1984
DOI: 10.1016/0030-4018(84)90016-6
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Deterministic chaos in laser with injected signal

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Cited by 244 publications
(109 citation statements)
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“…A classification of lasers due to Arecchi et al [ARE84] characterizes lasers by the order of magnitude of characteristic dynamic timescales of these three parts:…”
Section: Laser Dynamics -Relaxation Oscillationsmentioning
confidence: 99%
“…A classification of lasers due to Arecchi et al [ARE84] characterizes lasers by the order of magnitude of characteristic dynamic timescales of these three parts:…”
Section: Laser Dynamics -Relaxation Oscillationsmentioning
confidence: 99%
“…The dual-frequency laser, sustaining two orthogonal linear polarizations with a tunable frequency difference can perfectly fit the above mentioned applications. Such dual-frequency operation has been achieved for different solid-state lasers [6,7], but these lasers suffer from relatively strong intensity noise due to relaxation oscillations inherent to their class-B dynamical behavior [8]. The dual-frequency vertical-external-cavity surfaceemitting laser (DF-VECSEL) exhibits low noise due to its relaxation oscillation free class-A dynamical behavior, as the photon lifetime (∼10 ns) inside the cm-long external cavity is longer than the carriers' lifetime (∼3 ns) of the semiconductor gain medium.…”
Section: Introductionmentioning
confidence: 99%
“…In a Class A laser, the laser approaches the equilibrium exponentially like an overdamped oscillator while in a Class B laser it slowly oscillates back to its stable steady-state like an underdamped oscillator, and these are the aforementioned ROs. Class A lasers include Ar, He-Ne, and dye lasers while Class B lasers include most of the lasers used today such as CO 2 ; solid state and SLs. When subject to optical injection, Class A and Class B lasers exhibit quite different stability properties.…”
Section: Introductionmentioning
confidence: 99%