Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/100584
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dc.contributorDepartment of Electrical and Electronic Engineeringen_US
dc.contributorMainland Development Officeen_US
dc.creatorZhang, Cen_US
dc.creatorYang, Yen_US
dc.creatorTan, Yen_US
dc.creatorHo, HLen_US
dc.creatorJin, Wen_US
dc.date.accessioned2023-08-11T03:10:46Z-
dc.date.available2023-08-11T03:10:46Z-
dc.identifier.issn1041-1135en_US
dc.identifier.urihttp://hdl.handle.net/10397/100584-
dc.language.isoenen_US
dc.publisherInstitute of Electrical and Electronics Engineersen_US
dc.rights© 2018 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media, including reprinting/republishing this material for advertising or promotional purposes, creating new collective works, for resale or redistribution to servers or lists, or reuse of any copyrighted component of this work in other works.en_US
dc.rightsThe following publication C. Zhang, Y. Yang, Y. Tan, H. L. Ho and W. Jin, "All-Optical Fiber Photoacoustic Gas Sensor With Double Resonant Enhancement," in IEEE Photonics Technology Letters, vol. 30, no. 20, pp. 1752-1755, 15 Oct. 2018 is available at https://doi.org/10.1109/LPT.2018.2868450.en_US
dc.subjectAcoustic resonatorsen_US
dc.subjectGas detectorsen_US
dc.subjectOptical fiber sensorsen_US
dc.subjectPhotoacoustic spectroscopyen_US
dc.titleAll-optical fiber photoacoustic gas sensor with double resonant enhancementen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1752en_US
dc.identifier.epage1755en_US
dc.identifier.volume30en_US
dc.identifier.issue20en_US
dc.identifier.doi10.1109/LPT.2018.2868450en_US
dcterms.abstractAn all-optical fiber photoacoustic gas sensor with double resonant signal enhancement is presented. The sensor uses a fiber-tip graphene nano-mechanical resonator operating at one of its resonances as the acoustic detector and a micro-acoustic resonant tube, whose resonant frequency is matched to that of the graphene resonator, as the PA gas cell. Compared with the single resonant detection with a graphene resonator, a five-fold signal enhancement is achieved. With 138-mW pump power and 1-s lock-in time constant, a noise equivalent concentration of ∼ 25-ppb C2H2 is achieved, corresponding to a normalized noise equivalent absorption of 1.29 × 10-8 cm-1WHz-1/2.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationIEEE photonics technology letters, 15 Oct. 2018, v. 30, no. 20, p. 1752-1755en_US
dcterms.isPartOfIEEE photonics technology lettersen_US
dcterms.issued2018-10-15-
dc.identifier.scopus2-s2.0-85052794112-
dc.identifier.eissn1941-0174en_US
dc.description.validate202307 bckwen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberEE-0435-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextNational Natural Science Foundation of China; The Hong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS53862225-
dc.description.oaCategoryGreen (AAM)en_US
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