2010
DOI: 10.1103/physrevlett.104.083904
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Observing the Intrinsic Linewidth of a Quantum-Cascade Laser: Beyond the Schawlow-Townes Limit

Abstract: A comprehensive investigation of the frequency-noise spectral density of a free-running midinfrared quantum-cascade laser is presented for the first time. It provides direct evidence of the leveling of this noise down to a white-noise plateau, corresponding to an intrinsic linewidth of a few hundred hertz. The experiment is in agreement with the most recent theory on the fundamental mechanism of line broadening in quantum-cascade lasers, which provides a new insight into the Schawlow-Townes formula and predict… Show more

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Cited by 151 publications
(117 citation statements)
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“…The QCLs frequency noise was measured using a spectroscopic setup as implemented in former studies [7,[10][11][12]. The side of a molecular transition was used as a frequency-to-intensity converter (a so-called frequency Here, a 10-cm-long sealed glass cell filled with 2 mbar of pure N 2 O was used with QCLs emitting in the 7.6-8 μm wavelength range.…”
Section: Methodsmentioning
confidence: 99%
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“…The QCLs frequency noise was measured using a spectroscopic setup as implemented in former studies [7,[10][11][12]. The side of a molecular transition was used as a frequency-to-intensity converter (a so-called frequency Here, a 10-cm-long sealed glass cell filled with 2 mbar of pure N 2 O was used with QCLs emitting in the 7.6-8 μm wavelength range.…”
Section: Methodsmentioning
confidence: 99%
“…Novel applications of QCLs in very high-resolution spectroscopy and optical metrology have emerged in the last years, in particular in combination with optical frequency combs [2][3][4][5], which are generally more demanding in terms of low frequency-noise and nar-row spectral linewidth. QCLs have the potential to achieve very narrow linewidths with an intrinsic value of a few hundreds hertz only [6,7] resulting from their close-to-zero Henry's linewidth enhancement factor [8]. However, a narrow linewidth is generally not achieved in practice in freerunning QCLs as a result of the presence of undesired noise that compromises their spectral properties.…”
Section: Introductionmentioning
confidence: 99%
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“…2 shows the resulting frequency noise power spectral density (PSD) of the QCL. It has a 1/f trend at low frequency, followed by a steeper slope above ∼ 300 kHz, as observed in 21,22 . Note however that the measured frequency noise PSD is roughly one order of magnitude lower than previously published characterizations of free-running cw-mode near-RT DFB QCLs 20-24 .…”
mentioning
confidence: 72%
“…Optical frequency discriminators directly convert optical frequency fluctuations of the laser into intensity fluctuations that are detected by a photodetector. Optical discriminators are typically devices displaying a frequency-dependent transmission in a restricted frequency range, such as gas-filled cells near an atomic/molecular resonance (Doppler-broadened [10][11][12] or sub-Doppler 13 ), Fabry-Perot resonators 14 or unbalanced twobeam interferometers. 15 As it is not always possible to have a proper optical discriminator at the considered laser wavelength, another approach consists in heterodyning the laser under test with a second laser, either similar to the first one or with a negligible frequency noise, and subsequently analyzing the generated RF beat signal.…”
Section: Frequency Discriminatorsmentioning
confidence: 99%