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:
Typical Applications:
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 | 3~30KHz | 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:
Typical Applications:
Specifications:
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:
Typical Applications:
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:
Typical Applications:
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
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 |
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 |
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 | <=0.6 |
Pointing stability (urad) | <=30 | <=30 | £30 | <=5 | |
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 |
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:
Applications:
Laser ablation
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 |
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:
Applications:
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 |
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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 optional12-15ns, 15-20ns optional | ||||||||||||||||||
| Divergence4 | <=0.5mrad for VRM, <=4mrad for MM |
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Peak to average | <=1.8:1 |
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Polarisation | Linear 100:1 |
Cross | |||||||||||||||||
Energy stability5 RMS | <1% |
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Power drift RMS | <5% |
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Pointing stability | <50urad |
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Jitter6 RMS | <1ns |
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Warm up time7 | <5min |
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
The STLQ115 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 STLQ115 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 STLQ115 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 STLQ115 incorporates LiNbO3 electrooptical 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 STLQ115 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 STLQ115 laser a number of essential operational advantages:
Model | STLQ115 (1064 nm) | STLQ115 (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 |
Model | STLQ115 (1064 nm) | STLQ115 (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 |
Model | STLQ115 (355 nm) | STLQ115 (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
The STLQ215 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
STLQ215 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 STLQ215 ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ215 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 STLQ215 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 STLQ215 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 STLQ215 is an ideal instrument for such applications as:
Model | STLQ215 (1064 nm) | STLQ215 (532 nm) | STLQ215 (355 nm) | STLQ215 (266 nm) | STLQ215 (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 |
Up to 100mJ @ 1064nm and 50mJ @ 532nm in each pulse
The STLQ215-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 STLQ215-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 STLQ215-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 STLQ215-D ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ215-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.
Model | STLQ215-D | |
---|---|---|
Maximum PRR, Hz 1) | 20 | |
Each pulse output energy, mJ, not less than 2) | 1064nm | 100 |
532nm | 50 | |
Pulse duration, ns 2) | 6…10 | |
Adjustable delay between pulses, μs | 0…80 | |
Step of adjustable delay between pulses, μs | 1 (0.1 – upon request) | |
Beam diameter, mm 3) | ≤ 5 | |
Divergence, mrad 3) | ≤ 1.5 | |
Pulse-to-pulse energy stability, ±% 3) | < 2.5 | |
Beam pointing stability, mrad, not worse than 3) | 0.1 | |
Jitter, ns 4) | < 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.
Up to 500mJ at 1064nm and harmonic generators up to 213nm
FEATURES:
The STLQ529 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 STLQ529 series are based on ring cavity and incorporate a pump chamber with diffuse ceramic reflector. Due to this technical solution the STLQ529 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 STLQ529 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 STLQ529 ensure warm-up time of less than 10 min.
To reduce your time expenses on routine service of the STLQ529 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.
Model | STLQ529A (1064 nm) | STLQ529A (532 nm) | STLQ529A (355 nm) | STLQ529A (266 nm) | STLQ529A (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 |
Model | STLQ529B (1064 nm) | STLQ529B (532 nm) | STLQ529B (355 nm) | STLQ529B (266 nm) | STLQ529B (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 |
Model | STLQ529C (1064 nm) | STLQ529C (532 nm) | STLQ529C (355 nm) | STLQ529C (266 nm) | STLQ529C (213 nm) | |
PRR, Hz | 50 | |||||
Output energy, mJ, not less than | 1064 nm | 150 | 150 | 150 | 150 | 150 |
532 nm | - | 80 | 65 | 80 | 65 | |
355 nm | - | 40 | - | 40 | ||
266 nm | - | 20 | - | |||
213 nm2) | - | 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.
Up to 200mJ @ 1064nm and harmonic generators up to 213nm
The combination of high laser pulse energy, high PRR and excellent beam quality unattainable for most conventional models is the peculiarity of the STLQ629 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 STLQ629 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 STLQ629 ensure warm-up time of less than 10min.
To reduce your time expenses on routine service of the STLQ629 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.
Model | STLQ629 (1064 nm) | STLQ629 (532 nm) | STLQ629 (355 nm) | STLQ629 (266 nm) | STLQ629 (213 nm) | |
Output energy, mJ, not less than | 1064 nm | 200 | 200 | 200 | 200 | 200 |
532 nm | - | 90 | 80 | 90 | 80 | |
355 nm | - | 50 | - | 50 | ||
266 nm | - | 15 | - | |||
213 nm1) | - | 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 STLG105 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
The STLQ830 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 pergence 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 STLQ830 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.
Model | STLQ830 (1064 nm) | StLQ830 (532 nm) | STLQ830 (355 nm) | STLQ830 (266 nm) | STLQ830 (213 nm) | |
---|---|---|---|---|---|---|
Output energy, mJ, not less than | 1064 nm | 700 | 700 | 700 | 700 | 700 |
532 nm | - | 450 | 350 | 450 | 315 | |
355 nm | - | 300 | - | 300 | ||
266 nm | - | 130 | - | |||
213 nm1) | - | 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.
Up to 1400mJ @ 1064nm and harmonic generators up to 213nm
The STLQ929 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 STLQ929 laser series, just as that of the STLQ529 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 STLQ929 ensure warm-up time of less than 10 min.
To reduce your time expenses on routine service of the STLQ929 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.
Model | STLQ929A (1064 nm) | STLQ929A (532 nm) | STLQ929A (355 nm) | STLQ929A (266 nm) | STLQ929A (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 |
Model | STLQ929B (1064 nm) | STLQ929B (532 nm) | STLQ929B (355 nm) | STLQ929B (266 nm) | STLQ929B (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.
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