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dc.contributor.authorJuang, Cen_US
dc.contributor.authorHwang, TMen_US
dc.contributor.authorJuang, Jen_US
dc.contributor.authorLin, WWen_US
dc.date.accessioned2014-12-08T15:45:45Z-
dc.date.available2014-12-08T15:45:45Z-
dc.date.issued2000-02-01en_US
dc.identifier.issn1041-1135en_US
dc.identifier.urihttp://dx.doi.org/10.1109/68.823509en_US
dc.identifier.urihttp://hdl.handle.net/11536/30778-
dc.description.abstractSynchronization between two identical chaotic systems (drive and response) with different initial conditions can be achieved provided that the conditional Lyapunov exponents are all negative. Adding an AM signal to the drive system, the two systems become asymptotically synchronized. The AM signal can be recovered by utilizing the property of the asymptotic synchronization. Chaotic AM noise is present as a direct result of the chaotic AM demodulation. Signal-to-chaotic-AM-noise ratio is calculated as a function of the signal amplitude.en_US
dc.language.isoen_USen_US
dc.subjectasymptotic synchronizationen_US
dc.subjectchaotic AM noiseen_US
dc.subjectoptical chaotic AIM demodulationen_US
dc.subjectself-pulsating laser diodesen_US
dc.titleOptical chaotic AM demodulation by asymptotic synchronizationen_US
dc.typeArticleen_US
dc.identifier.doi10.1109/68.823509en_US
dc.identifier.journalIEEE PHOTONICS TECHNOLOGY LETTERSen_US
dc.citation.volume12en_US
dc.citation.issue2en_US
dc.citation.spage179en_US
dc.citation.epage181en_US
dc.contributor.department應用數學系zh_TW
dc.contributor.departmentDepartment of Applied Mathematicsen_US
dc.identifier.wosnumberWOS:000085414500027-
dc.citation.woscount2-
Appears in Collections:Articles


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