Picosecond Microchip Lasers
![](https://www.thorlabs.com/Images/GuideImages/14322_Picosecond_Pulsed_Laser_4.jpg)
- Sub-Nanosecond Pulse Duration
- High Energy (40 µJ, 9 kHz) Version
- High Repetition Rate (2 µJ, 100 kHz) Version
- Turn-Key Material Processing Capability
- High Quality Beam Profile
QSL103A
Picosecond Microchip Laser Head,
40 µJ (Typ.), 9 kHz Rep. Rate (Typ.)
Controller Included
The head of the QSL106B laser (controller included) is mounted on the QSLB1 Base (sold separately below), increasing the laser beam height to 75.0 mm and providing additional thermal stability.
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Janis Valdmanis, Ph.D. Optics
Ultrafast Optoelectronics
General Manager
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Applications
- Material Processing
- Photoacoustic Imaging
- Fluorescence Lifetime Imaging
- Harmonic Generation
- LIDAR
- Laser-Induced Breakdown Spectroscopy
Key Specificationsa | ||
---|---|---|
Item # | QSL103A | QSL106B |
Center Wavelength | 1030 nm ± 1 nm | 1064 nm ± 1 nm |
Average Output Powerb | 350 - 450 mW | 150 - 250 mW |
Repetition Rateb | 8 - 10 kHz | 80 - 120 kHz |
Pulse Energy (Typical)b | 35 - 50 µJ | 1.7 - 2.2 µJ |
Output Peak Power | >65 kW | >2.5 kW |
Pulse Durationb | 500 ps ± 100 ps | 550 ps ± 100 ps |
Ellipticity | >0.94 | >0.92 |
Features
- 1030 nm or 1064 nm Center Wavelengths
- Sub-Nanosecond Pulse Duration
- Compatible with 30 mm Cage System
- Integrated Control Electronics
- Trigger Output for Pulse Monitoring
- Typical Repetition Rate of 9 kHz or 100 kHz Available
Thorlabs' Q-Switched Picosecond Microchip Lasers are compact laser systems designed to provide a turnkey, alignment-free solution for picosecond pulses at 1030 nm or 1064 nm. This compact microchip laser cavity design with a fiber-coupled pump laser produces a high-quality beam in both our high pulse energy version (Item # QSL103A) and high repetition rate version (Item # QSL106B), giving a range of options that are ideal for a variety of material processing applications or harmonic generation. For full performance specifications, please see the Specs tab. Each picosecond laser system includes a head and a controller that have integrated drive electronics, temperature stabilization, and safety interlocks. The picosecond laser head also includes a manual-slide shutter, which can be used to cover the laser aperture.
Laser Selection
Varied material processing will require different laser parameters. Producing 40 µJ pulses with around 500 ps duration, Item # QSL103A is a high peak power laser capable of high-volume material removal and efficient harmonic generation. For precision applications requiring a small mode-field diameter and high throughput, the higher repetition rate QSL106B laser with a typical repetition rate of 100 kHz is an appropriate selection. This higher repetition rate version may also be useful as a seed laser for high-power fiber amplification, lending itself toward efficient and high-volume material removal processes.
Optical Emission
The output from these sources is uncollimated and weakly divergent to allow the user control over the beam diameter. The laser head features SM05 (0.535"-40) internal threading on the beam aperture, as well as 4-40 threads for compatibility with our 30 mm cage components, as seen in the image in the far right. To compensate for any beam misalignment at the laser output, mount a collimating lens in a cage plate with XY translation.
For external beam attenuation, we recommend using Thorlabs' neutral density filters. A SHB025 diaphragm shutter mounted in a SHCP025 adapter (for cage system compatibility) can also be added in front of the laser aperture to remotely block the laser output.
Mounting
The laser head housing includes six clearance holes for mounting, including four for 8-32 (M4) cap screws and two for 1/4"-20 (M6) cap screws. When directly mounted to an optical table or breadboard, the output beam height is 0.98" (25.0 mm).
Some applications may require an increased beam height, and we recommend using the QSLB1 Base (offered separately below) as a convenient solution that provides thermal stability, as seen in the image to the right. Alternatively, the laser head can be mounted on a raised breadboard.
Electrical Connections
Each laser system is shipped with an umbilical cable for connecting the laser head and controller. This laser system integrates all required drive electronics, safety interlocks, and temperature stabilization needed for operation; a block diagram with more details can be found on the Specs tab. Note that the power supply is built into the unit and a region-specific power cord is included with each laser.
Panel Features
A trigger out (SMA female) is included on the laser head, which can be used for monitoring the output pulse and repetition rate, as well as for timing the arrival of a pulse with an electronic trigger. An indicator LED is also included for the laser emission.
