Learn More About Active Q-Switch Lasers
Active q-switches could be a mechanical shutter device, an optical chopper wheel, or spinning mirror / prism inside the optical cavity. However, typically, they are in the form of a modulator, such as an acousto-optic, magneto-optic, or electro-optic device (e.g., a Pockels cell or Kerr cell). Active q-switches rely on a controllable on/off ability and rapidly adjust the lasers cavity loss. A perfect example of this is an acousto-optic modulator, which, when activated creates a grating which deflects many spontaneously emitted photons out of the laser cavity. However, once the modulator is turned off, it allows the spontaneous photons to pass through and initiate stimulated emission.
Should I choose an actively q-switched or passively q-switched laser?
There are pros and cons to both types (active & passive). There are some main points to consider when determining which type best suits your application needs:
- Cost – passively q-switched lasers are less expensive and complex than actively q-switched lasers
- Size – passively q-switched lasers can be significantly more compact than actively q-switched lasers
- Triggering – actively q-switched lasers allow precise triggering control over pulses and does not suffer from the increased pulse to pulse jitter, as opposed to passively q-switched lasers
- Pulse Energy – actively q-switched lasers typically provide higher pulse energies than passively q-switched lasers
Our Active Q-Switch Products
RPMC offers a selection of Actively Q-Switched lasers at various levels of integration from OEM to turn-key, benchtop, laboratory and research laser systems. We group our active q-switch laser products into a few different categories, including Pulsed DPSS Lasers, Pulsed Fiber Lasers, Ultrafast Lasers, Tunable Lasers, and MIL-Spec. Lasers.
We provide many popular wavelength options, as well as non-standard wavelengths within the ultraviolet (UV), Violet, Blue, Green, Yellow, Red, near-infrared (NIR), short-wave infrared (SWIR), and mid-wave infrared (MWIR) spectral regions. Average output powers for these q-switched laser options range from a few 10s of mW (milliwatts) up to 150 W (watts), and pulse energy options ranging from a few nJ (nanojoules) up to around 200 mJ (millijoules).
On this page, you will find active q-switch lasers with pulse width options available from 125 ns down to 100 fs. A wide range of repetition rate options are available from single shot up to 80 MHz.
You can find Passive Q-Switch Lasers Here.
Our Active Q-Switch Laser Experience
RPMC Lasers is your preferred Active Q-Switch Laser Supplier, partnering with industry-leading and emerging manufacturers. We have been in business for over 25 years, providing researchers and OEM integrators with the best laser solution for their application. We have fielded 1000s of units for many different applications from micromachining to LIDAR and Bathymetry to medical applications such as tattoo removal and ablation-based surgical procedures.
Deeper Dive into Actively Q-Switched Lasers
Peak Power and Average Power in ns and Sub-ns Lasers:
Necessarily, the smoother leading and trailing edges of a Gaussian pulse slightly reduce (by a factor of 0.94) the peak power for given pulse energy or average power. The point is that the situation might be further complicated when lasers emitting few-nanosecond-long or sub-nanosecond (e.g., picosecond) pulses come into the picture. Usually, a Gaussian pulse shape is an excellent approximation for the real pulse profile of Q-switched DPSS lasers, even though it is accurate only for lasers operating in single longitudinal mode (SLM). Most commercially available Q-switched lasers rely on multiple longitudinal modes, oscillating at the same time with constant interference. This effect is visible by acquiring optical pulses with sufficiently fast photodiodes and digital oscilloscopes, showing an amplitude modulation superimposed to the Gaussian pulse shape.
The period and depth of the modulation depend on the number of longitudinal modes oscillating together. For tens-of-nanoseconds-long pulses, resonators support so many modes that the modulation is averaged out and hardly visible. Still, for sub-nanosecond operation, only a few modes are left, giving rise to deep modulation on the pulse envelope and strong deviation from the ideal Gaussian shape. A full-width half-maximum pulse duration definition becomes questionable, and a more refined statistical definition should be employed, giving rise to a correction factor for the peak power higher than 1 (potentially a factor of 1.5 could be a reasonable guess).
Read the full article here.
The Advantages and Disadvantages of Passive vs Active Q-Switching:
While there are a wide variety of q-switch technologies, notably including acousto-optic and electro-optic modulators, the technique as a whole can be broken down into two primary categories of q-switches, passive and active. Active q-switches rely on the ability of “flip a switch” and rapidly adjust the lasers cavity loss. A perfect example of this is an acousto-optic modulator, which, when activated creates a grating which deflects many spontaneously emitted photons out of the laser cavity, but once the modulator is turned off it allows the spontaneous photons to pass through and initiate stimulated emission. Passive q-switches, on the other hand, take advantage of a process known as saturable absorption. Saturable absorption derives from the fact that there is a limit to the amount of light that a material can physically absorb at a given wavelength before the energy level become saturated and the material becomes temporarily transparent. As a result, if a saturable absorbing material is placed inside of the laser cavity, it will absorb all of the spontaneously emitted photons until it reaches saturation where it will then allow the photons to pass through and initiate stimulated emission.
