WhatsApp: +65 91904616 E-mail: sales@sintec.sg
EO Q-switched lasers with 1064nm/532nm/355nm/266nm energy up to 10J at 10Hz 1064nm repetition rate up to 30Hz. They have high reliability and stability.
The lamp pumped Q-switched laser is a high energy laser with high stability, high conversion efficiency and high quality laser beam. With compact structure, easy installation and convenience to move, there are many options such as double pulse or more impulsive intervals and pulse output range. The system is equipped with adjustable control box and computer interface hand size limit, suitable for space and requirements and other equipment outside applications.
Features:
Super gauss beam output
Maximum output power can reach 100 joules
Industrial design, good reliability and no adjustment
Manual control box control, also can use computer operation
Typical Applications:
Laser rangefinder
Laser radar
Laser remote sensing
Strong Field of physics
Pump OPO lasers, fast, dye laser pump, Raman lasers
Laser fluorescence inspire
Plasma measurement
Optoelectronic detection
Optoelectronic countermeasures
Specifications:
Model | STHE-1000 | STHE-2000 | STHE-5000 | STHE-10000 | STHE-20000 | STHE-50000 | STHE-100000 | |
Pulse Width (FWHM) | -A:<10ns, -B:<2ns; -C:<200ps | |||||||
(-S) for single pulse design; (-D) for double pulse design; (-T) for multi pulse design | ||||||||
Energy (m J) on different Wavelength | 1064nm | 1000 | 2000 | 5000 | 10,000 | 20,000 | 50,000 | 100,000 |
532nm | 500 | 1000 | 2500 | 5000 | Option | Option | Option | |
355nm | 200 | 400 | Option | Option | Option | Option | Option | |
266nm | 80 | 150 | Option | Option | Option | Option | Option | |
213nm | 15 | 30 | Option | Option | Option | Option | Option | |
Beam Mode | -M (TEM00); -V(VRM) | |||||||
Repeat Frequency | 1-10Hz | 1-5 Hz | ||||||
Work method | Pulsed | |||||||
Power instability rate | Excel than 3% | |||||||
Pump method | Lamp pumped | |||||||
Beam Diameter | <10mm | <16mm | <20mm | <25mm | <25mm | <25mm | ||
Divergence | <0.5mrad | <0.3mrad | ||||||
Cooling method | pure water cooling (-W) ( or anti-freezing liquid cooling –A) | |||||||
Current | AC220V±20V/10A/50Hz±1 | |||||||
Voltage | 1 phase | 3 phases | ||||||
Marking head Size (mm) | 450×100×120 (L×W×H) | 650×200×120 (L×W×H) | 800×300×120 (L×W×H) | 800×300×220 (L×W×H) | 800×500×320 (L×W×H) | 900×500×420 (L×W×H) | 1200×600×420 (L×W×H) |
Part number | STHE-532-400 |
Laser Wavelength | 532nm |
Pulse Energy | ≥400 mJ |
Initial Beam Diameter | 8 mm |
Pulse width | ≤8ns |
PRF (Variable up to 10 Hz) | 1-10 Hz |
Single pulse operation | Yes |
Divergence @ 532 nm | ≤0.5 mrad |
Line width | ≤2 cm-1 |
PC interface | USB/RS232/Ethernet |
Power Requirement | 220V, 50 Hz AC |
Weight with second harmonic | 9.6 Kg |
Integrated Cooling unit with power supply | < 30 Kg |
Our compact lamp-pumped EO Q-switched nano-second laser is a low-medium energy pulsed solid-state laser. It has the features of small size, easy operation, stability. It also has a good reliability due to modular design. Thus these lasers are widely used in LIBS measurement, OPO pumping, laser cleaning etc.
Features:
Compact in size for easy integration
Sealing in water and air
All-in-one design
Red pilot available upon request
TEM00/VRM beam mode output
Controllable via mobile phone or computer
Typical Applications:
LIBS measurement
Laser radar
Laser cleaning
Pump OPO lasers, fast, dye laser pump, Raman lasers
Plasma measurement
Laser communications
Specifications:
Part number: STHE-P-200
Laser wavelength: 1064nm
Pulse energy: >=200mJ@1064nm
Energy stability: <=2%
Pulse repetition rate: 1Hz
Pulse width: <=15ns
Beam diameter: 6mm~10mm
Beam divergence: £1mrad
Pumping: flashlamp pumping
Warm up time: <10min
Store temp: -15-45℃
Environment humility: 20%-70%
Power input: 230VAC, 50Hz, single phase
Laser head dimension: 375x115x89 mm (LxWxH)
Laser head weight: 7.2kg
Power supply weight: 42kg
This series product is compact with a special EO Q-switch. They can provide high efficiency and stable signal pulse energy at 1064nm and the pulse width can be adjusted from 0.5μs to2.0μs.
Features:
Very compact and stable design;
Easy flash lamps replacement;
Energy can be adjusted from 15mJ to 400 mJ
Highly flexible design with repetition rate from 1Hz, 5Hz, 10Hz & 20Hz;
Can provide multiple triggering capabilities, such as internal trigger, external TTL trigger. Control lamps and Q-switch for precise laser pulse timing control.
Convenient operation. Controlled by single power supply and equipped with closed- loop water cooling system;
Thermally compensated resonator assures stable operation.
Typical Applications:
Burning blaze detected;
Laser Medical
Repetition Rate | 1, 5, 10, 20Hz |
Energy | >100mJ @ 1064nm, max. 800mJ |
Energy Stability | ±< 5% |
Pulse Width | 0.5 - 2.0μs |
Power Supply | 220V 50Hz AC |
Cooling System | closed- loop water cooling system |
Remarks: We also supply the customized lasers, such as four laser beams or more beams products.
Ordering Information: STLT-xxxx-yyy-zzz, where xxxx means wavelength in nm, yyy means pulse energy in nJ and zzz means pulse repetition rate in Hz.
These lasers have dual or multiple laser-heads with compact size. They can provide high efficiency and stable green light source for Particle Image Velocimetry (PIV) applications. It is suitable for most liquid experiments and many air-based 2D/3D PIV ones.
Features:
Very compact and stable design;
Easy flash lamps replacement;
Energy can be adjusted from 15mJ to 400 mJ
Highly flexible design with repetition rate from 1Hz to 15Hz or 1Hz to 30Hz;
Can provide multiple triggering capabilities, such as internal trigger, external TTL trigger. Control lamps and Q-switch for precise laser pulse timing control.
