The emission linewidth is usually rather small – which is often very useful for applications in spectroscopy. A contributing factor for that is the small linewidth enhancement factor.

An example for a military application is the use for infrared countermeasures, i.e., irritating heat-seeking missiles attacking airplanes by sending mid-infrared light to their sensors.

Although both types of devices contain a sequence of thin layers of different semiconductor materials, they have very different principles of operation:

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Sacher Lasertechnik offers quantum cascade lasers with emission between 4 μm and 12 μm, suitable for applications like molecular spectroscopy.

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Perhaps the most important applications for quantum cascade lasers will be in the area of laser absorption spectroscopy of trace gases, e.g. for detecting very small concentrations of pollutants in air. In addition to the suitable wavelength range, QCLs usually feature a relatively narrow linewidth and good wavelength tunability, making them very suitable for such applications.

The function of the quantum wells is vital for the operation of such a laser. That means they definitely need to be embedded into regions with higher electron energy; without those regions, you would not have any quantum wells and there's an entirely different electronic structure. Therefore, the only way is to use tunneling for the injection of carriers from one quantum well into the other.

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Serving North America, RPMC Lasers offers a range of high-performance quantum cascade lasers. The PowerMir line emits in the main transmission bands of the atmosphere (4.0 µm, 4.6 µm, 4.8 µm, 9.x µm). Furthermore, the new line of UniMir Distributed Feedback (DFB) QCLs emit in the LWIR spectral region (11.3, 13.4 & 14 µm). The PowerMir line are Fabry–Pérot laser sources operating in the quasi CW regime. In other words, pulsed operation down to few tens of nanoseconds and high frequency above MHz at room temperature. The UniMir line are DFB sources with CW operation. These products exhibit high average power and wall-plug efficiency. Therefore, perfect for counter-measure and other defense applications, as well as gas detection in the nuclear and petrochemical industries.

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Frankfurt Laser Company offers quantum cascade laser diodes with emission wavelengths from 4 μm to 13 μm with either DFB or Fabry–Pérot type.

Terahertz quantum cascade lasers are also interesting for various imaging applications. See the article on terahertz radiation.

The carrier lifetime in quantum cascade lasers is much shorter than in ordinary laser diodes, for example; it is limited by phonon scattering phenomena. That also has consequences for the dynamic properties: there is very strong damping of relaxation oscillations (overdamped transient dynamics). For that reason, quantum cascade lasers can be modulated with very high intrinsic bandwidth limited of several tens of gigahertz.

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The power conversion efficiency of quantum cascade lasers is typically of the order of a few tens of percent. Recently, however, devices with efficiencies around 50% have been demonstrated [10, 11], although only for cryogenic operation conditions.

The diagram shows the electron energy versus position in the structure, which contains three quantum wells. The overall downward trend of energy towards the right-hand side is caused by an applied electric field. In reality, each gain region must be divided into an active region and an injector.

Alpes Lasers designs and manufactures a wide range of QCLs with wavelengths from 4 to 14 μm and powers up to hundreds of milliwatts. This includes FP, DFB, THz, frequency comb and external cavity lasers in the mid-IR. Additionally, Alpes offers uniquely fast and widely tuneable lasers with our ET and XT product line.

Whereas continuously operating room-temperature devices [4] are normally limited to moderate output power levels in the milliwatt region (although more than a watt is possible), multiple watts are easily possible with liquid-nitrogen cooling. Even at room temperature, watt-level peak powers are possible when using short pump pulses.

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Another application field of THz QCLs is free-space communications. Although terahertz beams exhibit substantially stronger beam divergence than optical beams, one can still use directed beams for short-distance transmission through air.

Most quantum cascade lasers emit mid-infrared light (which means wavelengths between 3 μm and 50 μm according to ISO 20473:2007) – they are thus a kind of mid-infrared laser sources. However, quantum cascade lasers can also be made for generating terahertz waves (→ terahertz sources). Such devices constitute particularly compact and simple (electrically pumped) sources of terahertz radiation. Even room temperature terahertz generation can been achieved via internal difference frequency generation [12].

The quantum cascade laser is a special kind of semiconductor laser, usually emitting mid-infrared light. Such a laser operates on laser transitions not between different electronic bands but on intersubband transitions of a semiconductor structure. Figure 1 shows what happens to an electron injected into the gain region: in each period of the structure, it undergoes a first transition (blue arrow) between two sublevels (minibands) of a quantum well (which is the laser transition on which stimulated emission occurs), then a non-radiative transition (red arrow) to the lowest sublevel, before tunneling (gray arrow) into the upper level of the next quantum well. By using several tens or even 100 quantum wells in a series (a cascade), a higher optical gain and multiple photons per electron are obtained at the expense of a higher required electrical voltage. The operation voltage can easily be of the order of 10 V, whereas few volts are sufficient for ordinary laser diodes.

As the transition energies are defined not by fixed material properties but rather by design parameters (particularly by layer thickness values of quantum wells), quantum cascade lasers can be designed for operating wavelengths ranging from a few microns to well above 10 μm, or even in the terahertz region. Note that a single injected carrier can generate (in the ideal case of perfect quantum efficiency) one photon for each quantum well region.

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In a quantum cascade laser, the mentioned quantum well structure is embedded in a waveguide, and the laser resonator is mostly of DBR or DFB type. There are also external-cavity lasers, where a wavelength tuning element such as a diffraction grating is part of the resonator.

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Definition: semiconductor lasers relying on intersubband transitions, normally emitting in the mid-infrared spectral region