Description
The Quantas-Q-SPARK-266 series is a compact, air-cooled, diode-pumped, Q-switched laser designed for researchers and application specialists. It operates at a wavelength of 266 nm and delivers pulse energies ranging from 0.1 mJ to 2.5 mJ, with a repetition rate of up to 100 Hz. With available multiple harmonic options, remote monitoring, control, and support, as well as active or passive Q-switching, this laser offers versatility and reliability for various applications.
Quantas-Q-SPARK-266: High Energy Compact Nanosecond DPSS Laser
Specifications
| Avg. Power: | 0.02 W |
|---|---|
| Wavelength: | 266 nm |
| Repetition Rate: | 0.01 – 0.1 kHz |
| Pulse Duration: | 0.8 ns |
| Pulse-to-Pulse Stability (RMS): | 1.5 % |
| Cooling: | Air |
| Pulse Energy: | 0.1 to 2.5 mJ |
| Typical Pulse Duration: | 2 ns |
| Linewidth: | SLM |
| Power Drift: | ± 3.0 % |
| Beam Divergence: | <1.5 mrad |
| Polarization: | linear, horizontal |
| Jitter (RMS): | 1 µs |
| Transmission Range: | 0.5-95 % |
| Laser Head (W×L×H): | 140 × 277 × 135 mm³ |
| Controller Unit (W×L×H): | 108 × 191 × 59 mm³ |
| Power Adapter (W×L×H) Typical (for +12 VDC Output): | 50 × 125 × 32 mm³ |
| Ambient Temperature: | 15-30 °C |
| Relative Humidity (non-condensing): | 10 – 80 % |
| Mains Voltage:: | 0 – 230 VAC, single phase, 47 – 63 Hz |
| Q-Switch Type: | passive, Cr:YAG/active, Pockels cell |
Got questions about specs? Use the inquiry form to ask.
Features
- Air-cooled Q-switched laser: Water-free, diode-pumped laser platform designed for reliable short-pulse operation without external chiller requirements.
- High pulse energy at 1064 nm: Delivers up to 20 mJ pulse energy at the fundamental wavelength for demanding laser ablation, LIBS, LiDAR, and spectroscopy applications.
- High peak power output: Generates up to 20 MW peak power, enabling efficient material interaction, plasma generation, and nonlinear optical processes.
- Sub-nanosecond and nanosecond pulse options: Short pulse duration down to 750 ps, with passively Q-switched models offering >5 mJ pulse energy and E-O Q-switched models providing up to 20 mJ with <1.5 ns pulse duration.
- Flexible repetition rate: Available with pulse repetition rates from 10 Hz to 100 Hz to support laboratory, industrial, and OEM integration requirements.
- Optional harmonic wavelengths: Built-in 2nd, 3rd, or 4th harmonic generator options provide access to 532 nm, 355 nm, and 266 nm outputs for UV and visible laser applications.
- Gaussian-like beam quality: Optimized end-pumped laser crystal design produces low-divergence, Gaussian-like pulses in a compact and energy-efficient package.
- Long pump diode lifetime: Pump diodes rated for >2 Gshot lifetime, supporting lower maintenance and long-term operational stability.
- Built-in synchronization output: Integrated sync pulse generator enables precise triggering of user equipment, detectors, cameras, delay generators, and data acquisition systems.
- Ethernet remote control: Built-in Ethernet interface with web-server control and API support allows convenient remote monitoring, operation, and OEM system integration.
- Optional motorized attenuator: Attachable PC-controlled attenuator enables automated pulse energy adjustment at the fundamental or harmonic wavelength.
- Optional pulse energy monitor: Attachable energy monitoring module with analog and/or digital output supports real-time pulse energy tracking and process control.
- Auxiliary wavelength access: Optional auxiliary exit port allows access to residual harmonic generator wavelengths for multi-wavelength experimental setups.
- Optional fiber-coupled output: Fiber output configuration is available by request for flexible beam delivery and integration into compact optical systems.
- Compact OEM-ready design: Air-cooled, water-free construction is ideal for portable instruments, integrated photonics systems, analytical equipment, and field-deployable laser platforms.
- Ideal for LIBS and analytical spectroscopy: High pulse energy and short pulse duration make the laser well suited for Laser-Induced Breakdown Spectroscopy, Raman spectroscopy, Time-Resolved Spectroscopy, and Time-of-Flight Spectroscopy.
- Suited for LiDAR and ranging: Nanosecond and sub-nanosecond pulse performance supports precision Light Detection and Ranging, remote sensing, and time-of-flight measurement systems.
- Effective for micromachining and ablation: High peak power and short pulse width enable precise laser ablation, microprocessing, and material modification with reduced thermal impact.
