STx Series High-performance Triggered Microchip DPSS Lasers

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

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

Actively Q-switched DPSS Lasers; 365, 532, 1064 nm; Pulse Energy >100->400 µJ; Repetition Rate ≤10 kHz; Min. Pulse Width <4, <5 ns; Jitter <±1 ns Our FQS range of DPSS lasers builds on the very successful SPOT actively Q-switched laser technology. Adopting key technical design features, the FQS range provides a series of models delivering up to 400 µJ with pulse widths of less than 5 ns. The FQS lasers’ jitter is maintained at a low level across the range. The compact laser head can be used to pump our dye laser products to produce a comprehensive range of wavelengths. The UV variant of the FQS has been very successful as a light source for MALDI (Matrix Assisted Laser Desorption/Ionization) applications. Key Features: Wavelengths: 355, 532, 1064 nm Pulse Energy @1 kHz: >100 µJ to >400 µJ Repetition Rate: ≤10 kHz Minimum Pulse Width: <4 ns, <5 ns Jitter: <±1 ns (typ. ± 0.5 ns) WRT ext. trigger input Spatial Mode: TEM00, M² <1.2 Beam Diameter: 1 mm at Output Aperture Beam Divergence: <1 mRad at 1 mm Diameter Polarization: >100:1 Variable Power Output RS232 Control Manual Safety Shutter User Interface (Interlock, On/Off Switch) Air Cooled External Trigger Laser Diode Protection 19” Rack Power Supply Universal Mains Input: 100 to 240 VAC, 50/60 Hz Max. Power Consumption: 1000 W Dimensions Laser Head: 240 mm x 210 mm x 100 mm Dimensions Power Supply: 19 Inch Rack, 2U High Applications: Photoacoustic Imaging; MALDI Mass Spectrometry (Matrix Assisted Laser Desorption/Ionization); Pumping of Dye Lasers / OPOs / Raman Lasers; LIDAR; Micromachining

532, 1064 nm; Output Energy >45, >72 µJ; Repetition Rate >70 kHz; Peak Power >100, >200 kW; Pulse Width <0.65 ns Teem Photonics’ HNx PicoSpark™ Series of amplified microchip DPSS lasers combines multi-watt average output power level with high repetition rate and exceptional pulse characteristics to provide the best price/quality ratio for micromachining applications. Passively Q-switched (PQS) microchip laser technology and fiber amplification are brought together, delivering pulses with hundreds of kW peak power and hundreds of GW per cm² power density in a sealed and air-cooled, compact package – with the controller included. This Master Oscillator Fiber Amplifier (MOFA) architecture notably offers full control over the pulse energy (or peak power) while leaving unchanged the pulse width and pulse shape . An Acousto Optic Modulator (AOM) option is also available to offer a rapid control of the repetition rate without distortion of the pulse and high energy stability from the first pulse on. While the HNP-70F amplified laser produces 550 ps pulses of 1064 nm light at 70 kHz with an average power reaching 5 W, the HNG-70F amplified laser produces sub-500 ps pulses of 532 nm light at 70 kHz with an average power reaching 4 W. The lasers operate with a single emission frequency. Key Features: Wavelengths: 532, 1064 nm Ultra-short Pulses, Pulse Width Down to 500 ps (<0.65 ns) High Repetition Rate >70 kHz (Can Be Factory-set to up to 100 kHz With Lower Energy per Pulse) AOM Option @532 nm Peak Power >200 kW at 1064 nm (>100 kW at 532 nm) Excellent Beam Quality: Beam Profile Gaussian TEM00, M²<1.2 Efficient, Air-cooled Sealed Package, Long Life Output Energy: >45 µJ, >72 µJ Applications: Micromachining; Selective Ablation of µm to nm Scale Layers; Edge Isolation; Cutting from PCB to PCD With No Heat Effect; Instrumentation; Laser-induced Breakdown Spectroscopy (LIBS); Raman Spectroscopy; Supercontinuum Generation; Ranging; Differential Absorption LIDAR; Biophotonics; Dense Tissue Ablation; Microsurgery

532, 1064, 1535 nm; Output Energy >3, >6, >8 µJ; Repetition Rate >2, >5 kHz; Output Power >12, >15, >40 mW; Peak Power >1.5, >4, >8 kW Teem Photonics’ MNx Series of ultra-compact microchip DPSS lasers covers the mid infrared (IR) to visible (VIS) part of the spectrum. The lasers integrate the pump diode, the micro cavity and even the second harmonic generation crystal in a package less than 7 cm long. The MNG-03E-100 is a 532 nm microchip laser which produces sub-nanosecond pulses and achieves a very good harmonic conversion efficiency with pulses displaying several kW peak power in a 750 ps pulse duration. It is housed in a 6.8 cm long package. The MNP-08E-100 is an economical, compact, and reliable 1064 nm microchip laser producing sub-nanosecond pulses with several kW peak power. The MNE-06E-100 is an eye safe 1535 nm laser which integrates the pump diode and the micro-cavity in a 10 cm long package. It produces more than 1 kW of peak power in a few nanoseconds pulse duration. The MNx Series ultra-compact microchip DPSS lasers are easy to operate and service. Controllers can be used with every laser head model and swapped within minutes while keeping constant operating parameters. Key Features: Ultra-compact Package: 68x41x29, 100x22x32 mm (Laser Head) Wavelengths: 532, 1064, 1535 nm Ultra-short Pulses: <0.75, <1, <3.5 ns Multi-kW Peak Power: >1.5, >4, >8 kW Excellent Beam Quality: Beam Profile Gaussian TEM00, M²<1.1 Efficient, Air-cooled Output Energy: >3, >6, >8 µJ Repetition Rate: >2, >5 kHz Average Output Power >12, >15, >40 mW Linewidth: 1 pm (MNE-06E-100) Applications: Supercontinuum Generation; Marking; Raman Spectrometry; Ranging; Biophotonics, Instrumentation; Micromachining