All required safety features are included with the controller, including key switch, interlock pin, and momentary switch to enable the laser output; see the Front & Back Panels tab for more details on the panel features. Note that the controller front panel includes dual color (red/green) status LEDs for the TEC and laser emission status, which are designed to be visible through most safety glasses.
Item # | QSL103A | QSL106B |
---|---|---|
Average Output Powera | 350 - 450 mW | 150 - 250 mW |
Repetition Ratea | 8 - 10 kHz | 80 - 120 kHz |
Pulse Energy (Typical)a | 35 - 50 µJ | 1.7 - 2.2 µJ |
Output Peak Power | >65 kW | >2.5 kW |
Pulse Durationa | 500 ps ± 100 ps | 550 ps ± 100 ps |
Typical Pulses | ![]() Click to Enlarge |
![]() Click to Enlarge |
Center Wavelength | 1030 nm ± 1 nm | 1064 nm ± 1 nm |
Output Spectrum (Typical) | ![]() Click to Enlarge |
![]() Click to Enlarge |
Power Stability (RMS) | <1% over 8 hours | <0.5% over 8 hours |
Beam Diameter (1/e2), at 100 mm | 3 mm | |
Beam Divergence (1/e2), Typical | 10 mrad | |
Beam Quality (M2) | <1.2 | <1.3 |
Ellipticity | >0.94 | >0.92 |
Beam Profile (Typical) | ![]() Click to Enlarge |
![]() Click to Enlarge |
Power, Environmental, and Physical Specifications | |
---|---|
AC Input Frequency Range to Power Supply | 50 - 60 Hz |
AC Input Voltage to Power Supply | 100 V to 250 VAC |
Power Consumption (Typical) | 22 W |
Trigger Out | 1 VPP, 50 Ω |
Relative Trigger Jitter | <10 ps |
Optical Repetition Rate Jitter (RMS) | <5% of Repetition Rate |
Operating Temperature Range | 10 to 45 °C |
Storage Temperature Range | 0 to 60 °C |
Laser Head Weight | 0.8 kg |
Laser Controller Weight | 1.7 kg |
Laser Head Dimensions | 136.3 mm x 88.9 mm x 47.1 mm (5.37" x 3.50" x 1.85") |
Laser Controller Dimensions | 307.4 mm x 149.8 mm x 84.0 mm (12.10" x 5.90" x 3.31") |
![QSL Block Diagram](https://www.thorlabs.com/images/tabimages/QSL_Block_Diagram_D1-450.gif)
Click to Enlarge
Block diagram depicting the internal architecture of the laser control system with drive electronics, safety interlocks, and temperature stabilization. The dual color TEC LED indicator (red/green) blinks during the 45 to 90 s warm up and glows continuously when temperature stability has been achieved.
QSL Series Laser Head Front and Back Panels
Front Panel | |
---|---|
Call Out | Description |
1 | Laser Aperture with SM05 (0.535”-40) Internal Threads |
2 | Manual Shutter |
3 | 4-40 Threads Spaced for 30 mm Cage Compatibility (4 Places) |
Back Panel | |
---|---|
Call Out | Description |
1 | Receptacle for Umbilical Cable to Laser Controller |
2 | Trigger Out (Female SMA) |
3 | Laser Emission Indicator LED |
QSL Series Controller Front and Back Panels
Front Panel | |
---|---|
Call Out | Description |
1 | Interlock Key Switch |
2 | TEC Status LED |
3 | Laser Emission Status LED |
4 | Laser Enable Switch |
Back Panel | |
---|---|
Call Out | Description |
1 | Main Power Switch |
2 | Interlock Connector |
3 | Fuse Holder |
4 | AC Power Cord Connector |
5 | Interlock Error Status LED |
6 | Head Error Status LED |
7 | Receptacle for Umbilical Cable for Laser Head |
Laser Safety and Classification
Safe practices and proper usage of safety equipment should be taken into consideration when operating lasers. The eye is susceptible to injury, even from very low levels of laser light. Thorlabs offers a range of laser safety accessories that can be used to reduce the risk of accidents or injuries. Laser emission in the visible and near infrared spectral ranges has the greatest potential for retinal injury, as the cornea and lens are transparent to those wavelengths, and the lens can focus the laser energy onto the retina.
Safe Practices and Light Safety Accessories
- Laser safety eyewear must be worn whenever working with Class 3 or 4 lasers.
- Regardless of laser class, Thorlabs recommends the use of laser safety eyewear whenever working with laser beams with non-negligible powers, since metallic tools such as screwdrivers can accidentally redirect a beam.
- Laser goggles designed for specific wavelengths should be clearly available near laser setups to protect the wearer from unintentional laser reflections.
