Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/94514
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dc.contributorDepartment of Electrical Engineeringen_US
dc.creatorQi, Yen_US
dc.creatorJin, Wen_US
dc.creatorHo, HLen_US
dc.date.accessioned2022-08-25T01:53:16Z-
dc.date.available2022-08-25T01:53:16Z-
dc.identifier.issn0146-9592en_US
dc.identifier.urihttp://hdl.handle.net/10397/94514-
dc.language.isoenen_US
dc.publisherOptical Society of Americaen_US
dc.rights©2021 Optical Society of Americaen_US
dc.rights© 2021 Optica Publishing Group. One print or electronic copy may be made for personal use only. Systematic reproduction and distribution, duplication of any material in this paper for a fee or for commercial purposes, or modifications of the content of this paper are prohibited.en_US
dc.rightsThe following publication Yun Qi, Wei Jin, and Hoi Lut Ho, "Tunable pulse advancement and delay by frequency-chirped stimulated Raman gain with optical nanofiber," Opt. Lett. 46, 178-181 (2021) is available at https://doi.org/10.1364/OL.409127.en_US
dc.titleTunable pulse advancement and delay by frequency-chirped stimulated Raman gain with optical nanofiberen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage178en_US
dc.identifier.epage181en_US
dc.identifier.volume46en_US
dc.identifier.issue2en_US
dc.identifier.doi10.1364/OL.409127en_US
dcterms.abstractWe demonstrate a novel method to optically tune the pulse advancement and delay based on stimulated Raman gain in hydrogen. With a frequency-chirped pump, the generated signal pulse is selectively amplified at the leading or trailing edge of the pump pulse, depending on whether the frequency difference between the pump and the signal beam is blue or red detuned from the Raman transition, which results in advancement or delay of the signal peak. Different from the method of slow/fast light, where advancement and delay are accompanied with power loss and gain, respectively, for a single resonance, both the advancement and delay are realized in the gain region for the method here. With a piece of 48-mm-long optical nanofiber in hydrogen, the time-shift for a signal peak ranging from 3.7 to −3.7 ns is achieved in a Raman-generated pulse with width of ∼12 ns.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationOptics letters, 15 Jan. 2021, v. 46, no. 2, p. 178-181en_US
dcterms.isPartOfOptics lettersen_US
dcterms.issued2021-01-15-
dc.identifier.scopus2-s2.0-85100125328-
dc.identifier.eissn1539-4794en_US
dc.description.validate202208 bchyen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberEE-0049-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextNational Key Research and Development Program of China; National Natural Science Foundation of China; Local Innovative and Research Teams Project of Guangdong Pear River Talents Program; The Hong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS53848190-
dc.description.oaCategoryGreen (AAM)en_US
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