1980
DOI: 10.1109/jqe.1980.1070479
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External optical feedback effects on semiconductor injection laser properties

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Cited by 2,593 publications
(1,292 citation statements)
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“…The emergence of chaotic fluctuations in mW SCLs with timedelayed feedback is well described by deterministic rate equations, the Lang-Kobayashi equations 30 . However, for sub µW lasers, there are two additional sources of fluctuations preventing a possible mathematical description by rate equations.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The emergence of chaotic fluctuations in mW SCLs with timedelayed feedback is well described by deterministic rate equations, the Lang-Kobayashi equations 30 . However, for sub µW lasers, there are two additional sources of fluctuations preventing a possible mathematical description by rate equations.…”
Section: Discussionmentioning
confidence: 99%
“…The second source is the low number of QDs (~10) being effectively involved in the lasing operation 10 . The robustness of the chaotic lasing phenomenon, with respect to quantum noise where a description by rate equations 30 is inconsistent, is of great interest from the point of view of nonlinear dynamics 31,32 . Our results give first insight into the chaotic behaviour of microlasers with self-feedback and have high potential to stimulate further experimental and theoretical studies.…”
Section: Discussionmentioning
confidence: 99%
“…The phenomenon was first characterized by Lang and Kobayashi [16], who analysed the effects of external optical feedback in a laser diode (LD) by means of the delayed differential equations of involved electric field. Later models, such as the one presented by Wang [17] (Fig.1), use an equivalent two cavity Fabry-Perot (FP) scheme that also results in the well known phase equation [18]:…”
Section: Self-mixing Interferometrymentioning
confidence: 99%
“…The delayed feedback due to the presence of an external cavity is characterized by: (i) the time delayτ = 2L/c which is the round-trip time in the external cavity, where c is the speed of light and L is the length of the external cavity; (ii) the feedback strengthη = R(1 − R 2 F )/(T R F ) proportional to the reflectivity of the external mirror R and inversely proportional to the Fabry-Perot round trip time T , R F is the reflectivity of the laser cavity facets; and (iii) the phase φ = ω eτ where ω e is the frequency of the injected signal. We adopt the Lang-Kobayashi approach to model the delayed feedback [65]. This approach is based on two approximations: a single longitudinal mode operation and the reflected field is sufficiently attenuated that it can be modeled by a single delay term.…”
Section: Passive Nonlinear Cavity With Delayed Feedbackmentioning
confidence: 99%