- Goggles are marked with the wavelength range over which protection is afforded and the minimum optical density within that range.
- Laser Safety Curtains and Laser Safety Fabric shield other parts of the lab from high energy lasers.
- Blackout Materials can prevent direct or reflected light from leaving the experimental setup area.
- Thorlabs' Enclosure Systems can be used to contain optical setups to isolate or minimize laser hazards.
- A fiber-pigtailed laser should always be turned off before connecting it to or disconnecting it from another fiber, especially when the laser is at power levels above 10 mW.
- All beams should be terminated at the edge of the table, and laboratory doors should be closed whenever a laser is in use.
- Do not place laser beams at eye level.
- Carry out experiments on an optical table such that all laser beams travel horizontally.
- Remove unnecessary reflective items such as reflective jewelry (e.g., rings, watches, etc.) while working near the beam path.
- Be aware that lenses and other optical devices may reflect a portion of the incident beam from the front or rear surface.
- Operate a laser at the minimum power necessary for any operation.
- If possible, reduce the output power of a laser during alignment procedures.
- Use beam shutters and filters to reduce the beam power.
- Post appropriate warning signs or labels near laser setups or rooms.
- Use a laser sign with a lightbox if operating Class 3R or 4 lasers (i.e., lasers requiring the use of a safety interlock).
- Do not use Laser Viewing Cards in place of a proper Beam Trap.
Laser Classification
Lasers are categorized into different classes according to their ability to cause eye and other damage. The International Electrotechnical Commission (IEC) is a global organization that prepares and publishes international standards for all electrical, electronic, and related technologies. The IEC document 60825-1 outlines the safety of laser products. A description of each class of laser is given below:
Class | Description | Warning Label |
---|---|---|
1 | This class of laser is safe under all conditions of normal use, including use with optical instruments for intrabeam viewing. Lasers in this class do not emit radiation at levels that may cause injury during normal operation, and therefore the maximum permissible exposure (MPE) cannot be exceeded. Class 1 lasers can also include enclosed, high-power lasers where exposure to the radiation is not possible without opening or shutting down the laser. | ![]() |
1M | Class 1M lasers are safe except when used in conjunction with optical components such as telescopes and microscopes. Lasers belonging to this class emit large-diameter or divergent beams, and the MPE cannot normally be exceeded unless focusing or imaging optics are used to narrow the beam. However, if the beam is refocused, the hazard may be increased and the class may be changed accordingly. | ![]() |
2 | Class 2 lasers, which are limited to 1 mW of visible continuous-wave radiation, are safe because the blink reflex will limit the exposure in the eye to 0.25 seconds. This category only applies to visible radiation (400 - 700 nm). | ![]() |
2M | Because of the blink reflex, this class of laser is classified as safe as long as the beam is not viewed through optical instruments. This laser class also applies to larger-diameter or diverging laser beams. | ![]() |
3R | Class 3R lasers produce visible and invisible light that is hazardous under direct and specular-reflection viewing conditions. Eye injuries may occur if you directly view the beam, especially when using optical instruments. Lasers in this class are considered safe as long as they are handled with restricted beam viewing. The MPE can be exceeded with this class of laser; however, this presents a low risk level to injury. Visible, continuous-wave lasers in this class are limited to 5 mW of output power. | ![]() |
3B | Class 3B lasers are hazardous to the eye if exposed directly. Diffuse reflections are usually not harmful, but may be when using higher-power Class 3B lasers. Safe handling of devices in this class includes wearing protective eyewear where direct viewing of the laser beam may occur. Lasers of this class must be equipped with a key switch and a safety interlock; moreover, laser safety signs should be used, such that the laser cannot be used without the safety light turning on. Laser products with power output near the upper range of Class 3B may also cause skin burns. | ![]() |
4 | This class of laser may cause damage to the skin, and also to the eye, even from the viewing of diffuse reflections. These hazards may also apply to indirect or non-specular reflections of the beam, even from apparently matte surfaces. Great care must be taken when handling these lasers. They also represent a fire risk, because they may ignite combustible material. Class 4 lasers must be equipped with a key switch and a safety interlock. | ![]() |
All class 2 lasers (and higher) must display, in addition to the corresponding sign above, this triangular warning sign. | ![]() |
Pulsed Laser Emission: Power and Energy Calculations
Determining whether emission from a pulsed laser is compatible with a device or application can require referencing parameters that are not supplied by the laser's manufacturer. When this is the case, the necessary parameters can typically be calculated from the available information. Calculating peak pulse power, average power, pulse energy, and related parameters can be necessary to achieve desired outcomes including:
- Protecting biological samples from harm.
- Measuring the pulsed laser emission without damaging photodetectors and other sensors.
