{"data":{"id":"10.6084/m9.figshare.c.3933991","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.3933991","prefix":"10.6084","suffix":"m9.figshare.c.3933991","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Zhihong Li","affiliation":[],"nameIdentifiers":[]},{"name":"Shen, Jie","nameType":"Personal","givenName":"Jie","familyName":"Shen","affiliation":[],"nameIdentifiers":[]},{"name":"Qiuping Ji","affiliation":[],"nameIdentifiers":[]},{"name":"Yaoju Zhang","affiliation":[],"nameIdentifiers":[]},{"name":"Xiukai Ruan","affiliation":[],"nameIdentifiers":[]},{"name":"Yuxing Dai","affiliation":[],"nameIdentifiers":[]},{"name":"Zhennao Cai","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Tuning the resonance of polarization-degenerate cladding mode LP1,j in excessively tilted long period fiber grating for highly sensitive refractive index sensing"}],"publisher":"Figshare","container":{},"publicationYear":2018,"subjects":[{"subject":"100506 Optical Fibre Communications","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"20504 Photonics, Optoelectronics and Optical Communications","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2017-11-18","dateType":"Created"},{"date":"2018-02-13","dateType":"Updated"},{"date":"2018","dateType":"Issued"}],"language":null,"types":{"ris":"GEN","bibtex":"misc","citeproc":"article","schemaOrg":"Collection","resourceType":"Collection","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1364/josaa.35.000397","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC BY 4.0","rightsUri":"https://creativecommons.org/licenses/by/4.0"}],"descriptions":[{"description":"This work presents a sensitive refractive index sensor based on the dual resonance of excessively tilted\nlong period fiber grating (Ex-TLPFG). The Ex-TLPFG is tuned to couple the guided core mode with only\npolarization-degenerate cladding mode LP1,l which consists of TE/TM0,l and HE2,l vector modes. It is\nfound that the p-polarized LPp\n1,l mode exhibits a higher sensitivity than that of s-polarized LPs\n1,l mode. An\noptimized sensitivity as high as 12182.9 nm/RIU is achieved for p-polarized LPp\n1,2 mode at low refractive\nindex region by tuning initial resonance condition. The sensing performance is also evaluated through\nthe power measurement method for a single resonance band. It is demonstrated that the improved sensitivity\nin this work for diameter-reduced Ex-TLPFG is much higher than that for the conventional LPFG\nbased devices, which makes this sensing platform very attractive for a variety of index sensing applications.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/collections/Tuning_the_resonance_of_polarization-degenerate_cladding_mode_LP1_j_in_excessively_tilted_long_period_fiber_grating_for_highly_sensitive_refractive_index_sensing/3933991","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":tru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