Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/5641
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dc.contributorDepartment of Electrical Engineering-
dc.creatorLiu, Z-
dc.creatorHe, X-
dc.creatorWang, D-
dc.date.accessioned2014-12-11T08:25:49Z-
dc.date.available2014-12-11T08:25:49Z-
dc.identifier.issn0146-9592-
dc.identifier.urihttp://hdl.handle.net/10397/5641-
dc.language.isoenen_US
dc.publisherOptical Society of Americaen_US
dc.rights© 2011 Optical Society of America. This paper was published in Optics Letters and is made available as an electronic reprint with the permission of OSA. The paper can be found at the following URL on the OSA website: http://www.opticsinfobase.org/ol/abstract.cfm?uri=ol-36-16-3024. Systematic or multiple reproduction or distribution to multiple locations via electronic or other means is prohibited and is subject to penalties under law.en_US
dc.subjectCrystal whiskersen_US
dc.subjectErbiumen_US
dc.subjectFiber lasersen_US
dc.subjectFibersen_US
dc.subjectGrapheneen_US
dc.subjectHoley fibersen_US
dc.subjectOptical fiber fabricationen_US
dc.subjectOptical fibersen_US
dc.subjectPhotonic crystalsen_US
dc.subjectPulse repetition rateen_US
dc.titlePassively mode-locked fiber laser based on a hollow-core photonic crystal fiber filled with few-layered graphene oxide solutionen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Zhi-Bo Liuen_US
dc.description.otherinformationAuthor name used in this publication: D. N. Wangen_US
dc.identifier.spage3024-
dc.identifier.epage3026-
dc.identifier.volume36-
dc.identifier.issue16-
dc.identifier.doi10.1364/OL.36.003024-
dcterms.abstractWe demonstrate a nanosecond-pulse erbium-doped fiber laser that is passively mode locked by a hollow-core photonic crystal fiber filled with few-layered graphene oxide solution. Owing to the good solution processing capability of few-layered graphene oxide, which can be filled into the core of a hollow-core photonic crystal fiber through a selective hole filling process, a graphene saturable absorber can be successfully fabricated. The output pulses obtained have a center wavelength, pulse width, and repetition rate of 1561:2nm, 4:85 ns, and 7:68MHz, respectively. This method provides a simple and efficient approach to integrate the graphene into the optical fiber system.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationOptics letters, 15 Aug. 2011, v. 36, no. 16, p. 3024-3026-
dcterms.isPartOfOptics letters-
dcterms.issued2011-08-15-
dc.identifier.isiWOS:000293890800003-
dc.identifier.scopus2-s2.0-80051739665-
dc.identifier.pmid21847147-
dc.identifier.eissn1539-4794-
dc.identifier.rosgroupidr59594-
dc.description.ros2011-2012 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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