- Exciting fluorescence and non-linear effects in materials.
Pulsed laser radiation parameters are illustrated in Figure 1 and described in the table. For quick reference, a list of equations is provided below. The document available for download provides this information, as well as an introduction to pulsed laser emission, an overview of relationships among the different parameters, and guidance for applying the calculations.
Equations: |
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and | ![]() |
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Peak power and average power calculated from each other: |
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and | ![]() |
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Peak power calculated from average power and duty cycle*: | ||||
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*Duty cycle (![]() |
![Pulsed Laser Emission Parameters](https://www.thorlabs.com/images/tabimages/RealPulseParameters_A5-350.gif)
Click to Enlarge
Figure 1: Parameters used to describe pulsed laser emission are indicated in the plot (above) and described in the table (below). Pulse energy (E) is the shaded area under the pulse curve. Pulse energy is, equivalently, the area of the diagonally hashed region.
Parameter | Symbol | Units | Description | ||
---|---|---|---|---|---|
Pulse Energy | E | Joules [J] | A measure of one pulse's total emission, which is the only light emitted by the laser over the entire period. The pulse energy equals the shaded area, which is equivalent to the area covered by diagonal hash marks. | ||
Period | Δt | Seconds [s] | The amount of time between the start of one pulse and the start of the next. | ||
Average Power | Pavg | Watts [W] | The height on the optical power axis, if the energy emitted by the pulse were uniformly spread over the entire period. | ||
Instantaneous Power | P | Watts [W] | The optical power at a single, specific point in time. | ||
Peak Power | Ppeak | Watts [W] | The maximum instantaneous optical power output by the laser. | ||
Pulse Width | ![]() |
Seconds [s] | A measure of the time between the beginning and end of the pulse, typically based on the full width half maximum (FWHM) of the pulse shape. Also called pulse duration. | ||
Repetition Rate | frep | Hertz [Hz] | The frequency with which pulses are emitted. Equal to the reciprocal of the period. |
Example Calculation:
Is it safe to use a detector with a specified maximum peak optical input power of 75 mW to measure the following pulsed laser emission?
- Average Power: 1 mW
- Repetition Rate: 85 MHz
- Pulse Width: 10 fs
The energy per pulse:
seems low, but the peak pulse power is:
It is not safe to use the detector to measure this pulsed laser emission, since the peak power of the pulses is >5 orders of magnitude higher than the detector's maximum peak optical input power.
Posted Comments: | |
Jiwon Yune
 (posted 2024-03-24 15:35:42.9) What is the best way to trigger this laser source for LIBS? Optical shutter might be too slow for my need. cdolbashian
 (posted 2024-03-29 02:49:06.0) Thank you for reaching out to us with this inquiry. This laser source cannot be triggered as you intend, but there are other workarounds which can be used. I have contacted you directly to discuss such options. |
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![QSL Collimating Lens](https://www.thorlabs.com/images/tabimages/QSL_Collimating_Lens_A3-150.jpg)
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An AC127-075-B achromatic doublet lens is mounted on the QSL103A laser head using a CP1XY cage plate and ER1.5 cage rods.
![QSL Mounted](https://www.thorlabs.com/images/tabimages/QSL_Laser_Drilling_A1-150.jpg)
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Laser-Drilled Hole Through a 100 µm Thick Aluminum Sheet
- Sub-ns Pulse Duration
- µJ-Level Pulse Energies
- Laser Head and Controller Included
These Q-Switched Picosecond Microchip Lasers have a compact design and provide picosecond pulses at 1030 nm or 1064 nm. The laser head features 4-40 threads for compatibility with our 30 mm cage components, for easy integration of an external collimating lens (see image to the far right), as well as SM05 (0.535"-40) internal threading on the beam aperture. These lasers have a variety of applications, including photoacoustic imaging, fluorescence lifetime imaging, LIDAR, and laser-induced breakdown spectroscopy.
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![QSL Mounted](https://www.thorlabs.com/images/TabImages/QSL106B_QSLB1_Side_A1-450.jpg)
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The QSL106B laser head is fixed to a QSLB1 Base and Riser, increasing the beam height.
- Raises Laser Beam Height to 2.95" (75.0 mm)
- Provides Thermal Stability
- Mounts Directly to Imperial and Metric Optical Tables
The QSLB1 Base and Riser is an aluminum block that raises the beam height of our Q-Switched Microchip Laser Systems to 2.95" (75.0 mm) while also providing thermal stability to the output. The base features two M6 x 1.0 tapped holes for securing the laser head; two M6 x 14 cap screws (4 mm hex) are included with each base. For mounting to the optical table, the base also has four clearance holes for 1/4"-20 (M6) cap screws.