Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/70663
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dc.contributorDepartment of Applied Physics-
dc.creatorZuo, WB-
dc.creatorTang, LB-
dc.creatorXiang, JZ-
dc.creatorJi, RB-
dc.creatorLuo, L-
dc.creatorRogee, L-
dc.creatorLau, SP-
dc.date.accessioned2017-12-28T06:17:42Z-
dc.date.available2017-12-28T06:17:42Z-
dc.identifier.issn0003-6951-
dc.identifier.urihttp://hdl.handle.net/10397/70663-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2017 Author(s).en_US
dc.rightsThis article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in W. B. Zuo et al., Appl. Phys. Lett. 110, 221901 (2017) and may be found at https://dx.doi.org/10.1063/1.4984238en_US
dc.titleFunctionalization of graphene quantum dots by fluorine : preparation, properties, application, and their mechanismsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume110-
dc.identifier.issue22-
dc.identifier.doi10.1063/1.4984238-
dcterms.abstractGraphene quantum dots (GQDs) possess unique photoelectronic properties ascribed to quantum confinement and edge effects, which have evoked important development and wide application in the optoelectronic field. Doping GQDs with heteroatoms can further modulate the energy band structure and thus produce unexpected properties. Herein, we obtained fluorine-doped GQDs (F-GQDs) by adopting an effective preparation technique, which includes the treatment of the as-prepared reaction precursor, fluorinated carbon fibers, with ultrasonic liquid phase exfoliation. The proposed method is simple, handy, and low-cost, opening up an alternate approach to prepare F-GQDs. Through multiple characterization techniques, the effective incorporation of fluorine in GQDs was confirmed, and the as-prepared F-GQDs exhibit excellent photoelectrical properties and good ultraviolet absorption performances. Accordingly, we have fabricated a vertical photovoltaic UV detector based on F-GQDs. The unoptimized device has an exceptionally large ratio of photocurrent to dark current of magnitude similar to 10(5), and its detectivity (D*) could stabilize at around 10(12) Jones at room temperature under lambda = 365 nm light irradiation and reverse bias voltage.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationApplied physics letters, 2017, v. 110, no. 22, 221901, p. 221901-1-221901-5-
dcterms.isPartOfApplied physics letters-
dcterms.issued2017-
dc.identifier.isiWOS:000403341300013-
dc.identifier.ros2016005758-
dc.identifier.eissn1077-3118-
dc.identifier.artn221901-
dc.identifier.rosgroupid2016005505-
dc.description.ros2016-2017 > Academic research: refereed > Publication in refereed journal-
dc.description.validatebcrc-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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