2008
DOI: 10.1109/jlt.2008.922212
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Nonlinear State–Space Model of Semiconductor Optical Amplifiers With Gain Compression for System Design and Analysis

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Cited by 24 publications
(13 citation statements)
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“…In the past, models without spatial resolution have been employed for the description of semiconductor amplifiers [BER03b,KUN08,ERN09a,KIM09a]. As soon as strong spatial inhomogeneities arise, such models are, however, bound to fail.…”
Section: Quantum-dot Semiconductor Optical Amplifier Modelmentioning
confidence: 99%
“…In the past, models without spatial resolution have been employed for the description of semiconductor amplifiers [BER03b,KUN08,ERN09a,KIM09a]. As soon as strong spatial inhomogeneities arise, such models are, however, bound to fail.…”
Section: Quantum-dot Semiconductor Optical Amplifier Modelmentioning
confidence: 99%
“…The SOA is modeled as a traveling wave amplifier [12,13]. In the amplifier the saturation effect and phase change is due to time dependent gain and refractive index coupling respectively.…”
Section: Theoretical Analysismentioning
confidence: 99%
“…It has been previously demonstrated that the SOA can be treated through lumped, input/output element modelling, by averaging the longitudinal carrier density distributions to a single, time dependent output value [6][7][8]. This assumption holds under conditions that the SOA photon transient time is much shorter than the time scale of modulated carrier density variations, and much longer than the SOA propagation delay [7,8].…”
Section: Introductionmentioning
confidence: 99%
“…This assumption holds under conditions that the SOA photon transient time is much shorter than the time scale of modulated carrier density variations, and much longer than the SOA propagation delay [7,8]. Considering the typical values of optical transient times (100 ps À 1 ns) and active region lengths (400 μm-800 μm) in RSOA, and today's typical applications for up to 10 Gb/s transmission by using direct RSOA signal modulation, we assume the carrier density ℵ to be constant over the RSOA active region length, ℵðz; tÞ ¼ ℵðtÞ [7]. Thus, the partial differential equations governing the photon and carrier densities can be approximated by first order nonlinear ordinary differential equations [7].…”
Section: Introductionmentioning
confidence: 99%
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