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Femtosecond second-order solitons in optical fiber transmission

dc.citation.epage336en_US
dc.citation.issue7en_US
dc.citation.spage331en_US
dc.citation.volume116en_US
dc.citation.woscount5
dc.contributor.authorChen, CFen_US
dc.contributor.authorChi, Sen_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.date.accessioned2014-12-08T15:37:05Z
dc.date.available2014-12-08T15:37:05Z
dc.date.issued2005en_US
dc.description.abstractA propagation of the femtosecond second-order solitons in an optical fiber is studied. We show that a generalized nonlinear Schrodinger equation well describes the propagation of the second-order soliton even containing only a few optical cycles. The propagations of a 50 fs and a 10 fs second-order soliton in an optical fiber are numerically simulated. It is found that, for the case of 10 fs second-order soliton, the soliton decay is dominated by the third-order dispersion, in contrast to the case of 50 fs second-order solitons, where the soliton decay is dominated by the delayed Raman response. It is also found that the exact delayed Raman response form must be used for the propagation of the 50 fs or less than 50 fs second-order soliton. (c) 2005 Elsevier GrnbH. All rights reserved.en_US
dc.identifier.doi10.1016/j.ijleo.2005.01.026en_US
dc.identifier.issn0030-4026en_US
dc.identifier.journalOPTIKen_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.ijleo.2005.01.026en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/25458
dc.identifier.wosnumberWOS:000231017300004
dc.language.isoen_USen_US
dc.subjectultrashort optical pulseen_US
dc.subjectoptical pulse propagationen_US
dc.subjectfemtosecond second-order solitonen_US
dc.subjectnonlinear effectsen_US
dc.subjectnonlinear Schrodinger equationen_US
dc.titleFemtosecond second-order solitons in optical fiber transmissionen_US
dc.typeArticleen_US

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