uniMIR

A wavelength range from 10 to 19 µm (corresponding to 1000 to 526 cm-1) can be covered by mirSense’s uniMIR DFB-QCL (Distributed Feedback Quantum Cascade Laser). Together with the University of Montpellier, mirSense holds the exclusive license to manufacture lasers in this wavelength range. In 2021, mirSense was a finalist in the “smart sensing” category at the Prism Awards at Photonics West with its uniMIR lasers and a wavelength range of 10 to 17 µm.

What makes these lasers special is their wide wavelength range from 10 to 19 µm, which opens up new areas of research. Narrow linewidths with high sensitivity are also possible. Continuous wave (CW) mode can be achieved for wavelengths up to 17.7 µm with output powers in the milliwatt range.
In continuous wave mode, the tuning range is typically 2 cm-1 with a narrow linewidth of <100 MHz (<0.003 cm-1). However, if higher wavelengths above 18 µm are required, the laser can only be operated in pulse mode. This provides a larger tuning range and higher operating temperature.
The long-wave uniMIR lasers have a very low spectral chirp during the pulse, typically <0.04 cm-1 / 100 ns. This enables intrapulse spectroscopy without high-speed detectors or quasi-continuous wave spectroscopy (QCW) without deterioration of the spectral resolution (up to 0.01 cm-1) – using mirSense electronics for pulsed operation. The uniMIR laser chips are mounted on a thermoelectric controller (TEC) to ensure a constant temperature of the laser chip. By changing the temperature, the emission wavelengths can be adjusted without mode jumping, while maintaining single-mode operation. The laser chip and its electronics are housed in a sealed enclosure, known as HHL (high heat load), with an integrated collimating lens and thermistor for reading the laser chip temperature. If a larger tuning range is required, pulsed operation is possible. When using pulsed operation, power consumption is low, operation at higher temperatures is possible, and access to a larger tuning range and larger wavelengths is possible.

What are DFB QCLs?

Distributed feedback quantum cascade lasers have an integrated grating—known as a Bragg grating—in the laser cavity, which selects a single mode. They are therefore single longitudinal mode narrow-band lasers. Quantum cascade lasers generally emit in the mid-infrared range. What makes them special is that

  • the cascade-like structure causes the electron to migrate through the structure (no electron-hole recombination),
  • the electron is recycled
  • and thus one electron can excite several electrons.

The QCL consists of an active/gain stage (where inversion population takes place) and an injection/relaxation stage (where electrons are recycled), which are repeated several times.
There are also Fabry-Pérot cavities (see powerMIR). External cavity QCLs (EC-QCLs) are not part of the mirSense portfolio.

Why is it interesting to use a wavelength range up to 19 µm?

A further wavelength range of more than 11 µm (lower than 909 cm-1) enables strong vibration spectra of small hydrocarbons such as ethene, acetylene, or propane, spectroscopy on the so-called BTEX molecules (benzene, toluene, ethylbenzene, and xylenes), or to detect nitrogen oxide. This low wavenumber range, which is covered exclusively by mirSense, also enables new applications in astrophysics, geosciences, quantum technology, measurement technology, and fundamental physics.

Scope of application

The following table shows some wavelengths and their applications:

Application familyWavelengthMeasurable speciesQCL product datasheet when available
OH Hydroxyl radical spectroscopy~18.8 µm~531 cm-1Hydroxyl radical (OH)UN0530Q003HNA
Fundamental science~ 17.7 µm~ 565 cm-1UN0565C002HNA
Carbon emissions~ 15 µmCarbon dioxide (CO2)
Fluoro~ 10.5 µm~ 948 cm-1Sulfur hexafluoride (SF6)
VOC~ 13.7 µm~ 729 cm-1TolueneUN0746C005HNA
VOC~ 14.4 µm~ 694 cm-1Toluene
VOC~ 14.3 µm~ 697 cm-1Ethylbenzene
VOC~ 13 µm~ 769 cm-1m-XyleneUN0746C005HNA
VOC~ 12.6 µm~ 795 cm-1p-XyleneUN0746C005HNA
VOC~ 13.5 µm~ 741 cm-1o-XyleneUN0746C005HNA
Nitrogen~ 10.7 µm~ 930 cm-1Ammonia (NH3)
Nitrogen~ 17.2 µm~ 581 cm-1Nitrous Oxide (N2O)
Nitrogen~ 10.6 µm~ 941 cm-1Hydrazine (N2H4)
Nuclear~ 11.3 µm~ 885 cm-1Methyl Iodid (CH3I)UN0885C010HNA
Toxic~ 11.8 µm~ 850 cm-1Phosgene (COCl2)
Toxic~ 14 µm~ 713 cm-1Hygrogen Cyanide (HCN)UN0713C005HNA

Specifications
General Information
Laser typeQCL single mode Distributed Feedback lasers (DFB) (1)
Mode of operationCW or pulsed
Typical Optical Power5-10mW typical for wavelength under 15 microns
1-5mW typical for wavelength above 15 microns
Up to 20mW with a Fabry-Pérot laser (1)
Full accessible wavelength range~3 cm-1 typically
Continuous tuning range>1 cm-1 typically
Side mode suppression ratioSMSR > 25 dB
Linewidth (FWHM)< 100 Mhz (free-running with suitable electronics for CW lasers)
Divergence< 10mrad
Beam qualityTM00
Output beam diameter (window output)Typically 4 mm
PolarizationLinear vertically polarized
(1) : Fabry-Pérot lasers are also available. They offer larger output power (up to 20 mW), with broader emission spectrum.
Example for DFB lasersSingle Mode DFB QCL
885 cm-1 = 11µm
Single Mode DFB QCL
746 cm-1 = 13µm
Single Mode DFB QCL
713 cm-1 = 14µm
ApplicationMethyliodid CH3IXylene & Propane C8H10 C3H8
Hydrogen Cyanide (HCN)
Laser typeQCL single mode DFBQCL single mode DFBQCL single mode DFB
Mode of operationCWCWCW
Guaranteed minium optical power at 885 cm-110 mW (with the base plate of the HHL-package at +20°C)5 mW (with the base plate of the HHL-package at +20°C)6 mW (with the base plate of the HHL-package at +20°C)
Full accessible wavelength range>3cm-1~ 3cm-1~ 3cm-1
Continuous tuning range> 1 cm-1> 0.5 cm-1> 1 cm-1
Side mode suppression ratioSMSR > 25 dBSMSR > 25 dBSMSR > 25 dB
Linewidth (FWHM)< 100 Mhz (free-running with suitable electronics)< 100 Mhz (free-running with suitable electronics)< 100 Mhz (free-running with suitable electronics)
Divergence< 10mrad< 10mrad< 10mrad
Beam qualityTM00TM00TM00
Output beam diameter
(window output)
Typically 4 mmTypically 4 mmTypically 4 mm
PolarizationLinear vertically polarizedLinear vertically polarizedLinear vertically polarized