Convenient operation, Control by single power supply and equipped with closed- loop cooling system;
Thermally compensated resonator assures stable operation;
Typical Applications:
Suitable for liquid experiments;
Air-based 2D/3D PIV;
Wind tunnel research;
Water tunnel research;
Micro-fluidic measurement;
Spray or flame research
Thermally compensated resonator assures stable operation;
Specifications:
Model | STLT-600 | STLT-610 | STLT-620 | STLT-630 | STLT-640 | STLT-650 | STLT-660 | STLT-670 |
Repetition Rate (Hz) | 15 | 30 | 15 | 15 | 15 | 10 | 100 | 200 |
Pulse Energy(mJ) 532nm | 30 | 30 | 80 | 120 | 200 | 360 | 100 | 50 |
Energy Stability (RMS)(%)532nm | 3 | 3 | 4 | 4 | 4 | 4 | 4 | 4 |
Wavelength | 532 | 532 | 532 | 532 | 532 | 532 | 532 | 532 |
Beam Size | ≤4 | ≤4 | ≤7 | ≤7 | ≤8 | ≤10 | ≤7 | ≤7 |
Pulse width (ms) | ≤10 | ≤10 | ≤10 | ≤10 | ≤10 | ≤10 | ≤10 | ≤10 |
Divergency (mrad) | ≤3 | ≤3 | ≤3 | ≤3 | ≤3 | ≤2 | ≤4 | ≤4 |
Spatial Profile | VRM Mode | VRM Mode | VRM Mode | VRM Mode | VRM Mode | VRM Mode | VRM Mode | VRM Mode |
Timing Jitter (ns) | ≤2 | ≤2 | ≤2 | ≤2 | ≤2 | ≤2 | ≤2 | ≤2 |
Remarks: We also supply the customized lasers, such as four laser beams or more beams products
Diode pumped with 1 billion shots lifetime
Air cooling without maintenance
EOQ switched with accurate timing
1064 nm with over 80 mJ energy output
Higher harmonics available
Portable design with compact size
Easy for system integration
STLA series DPSS lasers are with uniform pumping and conduction cooling technologies to realize real portable nanosecond laser source. This series provide the new solution to various scientific, industrial and military applications.
Diode pumping has the features such as low energy consumption, high efficiency and long lifetime. TEC conduction cooling technology is used to avoid any water usage while keeping the operation stability. Electro-optical Q-switched technology is used to provide accurate timing, which is key to analysis instrument.
Based on all these features, our lasers are the perfect choice for applications like LIDAR, mass spectroscopy, laser ultrasonic and LIBS.
Part number | STLB-LA-20-xxxx | STLB-LA-80-xxxx | |
Pulse repetition rate (Hz) | 1-100 | 20 | |
Pulse energy (mJ) | 1064nm | 20 | 80 |
532nm | 12 | 50 | |
355nm | 4 | 15 | |
266nm | 2 | 8 | |
Energy stability2 RMS | 1064nm | <1% | <0.5% |
532nm | <2% | <2% | |
355nm | <4% | <4% | |
266nm | <4% | <4% | |
Pulse width3 (ns) | 10 | 10 | |
Divergence4 (mrad) | 2 | 2 | |
Pointing stability (urad) | <50 | <50 | |
Beam dia.5 (mm) | 3 | 4 | |
Polarization | Horizontal | Horizontal | |
Jitter6 (RMS) (ns) | <1 | <1 | |
Cooling | Air | Air | |
Power input | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | |
Power consumption (W) | 800 | 800 | |
Operation temp. (oC) | 5-30 | 5-30 | |
Storage temp. (oC) | 5-50 | 5-50 | |
Dimension7 (mm) | Head | 413x160x128 | 413x160x128 |
Power | 380x323x89 | 380x323x89 |
All the specifications unless otherwise stated are for Q-switched 1064nm operation. The xxxx in the part numbers is laser wavelength.
Dev to average (shot to shot for 99% of pulses)
Full width half max. (FWHM)
Full angle at 1/e2 of the peak
With respect to external trigger
Measured at the laser output
All the dimensions are the lasers with 4th harmonic generation (266nm).
Fundamental wavelength covers 10-300 mJ output
Higher harmonics available
Module design and easy to use
Industrial design to ensure long term operation
Humanization design and easy for integration
Customization version available
STLB-DA series lasers are designed for an industrial level laser that greatly fits OEM system integration. The energy level is relatively low, from 10-300 mJ. The SHG, THG and FHG are available.
The lasers provides both multimode and variable reflectivity mirror (VRM) mode beam with good beam quality. The scientific and industrial design ensures the good beam quality. Features as optical shutter, flow sensor, power supply interlock make sure the safety use as the top priority. The lasers passed CE certification in 2014.
The lasers are suitable for many applications, including LIBS, LIDAR, LIF, PIV, laser ultrasonic, laser spark plug, laser cleaning, LCD repair etc.
Part number | STLB-DA-50-xxxx | STLB-DA-100-xxxx | STLB-DA-200-xxxx | STLB-DA-300-xxxx | |
Pulse repetition rate (Hz) | 1-20 | 1-20 | 1-20 | 1-10 | |
Pulse energy (mJ) | 1064nm | 50 | 100 | 200 | 300 |
532nm | 25 | 50 | 100 | 150 | |
355nm | 10 | 20 | 40 | 60 | |
266nm | 5 | 10 | 20 | 30 | |
Energy stability2 RMS | 1064nm | <1% | <1% | <1% | <1% |
532nm | <2% | <2% | <2% | <2% | |
355nm | <4% | <4% | <4% | <4% | |
266nm | <4% | <4% | <4% | <4% | |
Pulse width3 (ns) | 1064nm | <9 | <9 | <8 | <7 |
532nm | <8 | <8 | <7 | <6 | |
355nm | <7 | <7 | <6 | <5 | |
266nm | <7 | <7 | 6 | <5 | |
Divergence4 (mrad) | 1064nm | Multi-mode, <3mrad; Flat-top, <1rmad | Multi-mode, <3mrad; Flat-top, <1rmad | Multi-mode, <3mrad; Flat-top, <1rmad | Multi-mode, <3mrad; Flat-top, <1rmad |
Pointing stability (urad) | <50 | <50 | <50 | <50 | |
Jitter5 (RMS) (ns) | <1 | <1 | <1 | <1 | |
Beam dia.6 (mm) | 1064nm | 5 | 5 | 6 | 7 |
Spatial mode profile | Near field | >70% | >70% | >70% | >70% |
Far field | >95% | >95% | >95% | >95% | |
Cooling | Air to water | Air to water | Air to water | Air to water | |
Power input | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | |
Power consumption (W) | 500 | 500 | 500 | 500 | |
Cable length (m) | Control | 3 | 3 | 3 | 3 |
Power | 1.8 | 1.8 | 1.8 | 1.8 | |
Umbilical | 3 | 3 | 3 | 3 | |
Operation temp. (oC) | 5-30 | 5-30 | 5-30 | 5-30 | |
Storage temp. (oC) | 5-50 | 5-50 | 5-50 | 5-50 | |
Dimension7 (mm) | Head | 579x193x95 | 579x193x95 | 579x193x95 | 579x193x95 |
Power | 473x216x563 | 473x216x563 | 473x216x563 | 473x216x563 |
All the specifications unless otherwise stated are for Q-switched 1064nm operation. The xxxx in the part numbers is laser wavelength.
