2003
DOI: 10.1109/jlt.2003.809575
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Performance characterization of high-bit-rate optical chaotic communication systems in a back-to-back configuration

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Cited by 42 publications
(19 citation statements)
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“…The model used in simulation can be described by known Lang-Kobayashi equation as Eqs. (1)-(5) [1,6,8,14] , where ( , , )…”
Section: Theory and Modelmentioning
confidence: 99%
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“…The model used in simulation can be described by known Lang-Kobayashi equation as Eqs. (1)-(5) [1,6,8,14] , where ( , , )…”
Section: Theory and Modelmentioning
confidence: 99%
“…In close-loop configuration, the semiconductor lasers in transmitter and receiver are identical and both are subjected to external-cavity optical feedback. In open-loop configuration, the laser in transmitter is subjected to external-cavity feedback, while the laser in receiver is only a single diode similar to that in transmitter [6][7][8] . Meanwhile, the synchronization mechanisms in the two kinds of configuration are different.…”
mentioning
confidence: 99%
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“…A semiconductor laser can be driven to a chaotic regime operation by applying optical feedback [4][5][6] , optoelectronic feedback 10,11 and optical injection 12 . Several approaches have been proposed for the encryption of the message upon a chaotic carrier: The performance of chaotic masking (CMS), chaotic modulation (CM), chaos shift keying (CSK), on/off phase shift keying (OOPSK) and chaos shift keying in a wavelength chaos configuration [13][14][15][16] have been tested both numerically 14,17 and experimentally 18 . The philosophy of the decoding process however is always the same, based on a very good synchronization between the transmitter and the receiver system.…”
Section: Introductionmentioning
confidence: 99%