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Perturbed Manakov-Stackel system

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dc.contributor.author Hizanidis, K en
dc.contributor.author Frantzeskakis, DJ en
dc.contributor.author Polymilis, C en
dc.date.accessioned 2014-03-01T02:41:17Z
dc.date.available 2014-03-01T02:41:17Z
dc.date.issued 1996 en
dc.identifier.uri http://hdl.handle.net/123456789/30443
dc.subject.other Asymptotic stability en
dc.subject.other Light modulation en
dc.subject.other Light polarization en
dc.subject.other Light transmission en
dc.subject.other Nonlinear equations en
dc.subject.other Nonlinear optics en
dc.subject.other Optical communication en
dc.subject.other Parameter estimation en
dc.subject.other Perturbation techniques en
dc.subject.other Stochastic control systems en
dc.subject.other Waveguide couplers en
dc.subject.other Abstract only en
dc.subject.other Coupling coefficients en
dc.subject.other Perturbed Manakov-Stackel system en
dc.subject.other Optical fiber coupling en
dc.title Perturbed Manakov-Stackel system en
heal.type conferenceItem en
heal.identifier.primary 10.1109/AEM.1996.873152 en
heal.identifier.secondary http://dx.doi.org/10.1109/AEM.1996.873152 en
heal.publicationDate 1996 en
heal.abstract Nonlinear optical systems are dependent on the value of the coupling coefficient σ. For σ>>1, the system models the dynamics of the interaction of two modes in nonlinear optical fibers or in directional couplers with weak intermodal coupling in the high intensity limit. The value σ = 1 which is the Manakov case, corresponds to two cases; a purely electrostrictive nonlinearity and the elliptical birefringence. A wide class of travelling wave solutions is found to posses a Stackel potential character exhibiting two integrals of motion. Manakov case is used as the unperturbed reference state in a perturbative scheme for σ≠1. Stochasticity accompanies the solitary-type envelope solutions to the perturbed Manakov system. en
heal.publisher IEEE en
heal.journalName Trans Black Sea Region Symposium on Applied Electromagnetism en
dc.identifier.doi 10.1109/AEM.1996.873152 en


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