providing an unprecedented level of ruggedness and reliability for this type of laser architecture. Chromacity also offers a range of pulse repetition frequencies to meet your requirements, making this a laser source that can easily integrate into a number of different applications. Contact AMS Technologies for details! Key Features: Compact Air-cooled System Remote Installation Capability Plug & Play Functionality Simple OEM Integration Fiber Delivery Capability Competitive Price Point Output Power: Up to 2 W Wavelength: 520 nm Pulse Duration: <150 fs Pulse Energy: 20 nJ Pulse Repetition Frequency: 100 MHz (Other Repetition Frequencies Available) Access to 1040 nm Pulses Beam Parameters: Free Space, Linearly Polarized Beam Diameter: 1.0 mm (±0.2 mm) Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Cooling: Air-cooled Electrical: 110-240 VAC, 50-60 Hz, 80 W Power Supply: 19” 2U Rack-mount Unit Dimensions 520 Module: 240 mm x 114 mm x 90 mm (LxWxH) Dimensions Pump Source Laser Head: 426 mm x 250 mm x 108 mm (LxWxH) Dimensions Power Supply Unit: 483 mm x 255 mm x 177 mm (LxWxH, 19’’ 2U Rack-mount) Applications: Pump Source for OPO; Non-linear Optics; Measuring Fluorescence Lifetimes; Telecoms; Quantum Imaging; Photo-dynamic Therapy; Nanophotonics; Picosecond Ultrasonics; Semiconductor Applications like Detection of Photomask Defects via an Ultrasonics Technique

920 nm; Pulse Energy 12.5-20 nJ; Pulse Repetition Frequency 80 MHz; Pulse Duration <180 fs; Output Power 1.1 W Chromacity 920 is a highly stable 920 nm femtosecond laser to achieve your two-photon microscopy goals. This 920 nm femtosecond laser is the next generation of fiber-based technology which is enhancing multiphoton imaging with higher resolution and faster acquisition at significant depth. The 920 nm femtosecond laser is ideal for multiphoton excitation (MPE), particularly two-photon excitation of fluorophores and calcium markers (including YFP, GFP, eGFP, GCaMP). Chromacity’s range of ultrafast lasers are distinctively quick and simple to install, with an intuitive user-interface to guide ease of operation. Fiber coupling capability reinforces seamless integration into microscopy set-ups for fundamental research and industrial applications, with maximum optical power transmission and minimal dispersion of the femtosecond pulses. With the advent of the Chromacity 920 to complement Chromacity’s 1040 femtosecond laser, these truly-stable fiber-based systems equip researchers to make new discoveries in biomedical imaging. Key Features: Compact Air-cooled System Remote Installation Capability Plug & Play Functionality Simple OEM Integration Fiber Delivery capability Competitive Price Point Output Power: 1.1 W Wavelength: 920 nm Bandwidth: 17 nm Pulse Duration: <180 fs Pulse Energy: 12.5 nJ to 20 nJ (Depending on Repetition Frequency) Pulse Repetition Frequency: 80 MHz (Configurable at the Point of Manufacture) Beam Parameters: Free Space, M2 <1.2, Divergence <0.3 mrad (Half Angle) TEM00 Beam Ideal for Coupling into a Range of Microscopes Beam Diameter: 2 mm (±0.2 mm) Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Cooling: Air-cooled Electrical: 110-240 VAC, 50-60 Hz, 80 W Power Supply: 19” 2U Rack-mount Unit Dimensions 920 Module: 355 mm x 180 mm x 118 mm (LxWxH) Dimensions Control Unit: 483 mm x 285 mm x 88 mm (LxWxH, 19’’ 2U Rack-mount) Applications: Multiphoton Microscopy; Second Harmonic Generation (SHG) Microscopy; Light Sheet Microscopy; Time-resolved Photoluminescence Spectroscopy; FLIM; THz Generation; Optogenetics; Pump Source for Nonlinear Optics