Dev to average (shot to shot for 99% of pulses)
Full width half max. (FWHM)
Full angle at 1/e2 of the peak
With respect to external trigger
Measured at the laser output
All the dimensions are the lasers with 3th harmonic generation (355nm).
Compact size
High uniformity of beam profile
Industrial design to ensure long term operation
High SHG and UV efficiency
Built to withstand various environment
Easy for system integration
STNI series lasers are middle energy level Q-switched nanosecond Nd:YAG laser. The fundamental wavelength covers energy level from 400 mJ to 2000 mJ. These lasers possess the features of compact size, good pointing stability, high energy stability, high reliability, etc. The SHG, THG and FHG are available.
These lasers provide two types of laser mode, multimode and VRM mode. The scientific and industrial design ensures the good beam quality. Features as optical shutter, flow sensor, power supply interlock make sure the safety use as the top priority.
Up to now, around 4000 units have been delivered all over the world. They are the perfect choice for various kinds of scientific and industrial applications such as pump dye laser, pump OPO, pump Ti:Sapphire laser, laser shock peening, LCD repair, laser ablation, laser sintering, LIDAR.
Part number | STLB-NI-400-xxxx | STLB-NI-600-xxxx | STLB-NI-900-xxxx | STLB-NI-Extra-xxxx | |
Pulse repetition rate (Hz) | 1-10 | 1-10 | 1-10 | 1-10 | |
Pulse energy (mJ) | 1064nm | 450 | 650 | 900 | 2000 |
532nm | 250 | 350 | 480 | 1000 | |
355nm | 90 | 150 | 270 | 600 | |
266nm | 50 | 65 | 90 | 150 | |
Energy stability2 RMS | 1064nm | <=1% | <=1% | <=1% | <=1% |
532nm | <=2% | £2% | <=2% | <=2% | |
355nm | <=4% | <=4% | <=4% | <=4% | |
266nm | <=4% | <=4% | <=4% | <=4% | |
Pulse width3 (ns) | 1064nm | <=9 | <=9 | <=9 | <=9 |
532nm | <=8 | <=8 | <=8 | <=8 | |
355nm | <=7 | <=7 | <=7 | <=7 | |
266nm | <=7 | <=7 | <=7 | <=7 | |
Divergence4 (mrad) | 1064nm | <=0.6 | <=0.6 | <=0.6 | <=0.5 |
Pointing stability (urad) | <=30 | <=30 | <=30 | <=50 | |
Jitter5 (RMS) (ns) | <=1 | <=1 | <=1 | <=1 | |
Beam dia.6 (mm) | 1064nm | 8 | 8 | 9 | 11 |
Spatial mode profile | Near field | >70% | >70% | >70% | >70% |
Far field | >95% | >95% | >95% | >95% | |
Polarization | Horizontal | 1064/355/266nm | 1064/355/266nm | 1064/355/266nm | 1064/355/266nm |
Vertical | 532nm | 532nm | 532nm | 532nm | |
Cooling | Air to water | Air to water | Air to water | Chiller | |
Power input | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | 220VAC/50-60Hz, 10A | |
Power consumption (kW) | 2 | 2 | 2 | 3 | |
Cable length (m) | Control | 3 | 3 | 3 | 3 |
Power | 1.8 | 1.8 | 1.8 | 1.8 | |
Umbilical | 3 | 3 | 3 | 3 | |
Operation temp. (oC) | 5-30 | 5-30 | 5-30 | 5-30 | |
Storage temp. (oC) | 5-50 | 5-50 | 5-50 | 5-50 | |
Dimension7 (mm) | Head | 810.5x150x142 | 810.5x150x142 | 810.5x150x142 | 820x290x136 |
Power | 568x296x590 | 568x296x590 | 568x296x590 | 568x296x590 |
All the specifications unless otherwise stated are for Q-switched 1064nm operation. The xxxx in the part numbers is laser wavelength. For example, STNI-400-532 is 532nm laser and it includes 1064nm and 532nm modules.
Dev to average (shot to shot for 99% of pulses)
Full width half max. (FWHM)
Full angle at 1/e2 of the peak
With respect to external trigger
Measured at the laser output
All the dimensions are the lasers with 4th harmonic generation (266nm).
STLB-SGR Series Super-Gaussian Resonator series Q-Switched Nd:YAG lasers combine VRM (variable reflectivity mirror) with unstable resonator design creating a cavity with large TEM00 mode volume for excitation and energy extraction. A “flat-top-hat” can be specified with uniform energy distribution or “VRM Gaussian” profiles.
STLB-GR Series close-coupled diffuse pump chamber delivers uniform pumping of the laser rod for optimum lasing excitation efficiency and allows for higher stored energy by eliminating parasitic oscillations within the pump chamber. The pump chamber uses chemically inert materials to withstand high pumping energy and absorb unwanted UV and IR radiation emitted by the flash lamps. One or more amplifiers can be added to the oscillator for higher energy output. With scientific or industrial grade models available, the STGR series will fit right in with your scientific research, medical or OEM industrial application.
