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dc.contributor.authorTeğin, Uğuren_US
dc.contributor.authorElahi, Parvizen_US
dc.contributor.authorŞenel, Ç.en_US
dc.contributor.authorErgeçen, Emreen_US
dc.contributor.authorİlday, F. Ömeren_US
dc.coverage.spatialMunich, Germanyen_US
dc.date.accessioned2020-01-30T12:00:41Z
dc.date.available2020-01-30T12:00:41Z
dc.date.issued2015
dc.identifier.isbn9781467374750
dc.identifier.urihttp://hdl.handle.net/11693/52933
dc.descriptionDate of Conference: 21–25 June 2015en_US
dc.descriptionConference Name: 2015 European Conference on Lasers and Electro-Optics - European Quantum Electronics Conferenceen_US
dc.description.abstractStolen, et al. introduced synchronously pumped oscillators where gain was achieved through stimulated Raman scattering (SRS) as a method to reach wavelengths outside of the limited range covered by laser gain media [1]. Raman lasers are thus pumped by another laser source and generate a frequency-shifted Stokes (or anti Stokes) wave. Raman solitons which are generated by this technique typically require km-long cavities, require anomalous-dispersion fibers and are limited to low pulse energies [2]. Self-similarly evolving parabolic pulses have also been generated, but required km-long fibers and achieved 6 ps duration [3]. Here, we present a new type of Raman oscillator, which supports dissipative solitons, does not require anomalous dispersion and a km-long cavity.en_US
dc.language.isoEnglishen_US
dc.source.titleThe European Conference on Lasers and Electro-Optics 2015en_US
dc.titleDissipative solitons generated from a mode-locked Raman laseren_US
dc.typeConference Paperen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.citation.spageCJ_2_6en_US
dc.publisherIEEEen_US
dc.contributor.bilkentauthorTeğin, Uğur
dc.contributor.bilkentauthorElahi, Parviz
dc.contributor.bilkentauthorErgeçen, Emre
dc.contributor.bilkentauthorİlday, F. Ömer


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