Distributed Feedback Lasers: 6000 nm - 14000 nm
nanoplus offers DFB quantum cascade lasers at any wavelength between 6000 nm and 14000 nm.
Key features of nanoplus distributed feedback quantum cascade lasers
- monomode
- pulsed operation
- room temperature
- tunable
- custom wavelengths
Why choose nanoplus distributed feedback quantum cascade lasers
- stable longitudinal and transversal single mode emission
- precise selection of target wavelength
- wavelength tunability
- small size
- long-term stability
For more than 20 years nanoplus has been the technology leader for lasers in gas sensing. We produce lasers at large scale at our own fabrication sites in Gerbrunn and Meiningen. nanoplus cooperates with the leading system integrators in the TDLAS based analyzer industry. More than 30,000 installations worldwide prove the reliability of nanoplus lasers.
Quick description of nanoplus distributed feedback laser technology
nanoplus uses a unique and patented technology for DFB laser manufacturing. We apply a lateral metal grating along the ridge waveguide, which is independent of the material system. Read more about our patented distributed feedback technology.
Related Information for nanoplus DFB quantum cascade lasers from 6000 nm to 14000 nm
Specifications
Mountings & Accessories
Applications
Papers & Links
The following table summarizes the typical DFB laser specifications in the 6000 nm to 14000 nm range:
| parameters (T = 25 °C) | symbol | unit | minimum | typical | maximum |
|---|---|---|---|---|---|
| wavelength precision | δ | nm | 0.1 | ||
| average output power | Pavg | mW | 1 | 3 | 20 |
| peak output power | Ppeak | mW | 10 | 100 | 1000 |
| pulsed operation current | If | mA | 1000 | 3600 | |
| pulsed threshold current | lth | mA | 500 | 2000 | |
| direct current tuning coefficient | CI | nm / mA | 0.05 | 0.2 | |
| temperature tuning coefficient | CT | nm / K | 0.45 @ 6 µm | 0.5 | 1.1 @ 14 µm |
| operating voltage | Vop | V | 10 | 15 | 20 |
| peak slope efficiency | e | mW / A | 200 | 500 | 800 |
| repetition frequency | f | kHz | 0.001 | 100 | 2000 |
| pulse length | t | ns | 2 | 100 | 3000 |
| duty cycle | d. c. | % | 0 | 3 | 10 |
| side mode suppression ratio | SMSR | dB | > 35 | ||
| slow axis (FWHM) | degrees | 20 | 25 | 30 | |
| fast axis (FWHM) | degrees | 50 | 60 | 70 | |
| storage temperature | TS | °C | -40 | 20 | 80 |
| operational temperature at case | TC | °C | -20 | +25 | +80 |
nanoplus distributed feedback lasers show outstanding spectral, tuning and electrical properties. They are demonstrated in figures 1 - 3. Click on the graphics to enlarge.
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If you are uncertain whether you require a distributed feedback laser, compare the specifications with our Fabry-Pérot lasers or contact us.
Free space mounting
The TO3 header is hermetically sealed with a cap and window.
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Accessories
Collimation for TO3 header offers collimated beam shape
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Application samples will follow soon.
For detailed absorption data, please refer to HITRAN database.
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Please find below a selection of related papers from our literature list.
Let us know if you published a paper with our lasers. We will be happy to include it in our literature list.
#9 DFB Lasers Between 760 nm and 16 µm for Sensing Applications;
W. Zeller, L. Naehle, P. Fuchs, F. Gerschuetz, L. Hildebrandt, J. Koeth, Sensors 2010, 10, pp. 2492-2510.
#11 Quantum cascade laser linewidth investigations for high resolution photoacoustic spectroscopy;
M. Germer, M. Wolff, Appl. Opt. 48, 4, 2009, pp. B80-B86.
#31 QCL based NO Detection;
M. Wolff, J. Koeth, L. Hildebrandt, P. Fuchs; 16th International Conference on Photoacoustic and Photothermal Phenomena.
#40 Comb-assisted spectroscopy of CO2 absorption profiles in the near- and mid-infrared regions;
A. Gambetta, D. Gatti, A. Castrillo, N. Coluccelli, G. Galzerano, P. Laporta, L. Gianfrani, M. Marangoni, Appl. Phys. B, 109, 3, Nov. 2012, pp. 385-390.
#49 Spectroscopic monitoring of NO traces in plants and human breath: applications and perspectives;
S. M. Cristescu, D. Marchenko, J. Mandon, K. Hebelstrup, G. W. Griffith, L. A. J. Mur, F. J. M. Harren, Appl. Phys. B, 109, 3, Nov. 2012, pp. 203-211.
#56 Widely tunable quantum cascade lasers with coupled cavities for gas detection;
P. Fuchs, J. Seufert, J. Koeth, J. Semmel, S. Hoefling, L. Worschech, A. Forchel, App. Phys. Lett., 97, 2010, 181111.
#57 Distributed feedback quantum cascade lasers at 13.8 µm on indium phosphide;
P. Fuchs, J. Semmel, J. Friedl, S. Hoefling, J. Koeth, L. Worschech, A. Forchel, Appl. Phys. Lett. 98, 2011, 211118.
#60 Single mode quantum cascade lasers with shallow-etched distributed Bragg reflector;
P. Fuchs, J. Friedl, S. Hoefling, J. Koeth, A. Forchel, L. Worschech, M. Kamp, Opt. Expr., 20, 4, 2012, pp. 3890-3897.
#80 Single-mode interband cascade lasers emitting below 2.8 μm;
J. Scheuermann, R. Weih, M. v. Edlinger, L. Nähle, M. Fischer, J. Koeth, M. Kamp, S. Höfling, Appl. Phys. Lett. 106, 2015, 161103.