Pulse duration <100 fs – 70 ps; Output power levels 15 W – 100W; Pulse Energy ≤ 250 µJ – 500 µJ; Repetition rates single shot to 80 MHz; Beam quality TEM0,0 / M2 < 1.3 The neoMOS ultrashort pulse laser series combines the reliability and low maintenance of state of the art fiber oscillators with a solid-state amplifier. The ultra-compact laser head has the smallest footprint currently available and enable easy system integration. High stability and long lifetime are provided by design for 24/7 industrial use. The multi-megawatt level peak-power and ultrafast pulses delivered by the neoMOS series are suitable for processing the most demanding materials including transparent glasses and plastics. Typical applications include photovoltaic and electronics production, display glass processing as well as security and decorative marking. The neoMOS laser is available with 10 ps and 70 ps pulse duration as well as the neoMOS SMAART, which combines pico- and femtosecond laser pulses within one compact laser system. The system is based on high reliable and low maintenance fiber oscillators and robust solid-state amplifiers. The new developed laser system further expands the neoMOS pulse duration range into the area of less than 900 fs up to a few ten picoseconds or even nanoseconds. With the short-pulse option the neoMOS SMAART can offer pulse duration down to 100 fs. Key features neoMOS 10ps Pulse durations <10 ps Output power levels ≤ 50 W Pulse energy ≤ 250 µJ Repetition rates single shot to 40 MHz Beam quality: TEM0,0 / M < 1.3 Key features neoMOS 70ps Pulse durations 70 ps Output power levels 15 W Pulse energy ≤ 250 µJ Repetition rates single shot to 80 MHz FlexPulse Technologie Beam quality: TEM0,0 / M2 < 1.3 Key features neoMOS SMAART Pulse durations 40 ps / 900 fs Output power levels 100 / 75 W Pulse energy ≤ 500 / 400 µJ Repetition rate 200 kHz – 2 MHz TEM0,0 Beam quality, M2 < 1.3 Key features neoMOS SMAART with Short Pulse Option Pulse durations <100 fs Output power > 50 W Pulse energy > 150 µJ Applications: Photovoltaic and electronics production, display glass processing, security and decorative marking

213, 266, 355, 532, 1064 nm; Output Energy >2->80 µJ; Repetition Rate 400-5000 Hz; Peak Power >2->160 kW; Pulse Width <350-<1000 ps Teem Photonics’ PNx Series of high peak power (up to 160 kW), passively Q-switched PowerChip™ DPSS lasers offers the highest peak powers and shortest pulses at kilohertz repetition rates with an excellent beam quality. PNx Series lasers feature a completely integrated platform which includes the laser head, power supply and air cooling in a compact, rugged, and turnkey package. Available wavelengths are 1064 nm, 532 nm, 355 nm, 266 nm – and the newest laser in the PNx Series transmits light at 213 nm through an advanced fifth harmonic conversion of the 1064 nm stage. Standard repetition rates are 400 Hz to 1 kHz, while the latest additions to the PNx Series feature a pulse frequency of 5 kHz with a pulse duration kept under 350 to 600 ps for output wavelengths of 355, 532 and 1064 nm. Key Features: Peak Power: up to 200 kW (>2 to >160 kW) Pulse Width: Down to 350 ps (<350 to <1000 ps) Wavelengths: 213, 266, 355, 532, 1064 nm Repetition Rate: Single Shot to 5000 Hz (400 to 5000 Hz) Excellent Beam Quality: Beam Profile Gaussian TEM00, M²<1.3 All-in-one Package Output Energy: >2 to >80 µJ Applications: Materials Processing; Inscribing Glass; PCB Via Drilling; Micromachining; MALDI-TOF; Micro-dissection; Laser-induced Fluorescence (LIF); Time Resolved Fluorescence; Laser-induced Breakdown Spectroscopy (LIBS); Light Detection and Ranging (LIDAR)