Features:
Fundamental wavelength covers 2-6 J output
Higher harmonics available
Repetition rate up to 50 Hz
Injection seeded for narrow linewidth
RS232 and TTL interface for remote or external control
Invar structure inside
Applications:
Photo chemistry
Molecular chemistry
Non-linear optics
Laser illumination
LIDAR
Laser cleaning
Laser ablation
Optical remote sensing
LIF (Laser Induces Florescence)
PLD (Pulsed Laser Deposition)
Plasma diagnostics
Technical Specifications
Part no. | STLB-SGR-10 | STLB-SGR-20 | STLB-SGR-30 | STLB-SGR-40 | STLB-SGR-50 | STLB-SGR-60 | ||||||||
Rep. rate | 10 | 10 | 20 | 30 | 50 | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | |
Energy (mJ) | 1064nm | 1000 | 2000 | 2000 | 2000 | 1500 | 3000 | 3000 | 4000 | 4000 | 5000 | 5000 | 6000 | 6000 |
532nm | 500 | 1000 | 1000 | 1000 | 750 | 1500 | 1500 | 2000 | 2000 | 2500 | 2500 | 3000 | 3000 | |
355nm | 250 | 500 | 400 | 400 | 300 | 750 | 750 | 1000 | 1000 | 1250 | 1250 | 1500 | 1500 | |
266nm | 90 | 180 | 100 | 90 | 50 | 250 | 200 | 300 | 300 | 400 | 350 | 500 | 400 | |
Power stability2 RMS | 1064nm | <1% | ||||||||||||
532nm | <2% | |||||||||||||
355nm | <4% | |||||||||||||
266nm | <4% | |||||||||||||
Power drfit3 | 1064nm | <3% | ||||||||||||
532nm | <5% | |||||||||||||
355nm | <6% | |||||||||||||
266nm | <8% | |||||||||||||
Pulse width4 | 1064nm: 8-10ns; other wavelength: 7-10ns | |||||||||||||
Spatial profile5 | Near field | >70% | ||||||||||||
Far field | >90% | |||||||||||||
Beam dia.6 (mm) | 10 | 12 | 12 | 12 | 12 | 15 | 15 | 15 | 15 | 17 | 17 | 20 | 20 | |
Divergence7 | <0.5mrad | |||||||||||||
Pointing stability | <50urad | |||||||||||||
Jitter8 (RMS) | <1ns | |||||||||||||
Linewidth | Standard | <1cm-1 | ||||||||||||
Injection seeded | <0.0031cm-1 |
Part no. | STLB-SGR-S400 | STLB-SGR-S500 | STLB-SGR-S600 | STLB-SGR-S600 | |
Rep. rate (Hz) | 10 | 20/30/50 | 20/30 | 10 | |
Energy (mJ) | 1064nm | 400 | 500 | 600 | 800 |
532nm | 200 | 250 | 300 | 400 | |
355nm | 100 | 100 | 150 | 200 | |
266nm | 40 | 40 | 50 | 80 | |
Divergence7 | <0.7mrad | <0.5mrad | <0.5mrad | <0.5mrad | |
Beam dia.8 | 8mm | 8mm | 8mm | 8mm | |
Other specifications | Please refer to the table above | Please refer to the table above | Please refer to the table above | Please refer to the table above |
All specifications unless otherwise stated are for 1064nm operation.
Dev. To average (shot to shot for 99% of pulses).
Average for 8 hours with room temp. variation less than +/-3 deg.
Full width half max (FWHM)
Near field profiles measured at the focal plane, least square fit to Gaussian profile.
Measured at the laser output.
Full angle at 1/e2 of the peak.
With respect to external trigger.
Other Specifications
STLB-SGR-S | STLB-SGR-10 | STLB-SGR-20/30/40 | STLB-SGR-60 | ||
Size (LxWxH) (mm) | Laser head | 1162x333x290.5 | 1162x410x290.5 | 1162x410x290.5 | 1266x565x243 |
Power supply | 476x443x200 | 914x520x737 | 914x520x737 | 914x520x737 | |
Cooling system | N/A | N/A | 240x170x70 | 836x688x1125 | |
Power input | 220V-50Hz-16A | 220V-50Hz-16A | 220V-50Hz-16A | 380V-50Hz-25A | |
Operation temp. | 5-30oC | 5-30oC | 5-30oC | 5-30oC | |
Cables | Control line | 3m | 3m | 3m | 3m |
Power line | 1.8m | 1.8m | 1.8m | 1.8m | |
Umbilical line | 3m | 3m | 3m | 3m |
STLB-SGRE series lasers have been developed since 2007 as high energy nanosecond laser systems which are suitable for laser peening, pump source, plasma physics, etc. STLB-SGRE series lasers provide the customization service. Specifications such as wavelength, repetition rate, energy, pulse width, beam profile, SLM are all available for customization. We also developed and gained much experience on burst mode technique and vehicular applications during this process. As a result, we can provide the ideal laser source solution for the customer in various applications.
Main Features:
High output energy up to 50J@1064 nm
8-26ns pulse width, high peak power
Unique cavity design to ensure uniform beam profile
Good stability for long term operation
Local and remote control interface with compatibility
Customization version available
Applications:
Laser peening
Pump Ti:Sapphire laser
Plasma diagnostics
Nonlinear optics
LIDAR
Laser cleaning
Model1 | STLB-SGRE-04 | STLB-SGRE-06 | STLB-SGRE-08 | STLB-SGRE-10 | STLB-SGRE-12 | STLB-SGRE-15 | STLB-SGRE-20 | STLB-SGRE-25 | STLB-SGRE-30 | STLB-SGRE-40 | STLB-SGRE-50 |
Wavelength2 | 1064nm | ||||||||||
Rep rate, Hz | 20/30/50 | 5/10 | 5/10 | 5/10 | 5 | 5 | 2 | 2 | 5 | 2 | 2 |
Pulse energy at 1064nm | 3-4J | 6J | 8J | 10J | 12J | 15J | 20J | 25J | 30J | 40J | 50J |
Pulse width at 1064nm3 | 10-12ns, 15-20ns optional | 12-15ns, 15-20ns optional | |||||||||
Divergence4 | <=0.5mrad for VRM, <=4mrad for MM | ||||||||||
Peak to average | <=1.8:1 | ||||||||||
Polarisation | Linear 100:1 | Cross | |||||||||
Energy stability5 RMS | <1% | ||||||||||
Power drift RMS | <5% | ||||||||||
Pointing stability | <50urad | ||||||||||
Jitter6 RMS | <1ns | ||||||||||
Warm up time7 | <5min |
1. All specifications unless otherwise stated are for 1064nm operation.
2. SHG, THG, FGH are available upon request.
3. Full width half max (FWHM). The rising time can be cut down to <5-10ns by slice as option.
4. Full angle at 1/e2 of the peak.
5. Dev. To average (shot to shot for 99% of pulses).
6. With respect to external trigger.
7. Time to full energy.
Mechanical & Utilities
Size (LxWxH), mm | Customisation |
Electrical input | 380VAC 50Hz, 50A, 3-phase |
Water cooling | Distilled water, chiller |
Operation temperature | 10-30 degree |
Storage temperature | 0-40 degree |
Up to 90mJ @ 1064nm and built in harmonic generators 532nm, 355nm, 266nm
FEATURES:
No cooling water required
Compact & rigid design
Excellent beam profile
Continuous operation mode
Built-in harmonics
Turn-key operation
Remote control
The STLQ-115 is an ultra-compact model of air-cooled Nd:YAG laser for applications requiring compact and undemanding laser source.