Both of these q-switching techniques produce short pulses and high peak powers, but they each have their pros and cons. For example, active q-switching allows the user far more control over when the pulse will be emitted and therefore how long population inversion will be allowed to build up. But, on the other hand many common active q-switches such as Pockels cells (which utilize the electro-optic effect) often require the driver to swing several kilovolts each time the switch is triggered. By contrast saturable absorbers require no drivers at all, meaning that not only are they compact, but they are also far less expensive. As a result, when you are deciding between an active versus passive q-switched laser there are four key things that you must keep in mind.
Read the full article here.
Why is a Low Jitter Feature Important in Actively Q-Switched DPSS Lasers?
In actively Q-switched lasers, the user controls the pulsed laser output, so that no laser pulse emission occurs without providing a proper input signal, aka “the trigger”. Due to the trigger signal propagation through the interface electronics, the Q-switch driver chain, and the laser resonator build-up time, a time delay (Td) is present between the externally supplied trigger signal and the actual laser pulse emitted by the laser source. The Td can show fluctuations if any electronics or optics involved in the pulse generation process have a functional variance in time.
The parameter Td is very relevant in the timing management of some applications. You must consider both the time delay (Td) and a time jitter (Tj), which is a statistical variation of the time delay depending mostly on:
- electrical noise in the trigger-chain
- pulse-to-pulse fluctuation of trigger-chain electrical parameters
- laser pulse build-up time-mechanism and associated fluctuations.
- fluctuation of rising (-falling) edge temporal profile of the trigger signal
Because of the jitter phenomena, the actual value of the time delay is statistically altered. Therefore, the laser pulse emission event happens (in the vast majority of cases) inside a normal time distribution, defined by an average time delay Td and a standard deviation value Tj (i.e 68.2 out of 100 pulses develop in the time interval Td ±Tj).
Read the full article here.
High-Energy Q-Switched Lasers for Harmonic Generation – Part 1
Solid-state lasers offer many advantages over other laser sources. One of their most unique benefits is the ability to produce extremely high pulse energy. Solid-state lasers can achieve this through q-switching, which is a process where the resonator losses are periodically increased, therefore interrupting the lasing process. Unlike other laser pulsing methodologies, q-switching is unique in that the pump source remains active while no lasing is occurring. Constant pumping forces the laser crystal to store the energy from the pump, similar to a capacitor. And just as with a capacitor in an electrical circuit, once you flip the switch and lasing can once again occur, the crystal will “discharge” all of the stored energy as fast as physically possible, resulting in an extremely high-energy laser pulse.
Read the full article here.
High-Energy Q-Switched Lasers for Harmonic Generation – Part 2
In our last blog post (Part 1), we highlighted the benefits of high-energy q-switched lasers for harmonic generation. In that article, we reviewed how q-switched lasers work and why the resultant short duration, high-energy pulses are required for higher-order harmonics. So, we won’t rehash that here. Instead, we will highlight another set of lasers offered here at RPMC, which are ideal for higher-order harmonic generation, allowing it to produce wavelengths from the infrared to the ultraviolet; the Sol, Wedge, and Onda from Bright Solutions. All three of these laser sources are robust and compact, making them ideal for integration into OEM systems. In this blog, we will highlight several of the features which make each unit uniquely suited for harmonic conversion.
Read the full article here.
Laser Requirements for Time Gated Active Night Vision Imaging Systems
That being said, in many active imaging systems, one is not merely interested in producing a two-dimensional image, but instead creating a three-dimensional “point cloud” of the environment. To produce such an image, the system must have a way of recording the round-trip time-of-flight (TOF) of the light. As a result, the camera and the illumination source must be pulsed, and the IR camera must be time-gated. This is remarkably similar to TOF lidar or TOF radar [4] with the exception that, instead of measuring the return signal with a single photodetector, the receiver is instead an infrared camera. While in theory this process could be done with an SLD, when you gain switch a diode source, the peak power of the laser is the same as in continuous operation, and as a result the pulse energy is typically rather low. By contrast, if a q-switched laser is used, short pulses can be generated with considerable peak powers. Since only a fraction of a percentage of the transmitted light from the IR illuminator will ever make it back into the imaging system, it is imperative that the pulse contains as much energy as possible to maximize the overall effacing.
Read the full article here.
LIDAR Becoming the Future of Bathymetry:
While liquid water does have significantly lower absorption at these shorter wavelengths, that is not the only factor that will determine the lasers ability to penetrate deep below the surface of the water; scattering is also a significant factor. Even if you measure crystal clear water, there will always be a certain amount of scattering associated with the Rayleigh effect. As a result, it is essential to use a laser with significant pulse energy, for enough photons to survive the round-trip flight back out of the body of water without scattering or being absorbed. Additionally, the laser must have as short a pulse width as possible since the depth resolution is directly proportional to the pulse width of the laser. A detailed explanation of this relationship is beyond the scope of this blog post, but it should be reasonably straightforward to understand that the lidar system cannot resolve TOF less than the width of the laser pulse itself.