266, 355, 532, 1064 nm; Output Energy >0.2->18µJ; Repetition Rate >5->130 kHz; Output Power >2->300 mW; Peak Power >0.35->13 kW For generating high peak power UV, green or IR pulses of a few hundred picoseconds, Teem Photonics’ SNx Series of high-performance sealed microchip lasers are economical, compact, and reliable. SNx Series lasers are designed for high average power, delivering multi kW peak power at repetition rates up to 130 kHz. The SNP models’ sub-nanosecond 1064 nm pulses are directly generated from the diode-pumped, passively Q-switched Nd:YAG microchip engine with high average power, either from pulse energies of 20 µJ at 1064nm, or from repetition rates up to 130 kHz. The SNG models’ 532nm pulses as well as the SNV and SNU models’ micro joule UV pulses are produced by harmonic conversion from the passively Q -switched Nd:YAG engine IR system. The SNx Series high-performance sealed microchip DPSS lasers are easy to operate and service. Controllers can be used with every laser head model and swapped within minutes while conserving constant performances. Key Features: Repetition Rate: >5 to ≤130 kHz Wavelengths: 266, 355, 532, 1064 nm Ultra-short Pulses: <0.55 to >3ns Multi-kW Peak Power: >0.35 to >13 kW Excellent Beam Quality: Beam Profile Gaussian TEM00, M²<1.2 to <1.4 Efficient, Air-cooled Sealed Package, Extremely Long Life Output Energy: >0.2 to >18 µJ Average Output Power >2 to >300 mW Applications: Material Processing; Cost-effective Marking Solutions; Graphitization; Instrumentation; Ranging; Differential Absorption LIDAR; Supercontinuum Generation; Distributed Temperature Sensing; Raman Spectroscopy; Biophotonics; Nanosurgery; Protein Cross-linking; Semiconductor Inspection; PCB Repair; Laser-induced Fluorescence (LIF); Micro Dissection; Organic Compound Marking and Micromachining; Biohazard Detection; Time Resolved Fluorescence; Laser-induced Breakdown Spectroscopy (LIBS); Photoacoustic Microscopy; Photoacoustic Imaging

Actively Q-switched DPSS laser; pulse width <2 ns; repetition rate up to 50 kHz; very low jitter; 1064 nm and harmonics down to 355 nm Utilising advanced technology, SPOT actively Q-switched DPSS lasers provide a short pulse output (pulse widths <2 ns) at repetition rates from single shot up to >50 kHz with very low jitter. The series features fundamental YAG wavelength at 1064 nm and harmonics down to 355 nm. The compact design enables the lasers to be easily integrated into scientific instrumentation. Applications include laser induced fluorescence, time resolved fluorescence, micromachining, biotechnology, plasma generation, remote sensing, photo acoustic imaging, MALDI mass spectrometry and MALDI imaging. SPOT laser systems consist of a laser head with a separate power supply unit. Both units are connected with a cable which is hard wired into the laser head while having a 37 way ‘D’ connector for connection to the power supply unit. The SPOT DPSS laser series feature simple, user-friendly control with the minimum of user defined parameters. The systems are designed as fixed power level devices under automatic operation, or power can be varied by adjusting the pump diode current via RS232 interface. Specifications Wavelength: 1064 nm; 532 nm; 355 nm Pulse Energy: up to 50 µJ Pulse width: <2 ns Low jitter: <±1 ns Repetition rate: up to 50 kHz Spatial Mode: TEM00 M2 < 1.2 Features Low pulse width and jitter RS232 controllable User interface (interlock, on/off keyswitch etc.) Manual safety shutter Active current limit Auto power-up sequence: warmup, current mode Laser diode protection circuitry Monitoring the following parameters:      - Diode current limit, diode current setpoint, actual diode current      - Diode & chipset temperature setpoint, actual temperature Diode-on-time LCD hour counter (internal) Overtemperature Sensors for heatsink and laser-head Applications: Photoacoustic Microscopy; MALDI Mass Spectrometry (Matrix Assisted Laser Desorption Ionisation); Fluorescence Lifetime Imaging (FLIM); Dye Laser Pumping

Four wavelengths: 532 nm, 555 nm, 579 nm, 606 nm; pulse-by-pulse switchable with 2 kHz; Pulse Energy 20 µJ; Pulse Length <5 ns The diode-pumped solid-state laser TETRA emits very short laser pulses (< 5 ns) of high energy (up to 20 µJ) with four wavelengths in the visible range, which are particularly suitable for multispectral photoacoustic imaging. Using sophisticated technology, the TETRA laser can switch from pulse to pulse between these four wavelengths with a very high pulse repetition frequency of 2 kHz. Utilizing the Raman effect and the light of a 532 nm pump laser, the TETRA laser additionally generates the wavelengths 555 nm, 579 nm and 606 nm. A tunable optical filter separates the four wavelengths and routes one wavelength at a time to the optical output of the unit at a switching frequency of up to 2 kHz. This makes TETRA about ten times faster than tunable lasers based on OPOs (Optical Parametric Oscillators) – typical frequencies of such OPO systems range from 100 Hz to 200 Hz – while also being considerably more cost-effective. The wavelengths emitted by TETRA are well matched to the absorption curves of many blood components, making the laser particularly suitable for photoacoustic tomography in biomedicine. We have equipped TETRA with a number of features to meet the requirements of medical safety standards for use in clinical environments. For instance a fast, fault-tolerant shutter at the laser output interrupts the beam in the event of a fault in the shortest possible time in order to avoid any hazards to a patient.