- Medical and research applications: Applicable for dermatology, ophthalmology, tattoo removal research, TDTR, plasma generation, and advanced photonics experiments.
Applications
Applications for Air-Cooled Short Pulse Q-Switched Laser
- Laser-Induced Breakdown Spectroscopy (LIBS): High-peak-power nanosecond and sub-nanosecond pulses for elemental analysis of metals, minerals, soils, powders, liquids, coatings, and industrial process materials.
- LiDAR and Laser Range Finding: Compact air-cooled 1064 nm pulsed laser source for remote sensing, distance measurement, atmospheric monitoring, 3D mapping, topographic scanning, and target detection.
- Laser Ablation: Short-pulse laser ablation of metals, ceramics, semiconductors, glass, polymers, thin films, and composite materials with reduced heat-affected zones.
- Precision Micromachining: High peak power pulses for micro-drilling, micro-cutting, surface texturing, patterning, trimming, and fine material removal in R&D and industrial manufacturing.
- Time-of-Flight Spectroscopy: Sub-nanosecond and nanosecond pulse generation for time-of-flight measurements, particle detection, ion studies, and fast optical diagnostics.
- Time-Resolved Spectroscopy: Short optical pulses for studying fast physical, chemical, and biological processes, including transient absorption, fluorescence decay, and excited-state dynamics.
- Raman Spectroscopy: Pulsed laser excitation for Raman analysis, time-gated Raman spectroscopy, material identification, chemical sensing, and suppression of fluorescence background.
- Laser-Induced Fluorescence (LIF): Excitation source for fluorescence diagnostics, flow visualization, combustion research, plasma studies, and molecular detection.
- Photoacoustic Spectroscopy and Imaging: High-energy pulsed laser source for generating acoustic waves in materials, gases, liquids, and biological samples for sensing and imaging applications.
- Pump-Probe Experiments: Short pulse duration and synchronization capabilities for ultrafast and fast dynamics research, material relaxation studies, and optical response measurements.
- Time Domain Thermoreflectance (TDTR): Pulsed laser source for thermal conductivity measurements, thin-film thermal analysis, semiconductor characterization, and heat transport studies.
- Plasma Generation and Diagnostics: High peak power laser pulses for creating and analyzing laser-induced plasmas in spectroscopy, propulsion research, materials science, and high-energy-density studies.
- Mass Spectrometry Ionization: Pulsed laser source for laser desorption, laser ionization, MALDI-related research, and time-of-flight mass spectrometry applications.
- Nonlinear Optics Research: Fundamental and harmonic wavelength outputs for nonlinear frequency conversion, optical parametric studies, multiphoton excitation, and high-intensity laser-matter interaction experiments.
- Harmonic Generation Applications: Optional 532 nm, 355 nm, and 266 nm outputs for UV and visible excitation in spectroscopy, photochemistry, fluorescence, semiconductor processing, and advanced optical testing.
- Semiconductor Inspection and Processing: Short-pulse laser source for wafer inspection, defect analysis, thin-film ablation, photovoltaic research, and microelectronics development.
- Thin-Film Removal and Patterning: Controlled pulsed laser energy for selective removal of coatings, oxides, metals, transparent conductive films, and multilayer structures.
- Surface Modification and Texturing: Laser-based surface treatment for improving adhesion, wettability, tribological properties, optical response, and functional surface performance.
- Laser Cleaning Research: Non-contact removal of contaminants, oxides, paint layers, residues, and surface deposits from metals, stone, ceramics, and precision components.
- Material Damage Threshold Testing: High-peak-power pulsed source for laser-induced damage threshold testing of optics, coatings, crystals, fibers, sensors, and photonic components.
- Optical Sensor Testing and Calibration: Nanosecond and sub-nanosecond pulse source for testing photodetectors, avalanche photodiodes, photomultipliers, gated cameras, and high-speed optical sensors.
- High-Speed Imaging Illumination: Short optical pulses for stroboscopic illumination, motion freezing, ballistic imaging, flow imaging, and transient event visualization.
- Particle Image Velocimetry (PIV) and Flow Diagnostics: Pulsed laser illumination for fluid dynamics, aerodynamic testing, combustion studies, and particle tracking applications.
Frequently Asked Questions
How much pulse energy can this laser deliver at 266 nm?
What is the pulse duration range for this laser?
Can the Quantas-Q-SPARK-266 operate at different repetition rates?
Is the laser air-cooled or does it require water cooling?
How is the laser controlled for precise operations?
Does the laser offer options for pulse energy adjustment?
Is it possible to monitor the pulse energy?
What is the beam quality of the Quantas-Q-SPARK-266?
How reliable are the pump diodes in terms of lifetime?
Got more questions? Use the inquiry form to ask the supplier directly.
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