1.4-12 µm; Output Power 20-850 mW; Repetition Frequency 100, 200 MHz; Pulse Duration 1-5 ps; Beam Diameter 1-6 mm Chromacity has developed a range of tunable laser sources which span the short to long IR wavelength regions. The Chromacity Auskerry (formerly the Near-IR OPO) is Chromacity’s flagship tunable optical parametric oscillator (OPO) which generates light across 1.4 µm – 4.2 µm (7150 cm-1– 2400 cm-1). The Chromacity Auskerry tunable laser source can be integrated into an FTIR spectrometer, providing the ability to interrogate multiple chemical signatures in real time (at a high resolution). It has a broad bandwidth across the 3µm-3.5µm to quantify gases such as of methane, ethane and benzene in a single measurement with resolutions of 0.05cm-1. The high powers of the Chromacity Auskerry have demonstrated open-path stand-off detection measurements beyond 100m. The Chromacity Haskeir (formerly the Mid-IR OPO) is powered by a new generation of non-linear crystals which generate broad bandwidth coherent light across the long wavelength regions between 4.5 µm and 12 µm (2200 cm-1 to 850 cm-1). Spectroscopy across the fingerprint regime provides that ability to characterize volatile organic compounds with complex chemical signatures, and the high brightness of the Chromacity Haskeir OPO across 4.5 to 12µm can be used in a number of these set-ups. It can also be used to characterize and differentiate between compounds, such as VX and Sarin, as well as pharmaceutical powders such as aspirin and ibuprofen. Both picosecond OPOs deliver high power, broad band coherent light and are optically pumped by Chromacity’s high-power Chromacity 1040 femtosecond laser, which is fully integrated into the optical head to maximize stability and reduce the overall system footprint. Fiber delivery capability reinforces the inherent stability of Chromacity’s OPO systems and seamless OEM integration for industrial applications. Chromacity is the first laser manufacturer to remotely install ultrafast OPOs. Patent protected manufacturing and design processes have driven Chromacity to build truly robust and affordable OPO systems with drop-ship capability and plug & play functionality. With a wealth of expertise in optical parametric oscillator technology, non-linear optics and optical fiber delivery, the Chromacity team are able to consider a wide range of options to help meet your requirements. If you have a specific request, please don’t hesitate to contact AMS Technologies. Key Features Chromacity Auskerry: Compact Laser Housing With an Integrated Pump Source Coherent Beam With Broadband Coverage Intuitive Web Browser Interface Remote Installation Capability Signal Wavelength: 1.4 µm to 1.8 µm Pulse Duration: ~1 ps to 5 ps Signal Average Power: Up to 850 mW (@1.5 µm) and >350 mW Across the Range Idler Average Power: Up to 350 mW (@3.3 µm) With >200 mW Across the Range Idler Wavelength: 2.4 µm to 4.2 µm Pump Source: Fully Integrated Chromacity 1040 Pump Laser Residual Pump Power (@1040 nm): >300 mW (Depending on OPO Wavelength) Repetition Frequency: 100 MHz Beam Diameter: Signal 1 mm to 2 mm, Idler 3 mm to 6 mm Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Cooling: Air-cooled Electrical: 110-240 VAC, 50-60 Hz, 80 W Dimensions Chromacity Auskerry Module: 814 mm x 255 mm x 86 mm (LxWxH) Dimensions Control Unit: 483 mm x 285 mm x 86 mm (LxWxH) Key Features Chromacity Haskeir: Output Wavelength Tunability: Across 4.5 µm to 12 µm (2000 cm-1 to 850 cm-1) Output Power: Up to 100 mW @4.5 µm to 7 µm, Up to 20 mW @12 µm Quasi-CW, Providing Instantaneous Broad Bandwidth Spectra Repetition Frequency: 100 MHz or 200 MHz Available Pump Source: Fully Integrated Chromacity 1040 Pump Laser Remote Installation Capability Control Interface: Web Browser Interface, Ethernet and Serial Port (RS232) Also Available Crystals with Different Central Wavelengths Available Crystal Specifications: Quasi-phase Matching Crystal Design – Wavelength Tuning via Multi-grating (Discrete) or Fan-out (Continuous) Structures Pump Source: Integrated 1040 Pump Source (Access to Depleted 1040 Pump on Request) Cooling: Air-cooled, No Water Required Electrical: 110-240 VAC, 50-60 Hz, 80 W Dimensions Chromacity Haskeir Module: 970 mm x 245 mm x 82 mm (LxWxH) Dimensions Control Unit: 483 mm x 285 mm x 86 mm (LxWxH) Weight: 16 kg (Laser Head), 2 kg (Control Unit) Applications: Laser Spectroscopy, Including FTIR Spectroscopy, Stand-off Detection, Identification of Volatile Compounds; Nonlinear Physics Research; Material Characterization; Interrogation of Photonics Integrated Circuits (PIC); Multi-species Gas Analysis; Telecoms; Quantum Research; Explosive Detection

375 to 785 nm; 18 to 120 mW; Beam Size 0.8 to 1.3 mm Circular, 1x2 to 4x1 mm Elliptical Blue Sky Research’s CHROMALASE II™ series of high-performance laser diode modules has been optimized to meet the demanding performance requirements of medical, life sciences and automated instrumentation. These laser diode modules incorporate highly integrated sophisticated electronics for laser drive and protection, modulation and feedback functions. The CHROMALASE II ultra-compact stand-alone assembly is RoHs compliant and can be ordered with a variety of collimation optics which allows easy integration into your system. A wide variety of wavelength and power options are available including the very popular 405, 488, 532 and 635 nm products. Blue Sky Research’s CHROMALASE II design incorporates standardized control and alarm firmware, protection circuitry and low-noise operation into a compact, stand-alone assembly. Everything you need to operate this laser from a simple 12 VDC supply is integrated in the laser module. The CHROMALASE II laser diode modules are temperature stabilized with a thermoelectric cooler (TEC), and the integrated controller includes laser driver, output power stabilization, adjustable power level control, modulation capability, reverse and over voltage protection and ESD-fast transient suppression circuitry. Each semiconductor laser diode system can be ordered with or without Blue Sky Research’s patented “µLens” or micro-optic beam correction optics. Systems with µLens will have near perfect Gaussian and circular beam shapes and corrected laser diode wave front distortions. Laser systems without the micro-optic beam correction have all the advantages of Blue Sky Research’s small, highly integrated packaging while retaining the standard elliptical shape (typical 3:1 aspect ratio) of semiconductor lasers. For the CHROMALASE II series of fiber-coupled diode laser modules the dedicated power supply CLPS is available as an accessory. This device provides up to 2.5 A of current for laser diode and TEC and allows the operation of the CHROMALASE II series from standard power sockets with 100 to 240 VAC. Key Features: Diffraction Limited Optical Performance Wavelength Range: 375 to 785 nm Variable Laser Diode Power: 18 to 120 mW (Depending on Wavelength) Power Stability (2 h): <0.5% Configurable Launch Optics Simplify OEM Integration Circular (0.8 to 1.3 mm) or Elliptical (1x2 to 4x1 mm) Output Beams Integrated Drive and Power Electronics Electrical Power Consumption: <12 W Optical Noise (RMS): <0.5% Beam Alignment Accuracy: <5 mrad Beam Pointing Stability <10 µrad/°C Solid State Reliability Applications: Analytical Instruments; Biomedical & Medical; Flow Cytometry; Confocal Microscopy; Ophthalmology; Defense & Homeland Security