Due to application of original high-efficiency heat exchanger the STLQ-115 laser unlike most air-cooled laser models can work continuously with PRR up to 3Hz and cyclically with PRR up to 5Hz. The above operating modes are realised at output energies conventionally attained at water-cooled lasers.
The STLQ-115 laser provides up to 90mJ output pulse energy at the fundamental with possibility of further conversion of IR radiation into the second harmonic as well as into the third or fourth harmonic.
All the harmonic generators are built-in and temperature stabilised. This peculiarity together with optimised rigid laser head design ensures output radiation long-term stability comparable to that of standard laboratory lasers.
Unlike most compact lasers using DKDP-based Pockels cells, the STLQ-115 incorporates LiNbO3 electro-optical Q-Switch. Such Q-Switch is not hygroscopic and retains its parameters within a wide temperature range and ensures reliable and stable laser operation.
Dust-proof laser head design allows to align main optical components without removing the cover that increases their life in the field.
To reduce your time expenses on routine service of the STLQ-115 laser we use only long lifetime flash lamps by Heraeus Noblelight Ltd. Besides, the flash lamp replacement procedure is elementarily easy even for a unskilled user.
Absence of water cooling system gives to the STLQ-115 laser a number of essential operational advantages:
Footprint of both the laser head and power supply is considerably reduced.
Integration of the laser into different mobile systems is facilitated.
Technical reliability of the device operation is increased.
Operating costs are reduced.
STLQ-115STLQ-115
Model | (1064 nm) | (532 nm) | |||||
PRR, Hz | 1 | 2 | 3 | 1 | 2 | 3 | |
Output energy, mJ, not less than | 1064 nm | 90 | 90 | 75 | 90 | 90 | 75 |
532 nm | – | 45 | 40 | 30 | |||
355 nm | – | ||||||
266 nm | |||||||
Pulse-to-pulse energy stability, ±%1) | 3 | 3.5 | 4.5 | 3 | 3.5 | 4.5 |
STLQ-115STLQ-115
Model | (355 nm) | (266 nm) | |||||
Pulse repetition frequency, Hz | 1 | 2 | 3 | 1 | 2 | 3 | |
Output energy, mJ, not less than | 1064 nm | 90 | 90 | 75 | 90 | 90 | 75 |
532 nm | 35 | 30 | 22 | 45 | 40 | 30 | |
355 nm | 20 | 20 | 15 | - | - | - | |
266 nm | - | - | - | 6 | 5 | 4 | |
Pulse-to-pulse energy stability, ±%1) | 3 | 3.5 | 4.5 | 3 | 3.5 | 4.5 |
Model | For all the models | |
Pulse duration, ns1) | 5…9 | |
Beam diameter, mm1) | ≤ 4.5 | |
Divergence, mrad1) | ≤ 3 | |
Jitter, ns2) | ≤ 3.5 | |
Power consumption, W | ≤ 200 | |
Dimensions (LxWxH), mm | Laser head | 410 x 125 x 130 |
Power supply | 320 x 370 x 150 |
* Specifications are subject to change without notice.
1)At 1064 nm.
2)Relative to the Q-Switch driver external trigger pulse.
Up to 180mJ @ 1064nm and harmonic generators up to 213nm
FEATURES:
Excellent beam quality
Built-in harmonic generators up to 213 nm
Dust- and water-proof design
Reliability of industrial equipment
Compact single phase power supply
No need for external water
The STLQ-215 laser is built on the basis of a model produced for aerospace industry and combines excellent beam quality required for advanced scientific research with a highest reliability of industrial equipment.
Original and reliable optical scheme ensures compensation of both astigmatism and thermooptical distortions and places at your disposal laser radiation of the highest quality.
One more peculiarity of the laser optical scheme is that all the components operate at loads considerably lower than the admissible values. Such a smooth operation mode not only increases life time of the components but also ensures unique operational reliability of the whole laser. As a result, you can use the STLQ-215 laser for your experiments day-to-day and year-to-year having forgotten about repairs and other unpleasant operation costs.
All the laser optical components are installed on a rigid base fixed to the housing with specially developed dampers. Due to this, mechanical vibrations and housing stress no way influence the quality of the cavity alignment.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term output radiation stability. The efficient thermostats used in the STLQ-215 ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ-215 we provided flash lamp life time of more than 50 million pulses and foreseen easy and quick procedure of its replacement.
It should be noted that the laser design allows to replace the flash lamp without removing the laser head upper cover. Such a technical solution considerably reduces risks of the optical components contamination as well as increases operational reliability of the device.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
If you plan to use the STLQ-215 in laboratory experiments, as a bonus you will get unsurpassed operational reliability and minimization of accompanying expenses.
If you are attracted by the reliability of the STLQ-215 laser and you will use it for industrial or field applications, in addition to a highest reliability you get beam quality conventionally available only for high-precision laboratory equipment.
The STLQ-215 is an ideal instrument for such applications as:
Ti:Sapphire Lasers and OPO Pumping
Dye Lasers Pumping
Spectroscopy
LIDAR
LIF (Laser Induced Fluorescence)
LIBS (Laser Induced Breakdown Spectroscopy)
Education
PIV (Particle Image Velocimetry)
Range-Finding
Ablation
Marking
TFT-LCD Repair
Flat Panel Display (FPD) Manufacturing
STLQ-215STLQ-215STLQ-215STLQ-215STLQ-215
Model | (1064 nm) | (532 nm) | (355 nm) | (266 nm) | (213 nm) | ||||||
PRR, Hz | 10 | 20 | 10 | 20 | 10 | 20 | 10 | 20 | 10 | 20 | |
Output energy, mJ, not less than | 1064 nm | 180 | 180 | 180 | 180 | 180 | |||||
532 nm | - | 100 | 80 | 100 | 80 | ||||||
355 nm (HPV)1) | - | 60 | 60 | - | 60 | 60 | |||||
355 nm | 50 | 45 | - | 50 | 45 | ||||||
266 nm | - | 35 | - | ||||||||
213 nm (HPV)1),2) | - | 8 | 6 | ||||||||
213 nm2) | 6 | 5 |
Model | For all the Models | |
Pulse-to-pulse energy stability, ±%3) | < 2.5 | |
Pulse duration, ns3) | 6…10 | |
Beam diameter, mm3) | ≤ 5 | |
Divergence, mrad3) | ≤ 1.5 | |
Jitter, ns4) | ≤ 1.5 | |
Power consumption, W | ≤ 500 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 455 x 165 x 140 |
Power supply | 620 x 330 x 670 |
1)For the high-power version at 355 nm.
