2009
DOI: 10.1063/1.3089570
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Measurement of gain and losses of a midinfrared quantum cascade laser by wavelength chirping spectroscopy

Abstract: We present an optimized technique for the measurement of gain and losses of semiconductor lasers. We optically inject the beam of a distributed feedback laser (DFB) inside the cavity of the lasers under study. The DFB laser operates in a pulsed mode and shifts its emission wavelength as a function of time. This frequency chirp creates the Fabry–Pérot fringes of the transmitted intensity that contains all the information on the cavity losses. The setup has been validated by a quantitative study of the losses as… Show more

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Cited by 14 publications
(5 citation statements)
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“…For the threshold wavelength, on the other hand, an intermediate state between both laser transitions (l min m l max ) occurs, which is then dominated by the designed resonance emission with increasing current. In addition, this shift of states in alignment was also observed in the current dependence of gain coefficient, which confirms this theory [6,7].…”
Section: Resultssupporting
confidence: 75%
“…For the threshold wavelength, on the other hand, an intermediate state between both laser transitions (l min m l max ) occurs, which is then dominated by the designed resonance emission with increasing current. In addition, this shift of states in alignment was also observed in the current dependence of gain coefficient, which confirms this theory [6,7].…”
Section: Resultssupporting
confidence: 75%
“…A highlight is the realization and continuous improvement of Quantum Cascade Lasers (QCL) [2][3][4][5] that emit in this frequency range. The search for improved performances of QCLs includes a better design of the layer sequence to enhance the population inversion between the two subbands involved in the lasing transition, the decrease of the non radiative paths, but also the control of the photon re-absorption by the free carriers that are present in the structure [6][7][8][9][10][11][12] . The free carrier absorption (FCA), well known from bulk structures, is transferred to a variety of intra-subband and inter-subband oblique (in two-dimensional k space) transitions in heterostructures 13,14 .…”
mentioning
confidence: 99%
“…[4][5][6][7][8] Among the possible reasons for the degradation of performance are the depopulation of the upper levels (nonradiative escape) and the reabsorption of the laser photons, which is a widely studied topic. [9][10][11][12][13] The reabsorption is unavoidable because of the free carriers, in particular those that occupy the upper subband of the lasing transition. The free-carrier absorption (FCA) is well documented in bulk material where a quantum mechanical calculation 14 leads to a free-carrier absorption coefficient that closely resembles the semiclassical Drude result.…”
Section: Introductionmentioning
confidence: 99%