{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1361699994184490496.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1109/jlt.2003.815505"}},{"identifier":{"@type":"URI","@value":"http://xplorestaging.ieee.org/ielx5/50/27568/01230187.pdf?arnumber=1230187"}}],"dc:title":[{"@value":"Phased-only sampled fiber bragg gratings for high-channel-count chromatic dispersion compensation"}],"description":[{"notation":[{"@value":"Binary and multilevel phase-only sampling functions are proposed for the sampled fiber Bragg gratings (FBGs) with high channel count, which require significantly less refractive-index modulation than that does the sampled grating with amplitude sampling. The design using the new simulated quenching optimization with temperature rescaling results in high channel uniformity and minimum energy in the out-of-band channels. The technique can be applied to the sampled FBGs with very high channel count. A five-channel nonlinearly chirped multilevel phase-only sampled FBG for tunable chromatic dispersion compensation is demonstrated."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1420001326237083904","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"90362186"},{"@type":"NRID","@value":"1000090362186"},{"@type":"NRID","@value":"9000005592804"},{"@type":"NRID","@value":"9000004927061"},{"@type":"NRID","@value":"9000004756229"},{"@type":"NRID","@value":"9000018143160"},{"@type":"NRID","@value":"9000018428717"},{"@type":"NRID","@value":"9000006909982"},{"@type":"NRID","@value":"9000258143724"},{"@type":"NRID","@value":"9000258616744"},{"@type":"NRID","@value":"9000006794284"},{"@type":"NRID","@value":"9000016866322"},{"@type":"NRID","@value":"9000242904686"},{"@type":"NRID","@value":"9000242893323"},{"@type":"NRID","@value":"9000017442921"},{"@type":"NRID","@value":"9000242893319"},{"@type":"NRID","@value":"9000401674710"},{"@type":"NRID","@value":"9000017442706"},{"@type":"NRID","@value":"9000017716327"},{"@type":"NRID","@value":"9000280298529"},{"@type":"NRID","@value":"9000401683802"},{"@type":"NRID","@value":"9000018143164"},{"@type":"NRID","@value":"9000311485993"},{"@type":"NRID","@value":"9000006357952"},{"@type":"NRID","@value":"9000005601956"},{"@type":"NRID","@value":"9000242893330"},{"@type":"NRID","@value":"9000406172865"},{"@type":"NRID","@value":"9000017203305"},{"@type":"NRID","@value":"9000262061425"},{"@type":"NRID","@value":"9000321408851"},{"@type":"NRID","@value":"9000016866385"},{"@type":"NRID","@value":"9000018571142"},{"@type":"NRID","@value":"9000016912603"},{"@type":"NRID","@value":"9000017296267"},{"@type":"NRID","@value":"9000238616415"},{"@type":"NRID","@value":"9000301385592"},{"@type":"NRID","@value":"9000258616711"},{"@type":"NRID","@value":"9000258138520"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/Hongpuli"}],"foaf:name":[{"@value":"Hongpu Li"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994184490499","@type":"Researcher","foaf:name":[{"@value":"Yunlong Sheng"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994184490497","@type":"Researcher","foaf:name":[{"@value":"Yao Li"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994184490496","@type":"Researcher","foaf:name":[{"@value":"J.E. Rothenberg"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"07338724"}],"prism:publicationName":[{"@value":"Journal of Lightwave Technology"}],"dc:publisher":[{"@value":"Institute of Electrical and Electronics Engineers (IEEE)"}],"prism:publicationDate":"2003-09","prism:volume":"21","prism:number":"9","prism:startingPage":"2074","prism:endingPage":"2083"},"reviewed":"false","dc:rights":["https://ieeexplore.ieee.org/Xplorehelp/downloads/license-information/IEEE.html"],"url":[{"@id":"http://xplorestaging.ieee.org/ielx5/50/27568/01230187.pdf?arnumber=1230187"}],"createdAt":"2003-09-11","modifiedAt":"2025-04-03","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050573726369076992","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Phase-Inserted Fiber Gratings and Their Applications to Optical Filtering, Optical Signal Processing, and Optical Sensing: Review"}]},{"@id":"https://cir.nii.ac.jp/crid/1050845763798675456","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Ultrahigh-channel-count fiber Bragg grating based on the triple sampling method"}]},{"@id":"https://cir.nii.ac.jp/crid/1360584340724111360","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Full C-band covered and DWDM channelized high channel-count all-fiber orbital-angular-momentum mode generator based on the fiber gratings"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1109/jlt.2003.815505"},{"@type":"OPENAIRE","@value":"doi_dedup___::e6eeb2ac0cc57a26386428ea5390ce3e"},{"@type":"CROSSREF","@value":"10.3390/photonics9040271_references_DOI_YrABV1xhBa8ph4n4PK3TUSs1RsQ"},{"@type":"CROSSREF","@value":"10.1364/oe.494946_references_DOI_YrABV1xhBa8ph4n4PK3TUSs1RsQ"},{"@type":"CROSSREF","@value":"10.1016/j.optcom.2010.12.029_references_DOI_YrABV1xhBa8ph4n4PK3TUSs1RsQ"}]}