2018
DOI: 10.1364/ol.43.000210
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Comparison of optical feedback dynamics of InAs/GaAs quantum-dot lasers emitting solely on ground or excited states

Abstract: We experimentally compare the dynamics of InAs/GaAs quantum dot lasers under optical feedback emitting exclusively on ground states (GSs) or excited states (ESs). By varying the feedback parameters and putting focus either on their short or long cavity regions, various periodic and chaotic oscillatory states are found. The GS laser is shown to be more resistant to feedback, benefiting from its strong relaxation oscillation damping. In contrast, the ES laser can easily be driven into complex dynamics. While the… Show more

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Cited by 22 publications
(8 citation statements)
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“…In what follows, the r ext,p extracted from short-to long-cavity region of the undoped QD laser is shown in Figure 5. Extending the L ext from 5 cm to 50 cm, which corresponds to a ratio f RO /f ext ranging from 0.83 to 8.3, the boundaries of the periodic oscillation of the undoped laser show some residual undulations in the short-cavity region, which results from the interferences between the internal and external cavity modes; 28,29 whereas in the long-cavity region, the r ext,p keeps decreasing until it progressively becomes rather independent of L ext . Let us stress that whatever the L ext is, both the p-doped and undoped devices exhibit high tolerance for external reflection without showing any chaotic pulsations up to ∼ 20%.…”
Section: Resultsmentioning
confidence: 99%
“…In what follows, the r ext,p extracted from short-to long-cavity region of the undoped QD laser is shown in Figure 5. Extending the L ext from 5 cm to 50 cm, which corresponds to a ratio f RO /f ext ranging from 0.83 to 8.3, the boundaries of the periodic oscillation of the undoped laser show some residual undulations in the short-cavity region, which results from the interferences between the internal and external cavity modes; 28,29 whereas in the long-cavity region, the r ext,p keeps decreasing until it progressively becomes rather independent of L ext . Let us stress that whatever the L ext is, both the p-doped and undoped devices exhibit high tolerance for external reflection without showing any chaotic pulsations up to ∼ 20%.…”
Section: Resultsmentioning
confidence: 99%
“…Further increase of the external cavity length to the long cavity regime leads to frequency-locking regimes as reported elsewhere. 13 Experimental results reveal that the GS laser is perfectly stable such that no chaotic state was found whatever the feedback strength level used in this setup. Besides, the GS laser remains under the steady-state condition providing the feedback strength does not exceed 30% which is already much larger compared to any typical reflection levels taking place in a transmission system 13 .…”
Section: Laser Structure and Experimental Setupmentioning
confidence: 87%
“…For the QW FP laser, even under a weak EOF of −37 dB, multiple frequency noise peaks already exist in the RIN diagram in Figure 5B. The periodic peaks could be the high-order harmonics of the fundamental RO frequency, which are caused by the intracavity resonance, and thus the coherence collapse follows in the RF spectrum and RIN diagram (Lin et al, 2018). With increasing EOF levels, the noise level continuously grows, which leads to significant optical spectral broadening in Figures 3B,E.…”
Section: Relative Intensity Noise Measurementsmentioning
confidence: 98%