2)With the STLG-105 external fifth harmonic generator.
3)At 1064 nm.
4)Relative to the Q-Switch driver external trigger pulse.
Up to 100mJ @ 1064nm and 50mJ @ 532nm in each pulse
FEATURES
Excellent beam quality
1064 nm or 532 nm output wavelength
Beam pointing stability
Dust- and water-proof design
Reliability of industrial equipment
Compact single phase power supply
No need for external water
The STLQ-215-D is built on the basis of a laser produced for aerospace industry and combines excellent beam quality required for advanced scientific research and a highest reliability of industrial equipment.
The design of conventional lasers generating dual pulse is based either on combining two lasers or on successive generation of nanosecond pulses by one active element during one flash lamp discharge pulse. The first solution allows to build a system with the maximum capabilities for the user but leads to increase of its cost and dimensions. The second approach allows to create low-cost and compact systems but leads to reduction of each pulse energy and of laser beam profile worsening and stability as well as limits the delay range between the pulses.
The STLQ-215-D design demonstrates advantages of both the variants but eliminates their disadvantages: output radiation is generated by two separate cavities while both the Nd:YAG rods are installed in one pump chamber and are pumped by one flash lamp. Both the cavities are integrated into a common laser head controlled by a common power supply that provides to the user minimum dimensions and convenience in controlling dual pulse parameters.
Original and reliable optical scheme ensures compensation of both astigmatism and thermooptical distortions and places at your disposal laser radiation of the highest quality.
One more peculiarity of the laser optical scheme is that all the components operate at loads considerably lower than the admissible values. Such a smooth operation mode not only increases life time of the components but also ensures unique operational reliability of the whole laser. As a result, you can use the STLQ-215-D laser for your experiments day-to-day and year-to-year having forgotten about repairs and other unpleasant operation costs.
All the laser optical components are installed on a rigid base fixed to the housing with specially developed dampers. Due to this, mechanical vibrations and housing stress no way influence the quality of the cavity alignment.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term output radiation stability. The efficient thermostats used in the STLQ-215-D ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ-215-D we provided flash lamp life time of more than 50 million pulses and foreseen easy and quick procedure of its replacement.
It should be noted that the laser design allows to replace the flash lamp without removing the laser head upper cover. Such a design concept considerably reduces risks of the optical components contamination as well as increases operational reliability of the device.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
STLQ-215
Model | -D | |
Maximum PRR, Hz1) | 20 | |
Each pulse output energy, mJ, not less than2) | 1064 nm | 100 |
532nm | 50 | |
Pulse duration, ns2) | 6…10 | |
Adjustable delay between pulses, µs | 0…80 | |
Step of adjustable delay between pulses, µs | 1 (0.1 – upon request) | |
Beam diameter, mm3) | ≤ 5 | |
Divergence, mrad3) | ≤ 1.5 | |
Pulse-to-pulse energy stability, ±%3) | < 2.5 | |
Beam pointing stability, mrad, not worse than3) | 0.1 | |
Jitter, ns4) | < 1 | |
Power consumption, W | ≤ 500 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 534 x 190 x 135 |
Power supply | 620 x 330 x 670 |
* Specifications are subject to change without notice.
1)The laser operates at fixed PRR stipulated on placing an order. The PRR can be from 1Hz to 20Hz. All the parameters are specified for 20Hz PRR.
2)The difference between pulse energies in the dual pulse does not exceed ± 5%.
3)At 1064 nm.
4)Relative to the Q-Switch driver external trigger pulse.
Up to 500mJ at 1064nm and harmonic generators up to 213nm
FEATURES:
High PRR
High pulse energy up to 0.5 J
Excellent beam quality
All harmonics available up to 213 nm
Compact single-phase power supply
No external water requirements
The STLQ-529 is a series of popular compact lamp-pumped Nd:YAG lasers offering uncompromising combination of the main parameters: high output power, exceptional beam quality and minimum laser head and power supply dimensions.
All the lasers of the STLQ-529 series are based on ring cavity and incorporate a pump chamber with diffuse ceramic reflector. Due to this technical solution the STLQ-529 lasers, unlike the lasers with traditional linear cavity, provide homogeneous close to flat-top laser beam profile and possess exceptional stability of output energy and spatial radiation parameters. Beam pointing stability of the STLQ-529 is better than 20 µrad in the vertical plane and 80 µrad in the horizontal plane.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term output radiation stability. The efficient thermostats used in the STLQ-529 ensure warm-up time of less than 10 min.
To reduce your time expenses on routine service of the STLQ-529 we provided flash lamp life time of more than 30 million pulses and foreseen easy and quick procedure of its replacement.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
STLQ-529STLQ-529STLQ-529STLQ-529STLQ-529
Model | A (1064nm) | A (532 nm) | A (355 nm) | A (266 nm) | A (213 nm) | ||||||
PRR, Hz | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | |
Output energy, mJ, not less than | 1064 nm | 500 | 500 | 500 | 500 | 500 | |||||
532 nm | - | 280 | 225 | 280 | 225 | ||||||
355 nm (HPV)1) | - | 130 | 130 | - | 130 | 130 | |||||
355 nm | 110 | 100 | - | 110 | 100 | ||||||
266 nm | - | 85 | 70 | - | |||||||
213 nm (HPV)1),2) | - | 25 | 20 | ||||||||
213 nm2) | 20 | 15 | |||||||||
Beam diameter, mm3) | ≤ 8 | ||||||||||
Power consumption, W | ≤ 600 |
STLQ-529STLQ-529STLQ-529STLQ-529STLQ-529
Model | B (1064 nm) | B (532 nm) | B (355 nm) | B (266 nm) | B (213 nm) | ||||||
PRR, Hz | 10 | 20 | 10 | 20 | 10 | 20 | 10 | 20 | 10 | 20 | |
Output energy, mJ, not less than | 1064 nm | 350 | 350 | 350 | 350 | 350 | |||||
532 nm | - | 190 | 140 | 190 | 140 | ||||||
355 nm (HPV)1) | - | 100 | 100 | - | 100 | 100 | |||||
355 nm | 90 | 80 | - | 90 | 80 | ||||||
266 nm | - | 60 | 40 | - | |||||||
213 nm (HPV)1),2) | - | 18 | 15 | ||||||||
213 nm2) | 15 | 12 | |||||||||
Beam diameter, mm3) | ≤ 6 | ||||||||||
Power consumption, W | ≤ 800 |
STLQ-529STLQ-529STLQ-529STLQ-529STLQ-529
Model | C (1064 nm) | C (532 nm) | C (355 nm) | C (266 nm) | C (213 nm) | |
PRR, Hz | 50 | |||||
Output energy, mJ, not less than | 1064nm | 150 | 150 | 150 | 150 | 150 |
532nm | - | 80 | 65 | 80 | 65 | |
355nm | - | 40 | - | 40 | ||
266nm | - | 20 | - | |||
213nm2) | - | 4,5 | ||||
Beam diameter, mm3) | ≤ 5 | |||||
Power consumption, W | ≤ 1000 |
Model | For all the Models | |
Pulse-to-pulse energy stability, ±%2) | < 2,5 | |
Pulse duration, ns3) | 10…13 | |
Divergence, mrad3) | ≤ 1.5 | |
Jitter, ns4) | ≤ 1 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 615 x 180 x 120 |
Power supply | 620 x 330 x 670 |
* Specifications are subject to change without notice.
