Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/6560
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dc.contributorDepartment of Electrical Engineering-
dc.creatorShao, L-
dc.creatorWang, T-
dc.creatorCanning, J-
dc.creatorCook, K-
dc.creatorTam, HY-
dc.date.accessioned2014-12-11T08:24:38Z-
dc.date.available2014-12-11T08:24:38Z-
dc.identifier.issn1559-128X-
dc.identifier.urihttp://hdl.handle.net/10397/6560-
dc.language.isoenen_US
dc.publisherOptical Society of Americaen_US
dc.rights© 2012 Optical Society of America. This paper was published in Applied Optics 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/ao/abstract.cfm?URI=ao-51-30-7165. 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.subjectFiber Bragg gratingsen_US
dc.subjectMachine toolsen_US
dc.subjectProduction engineeringen_US
dc.subjectSilicaen_US
dc.titleBulk regeneration of optical fiber Bragg gratingsen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Li-Yang Shaoen_US
dc.identifier.spage7165-
dc.identifier.epage7169-
dc.identifier.volume51-
dc.identifier.issue30-
dc.identifier.doi10.1364/AO.51.007165-
dcterms.abstractThe reliability and reproducibility of regenerated gratings for mass production is assessed through simultaneous bulk regeneration of 10 gratings. The gratings are characterized and variations are compared after each stage of fabrication, including seed (room-temperature UV fabrication), regeneration (annealing at 850°C), and postannealing (annealing at 1100°C). In terms of Bragg wavelength (λ [sub B]), the seed grating variation lies within Δλ[sub B] = 0.16 nm, the regenerated grating within Δλ[sub B]= 0.41 nm, and the postannealed grating within Δλ [sub B] = 1.42 nm. All the results are within reasonable error, indicating that mass production is feasible. The observable spread in parameters from seed to regenerated grating is clearly systematic. The postannealed spread arises from the small tension on the fiber during postannealing and can be explained by the softening of the glass when the strain temperature of silica is reached.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationApplied optics, 20 Oct. 2012, v. 51, no. 30, p. 7165-7169-
dcterms.isPartOfApplied optics-
dcterms.issued2012-10-20-
dc.identifier.isiWOS:000310430900005-
dc.identifier.scopus2-s2.0-84868021978-
dc.identifier.eissn2155-3165-
dc.identifier.rosgroupidr66542-
dc.description.ros2012-2013 > 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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