With all of these factors taken into consideration, it isn’t a surprise that very few lasers possess the pulse width, pulse energy, form factor, and active q-switching required for bathymetric lidar.
Read the full article here.
Raman Spectroscopy: Why are Picosecond Pulses Superior to Femtosecond?
Raman-based spectroscopy, on the other hand, is an entirely different nonlinear technique, relying on the frequency shift experienced by laser radiation incident on a molecule, related to its rotational and vibrational modes. Not being related to electronic transitions, the Raman shift is relative concerning the irradiating wavelength, and therefore, unless pursuing coherent excitation, laser source tunability is not required. Raman-based spectroscopy, being a nonlinear process, usually requires ultrashort pulse generation (e.g., practical TPA set-ups usually require < 300 fs pulse duration). On the other hand, since the Raman gain is generally higher than TPA cross-sections, cheaper and simpler picosecond lasers could be efficiently employed in incoherent Raman spectroscopy. Furthermore, in Raman spectroscopy, the spectral resolution is related to the laser source bandwidth. Therefore, the narrower bandwidths of picosecond lasers represent a remarkable advantage over their femtosecond counterparts.
Read the full article here.
Let Us Help
With 1000s of fielded units, and over 25 years of experience, providing researchers with the best laser solution for their application, our expert team is ready to help! Working with RPMC ensures you are getting trusted advice from our knowledgeable and technical staff on a wide range of laser products. RPMC and our manufacturers are willing and able to provide custom solutions for your unique application.
If you have any questions, or if you would like some assistance please Contact Us here. Furthermore, you can email us at [email protected] to talk to a knowledgeable Product Manager.
Alternatively, use the filters on this page to assist in narrowing down the selection of actively q-switched lasers for sale. Finally, head to our Knowledge Center with our Lasers 101 page and Blogs, Whitepapers, and FAQ pages for further, in-depth reading.
Finally, check out our Limited Supply – In Stock – Buy Now page: This page contains an ever-changing assortment of various types of new lasers at marked-down/discount prices.
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The Aero Series is a high-energy, nanosecond pulsed DPSS laser, available at 266, 355, 532, and 1064nm, with up to 10W output power at 1064 (up to 200 mJ with water-cooling). This series provides unparalleled precision and accuracy in even the most challenging environments, ideal for LIBS, spectroscopy, and atmospheric LIDAR applications. All models come enclosed in an air-cooled, extremely compact and ruggedized, thermo-mechanically stable, low SWaP single unit platform, with options for air- or water-cooling, a range of add-ons, and even complete customization to fit your exact needs. Upon request, customized models undergo severe vibration and qualification tests for operation in space.
The Lampo Series is a line of compact ultrafast lasers that deliver megawatt-level ps laser pulses at a selectable PRR from 50 kHz to 40 MHz. Available in IR (1064 nm), SHG (532 nm), and Deep-UV (266 nm) versions (355nm by request), the series offers pulse durations < 70 ps and average power up to 20W, 10W, and 1.5W respectively. With pulse energy up to 250uJ, 150uJ, and 30uJ, these lasers are ideal for a wide range of scientific, industrial, defense, medical, biological, and LIDAR applications. Built into a rugged, air-cooled single-unit laser head, these lasers are easy to operate and integrate, making them a valuable tool for sophisticated laser systems and lab applications.
The Q-DOUBLE series is a DPSS, air-cooled, q-switched laser at 1064 or 1053 nm, designed to produce two pulses with variable temporal separation for PIV, LIBS, and other applications. The Q-DOUBLE can be configured for up to 160 mJ pulse energy @ 10 Hz or up to 40 mJ @ 100 Hz. The innovative laser design integrates all electronics (except power adapter) into the housing, resulting in a compact, user-friendly, turnkey, and air-cooled (water-free) system requiring little maintenance. User-friendly web-based GUI allows remote monitoring, control, and support from any computer or even a smartphone. Optional add-ons include built-in 2nd, 3rd, or 4th harmonic generator, built-in attenuator, energy monitor, and optional short cavity version.
The Q-TUNE-IR series is the perfect high peak power, coherent DPSS light source for researchers with infrared spectroscopy applications. This series uses an Optical Parametric Oscillator (OPO) to produce a tunable wavelength of 1380–4500nm (<10 cm-1 linewidth), achieving > 15mJ of pulse energy at the peak of the tuning curve. The Q-TUNE-IR requires little maintenance, with all laser electronics integrated into the housing, including an air-cooling system, eliminating the need for chillers or large power supplies while providing a guaranteed > 2 G shot pump diode lifetime.