1)For the high-power version at 355 nm.
2)With the STLG-105 external fifth harmonic generator.
3)At 1064 nm.
4)Relative to the Q-Switch driver external trigger pulse.
Up to 200mJ @ 1064nm and harmonic generators up to 213nm
FEATURES:
High PRR
High pulse energy
Excellent beam quality
All harmonics available up to 213 nm
Compact single-phase power supply
No external water requirements
The combination of high laser pulse energy, high PRR and excellent beam quality unattainable for most conventional models is the peculiarity of the STLQ-629 laser.
Active elements of master oscillator and amplifier are installed in one pump chamber and are pumped by a single flash lamp. The master oscillator is based on the time-proven ring cavity design ensuring excellent beam quality while the classical single-pass amplifier is supplemented with the optics compensating thermooptical aberrations.
Particularly due to this technical solution the STLQ-629 provides unique combination of parameters in a compact, reliable and inexpensive-in-operation design.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term stability of output radiation. The efficient thermostats used in the STLQ-629 ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ-629 we provided flash lamp life time of more than 50 million pulses and foreseen easy and quick procedure of its replacement.
It should be noted that the laser design allows to replace the flash lamp without removing the laser head upper cover. Such a design concept considerably reduces risks of the optical components contamination as well as increases operational reliability of the device.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
STLQ-629STLQ-629STLQ-629STLQ-629STLQ-629
Model | (1064 nm) | (532 nm) | (355 nm) | (266 nm) | (213 nm) | |
Output energy, mJ, not less than | 1064nm | 200 | 200 | 200 | 200 | 200 |
532nm | - | 90 | 80 | 90 | 80 | |
355nm | - | 50 | - | 50 | ||
266nm | - | 15 | - | |||
213nm1) | - | 5.5 |
Model | For all the Models | |
PRR, Hz | 100 | |
Beam diameter, mm2) | ≤ 5 | |
Pulse-to-pulse energy stability, ±%2) | ± 1.5 | |
Pulse duration, ns2) | 9…12 | |
Divergence, mrad2) | ≤ 1.5 | |
Jitter, ns3) | ± 1.5 | |
Power consumption, W | ≤ 2000 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 740 x 180 x 125 |
Power supply | 620 x 330 x 670 |
* Specifications are subject to change without notice.
1)With the STLG-105 external fifth harmonic generator.
2)At 1064 nm.
3)Relative to the Q-Switch driver external trigger pulse.
Up to 700mJ @ 1064nm in the TEM00 mode and harmonic generators up to 213nm
FEATURES:
TEM00, M2< 2
Oscillator-amplifier configuration
High pulse energy up to 0.7 J
Divergence of 0.25 mrad
High-power radiation in the VIS and UV ranges
All the harmonics available up to 213 nm
Compact single-phase power supply
No external water requirements
The STLQ-830 is a new model of lamp-pumped Nd:YAG laser possessing unique laser radiation characteristics: linewidth of less than 0.1 cm-1, low angular divergence of less than 0.25 mrad and high pulse energy up to 700 mJ at 1064 nm.
Master oscillator with high-stability ring cavity, preamplifier and high-power amplifier form at the laser output TEM00 diffractionally limited beam with high pulse energy and Gaussian profile in the far field.
High spectral radiation brightness with linewidth not more than 10pm and high coherence length of more than 10 cm is ensured by intracavity Fabry-Perot interferometer.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term stability of output radiation. The efficient thermostats used in the STLQ-830 ensure warm-up time of less than 10 min.
To reduce your time expenses on routine service of the StLQ830 we provided flash lamp life time of more than 30 million pulses and foreseen easy and quick procedure of its replacement.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
STLQ-830STLQ-830STLQ-830STLQ-830
Model | (1064 nm) | StLQ830 (532 nm) | (355 nm) | (266 nm) | (213 nm) | |
Output energy, mJ, not less than | 1064nm | 700 | 700 | 700 | 700 | 700 |
532nm | - | 450 | 350 | 450 | 315 | |
355nm | - | 300 | - | 300 | ||
266nm | - | 130 | - | |||
213nm1) | - | 50 |
Model | For all the models | |
PRR, Hz | 10 | |
Beam quality | TEM00, M2<2 | |
Divergence, mrad2) | ≤0.25 | |
Beam diameter, mm2) | 9±0.5 | |
Output linewidth, cm-1, not more than2) | 1 | |
Output linewidth with interferometer, cm-1, not more than2) | 0.1 | |
Pulse duration, ns2),3) | 6…9 | |
Beam pointing stability, µrad, not worse than2) | horizontal plane vertical plane | ±6 ±20 |
Pulse-to-pulse energy stability, ±%2) | ≤ 2 | |
Jitter, ns3),4) | ± 1 | |
Power consumption, W | ≤ 1000 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 650 x 324 x 119 |
Power supply | 700 x 366 x 693 |
* Specifications are subject to change without notice.
1)With the STLG-105 external fifth harmonic generator.
2)At 1064 nm.
3)Without the interferometer.
4)Relative to the Q-Switch driver external trigger pulse.
Up to 1400mJ @ 1064nm and harmonic generators up to 213nm
FEATURES:
Oscillator-amplifier configuration
High pulse energy up to 1.5 J
Excellent beam quality
All the harmonics available up to 213 nm
Compact single-phase power supply
No external water requirements
The STLQ-929 is a series of compact lamp-pumped Nd:YAG lasers built under the scheme master-oscillator – one-pass amplifier and having uncompromising combination of the main parameters: high output power, exceptional beam quality and minimum laser head and power supply dimensions.
