
1.CNRS LTCI, Télécom ParisTech, Université Paris Saclay, 75634 Paris Cedex 13, France
2.mirSense, 86 rue de Paris, bat. Erable, 91400 Orsay, France
3.LMOPS (Laboratoire Matériaux Optiques, Photonique et Systèmes), CentraleSupélec, Université Paris Saclay, 57070 Metz, France
4.LMOPS (Laboratoire Matériaux Optiques, Photonique et Systèmes), CentraleSupélec, Université de Lorraine, 57070 Metz, France
5.Center for High Technology Materials, University of New-Mexico, Albuquerque, 87106-4343 NM, USA
M Sciamanna, Email: marc.sciamanna@centralesupelec.fr
F Grillot, Email: frederic.grillot@telecom-paristech.fr
Published:2016-09,
Published Online:29 January 2016,
Received:08 October 2015,
Revised:27 January 2016,
Accepted:27 January 2016
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Jumpertz, L. et al. Chaotic light at mid-infrared wavelength. Light: Science & Applications, 5, e16088 (2016).
Jumpertz, L. et al. Chaotic light at mid-infrared wavelength. Light: Science & Applications, 5, e16088 (2016). DOI: 10.1038/lsa.2016.88.
The onset of nonlinear dynamics and chaos is evidenced in a mid-infrared distributed feedback quantum cascade laser both in the temporal and frequency domains. As opposed to the commonly observed route to chaos in semiconductor lasers
which involves undamping of the laser relaxation oscillations
quantum cascade lasers first exhibit regular self-pulsation at the external cavity frequency before entering into a chaotic low-frequency fluctuation regime. The bifurcation sequence
similar to that already observed in class A gas lasers under optical feedback
results from the fast carrier relaxation dynamics occurring in quantum cascade lasers
as confirmed by numerical simulations. Such chaotic behavior can impact various practical applications including spectroscopy
which requires stable single-mode operation. It also allows the development of novel mid-infrared high-power chaotic light sources
thus enabling secure free-space high bit-rate optical communications based on chaos synchronization.
chaosnonlinear dynamicsoptical feedbackquantum cascade laser
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