The master oscillator of the STLQ-929 laser series, just as that of the STLQ-529 has ring cavity. The principle of operation of the ring cavity scheme and utilisation of pump chambers with high-efficiency diffuse reflectors provide output laser radiation with homogeneous beam profile and exceptional stability of output energy and spatial radiation parameters.
All the critical components of the laser are thermally stabilised which in combination with vibration-proof design ensures unsurpassed long-term stability of output radiation. The efficient thermostats used in the STLQ-929 ensure warm-up time of less than 10 min.
To reduce your time expenses on routine service of the STLQ-929 we provided flash lamp life time of more than 30 million pulses and foreseen easy and quick procedure of its replacement.
Closed-loop water-to-air cooling system is integrated into a compact single-phase laser power supply which can be controlled both from PC and via the remote control unit.
STLQ-929STLQ-929STLQ-929STLQ-929STLQ-929
Model | A (1064 nm) | A (532 nm) | A (355 nm) | A (266 nm) | A (213 nm) | ||||||
PRR, Hz | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | |
Output energy, mJ, not less than | 1064 nm | 1400 | 1400 | 1400 | 1400 | 1400 | |||||
532 nm | - | 800 | 630 | 800 | 630 | ||||||
355 nm (HPV)1),2) | - | 420 | 420 | - | 420 | 420 | |||||
355 nm2) | 390 | 350 | - | 390 | 350 | ||||||
266 nm3) | - | 210 | 190 | - | |||||||
213 nm (HPV)1),4) | - | 45 | 40 | ||||||||
213 nm4) | 40 | 35 | |||||||||
Beam diameter, mm5) | ≤ 11 |
STLQ-929STLQ-929STLQ-929STLQ-929STLQ-929
Model | B (1064 nm) | B (532 nm) | B (355 nm) | B (266 nm) | B (213 nm) | ||||||
PRR, Hz | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | 5 | 10 | |
Output energy, mJ, not less than | 1064 nm | 1000 | 1000 | 1000 | 1000 | 1000 | |||||
532 nm | - | 600 | 450 | 600 | 450 | ||||||
355 nm (HPV)1),2) | - | 300 | 300 | - | 300 | 300 | |||||
355 nm2) | 280 | 250 | - | 280 | 250 | ||||||
266 nm3) | - | 200 | 180 | - | |||||||
213 nm (HPV)1),4) | - | 45 | 40 | ||||||||
213 nm4) | 40 | 35 | |||||||||
Beam diameter, mm5) | ≤ 10 |
Model | For all the Models | |
Pulse-to-pulse energy stability, ±%5) | < 2.5 | |
Pulse duration, ns5) | 10…12 | |
Divergence, mrad5) | ≤ 1.5 | |
Jitter, ns6) | ±1 | |
Power consumption, W | ≤ 1200 | |
Cooling system | water-to-air | |
Dimensions (LxWxH), mm | Laser head | 625 x 220 x 125 |
Power supply | 700 x 366 x 693 |
* Specifications are subject to change without notice.
1)For the high-power version at 355 nm.
2)With the STLG-103T external third harmonic generator.
3)With the STLG-103F external fourth harmonic generator.
4)With the STLG-105 external fifth harmonic generator.
5)At 1064 nm.
6)Relative to the Q-Switch driver external trigger pulse.
We present a new model of completely air-cooled pulsed diode-pumped Nd:YAG laser. The STQX-500 delivers 160mJ at 1064 nm in nanosecond pulses at repetition rates up to 20Hz. The STQX-500 laser features long-life laser diode bars and delivers excellent pulse-to-pulse and long-term stability which is ideally suited for use in scientific, industrial, and medical applications. Diode pumping reduces size, improves reliability, and eliminates most maintenance operations. Minimum service costs are conditioned by optical pumping using laser diode bars with more than 109 pulses lifetime. Stability of the parameters and the laser reliability are guaranteed due to dustproof housing design and thermal stabilization of the optical cavity. The possibility of operation in the VIS and UV spectral range thanks to small external harmonic generators will expand your opportunities. Compact laser design and complete air cooling not only simplify application of this device as a stand-alone unit, but also allow to integrate it into any equipment.
High-power output of 160mJ at 20Hz
Air cooling and no water required
Smooth flat-top beam profile
Vis and UV harmonic generators
OEM/industrial design for 24/7 operation
Long diode lifetime over 1 billion shots
Turn-key operation
Wavelength,nm | 355 |
Pulseenergy,mJ -at1064nm -at532nm 1) -at355nm 2) -at266nm 3) | ≥160 ≥80 ≥50 ≥25 |
Pulserepetitionrate4),Hz | 1…20 |
Pulseenergystability 5) (Std.Dev.),% | ≤1.5 |
Pulsewidth5) (FWHM),ns | 9...10 |
Beamdivergence 5),mrad | ≤1.5 |
Beamdiameter 5),mm | <5 |
Jitter(Std.Dev.) 6),ns | ≤1.0 |
Electricalservice | 100…240V,50/60Hz,≤500W |
Coolingsystem | Air |
Dimensions,mm -Laserheadandharmonicgenerators(L×W×H) -Powersupplyunit(W×D×H) | 375x230x115 405х350х150 |
Environmentalrequirements | |
Roomtemperature | 15-27ºС (airconditioningrecommended) |
Relativehumidity | ≤60%(noncondensing) |
1)With external third harmonic generator model STQH-120;
2)With external third harmonic generator model STQH-130;
3)With external fourth harmonic generator model STQH-140;
4)You can choose any PRR from 1Hz to 20Hz when placing an order. All parameters are specified for 20 Hz;
5)Specified at 1064 nm;
6)With respect to external trigger pulse.
The system consists of two modules – the DPSS pulsed laser model STQX-500 (at 1064nm) and removable module for any harmonic generator model STQH (at 532nm, 355nm, 266nm). So, the customer can work either with 1064nm or with any harmonic in depend on applications. The removable harmonic generator module can be fix at STQX-500 output or remove by manual.
Our DPSS lasers do not require visit of engineer for installation procedure due to special technical design that exclude the possible misalignment of the laser’s optical scheme. The end user can start to work STQX-500 laser by himself without any troubles. All necessary information for working is presented in the user manual and video guide instruction. Even the specialist without technical skills can start and work with QX500 laser comfortable.
A leading supplier and manufacturer of a wide range of photonics products such as lasers,laser parts & machines.
Office: 10 Bukit Batok Crescent #07-02 The Spire Singapore 658079
Tel: +65 63167112
Fax: +65 63167113
Whatsapp: +65 91904616