Controlling the photoconductivity: graphene oxide and polyaniline self assembled intercalation
buir.contributor.author | Uyar, Tamer | |
buir.contributor.orcid | Uyar, Tamer|0000-0002-3989-4481 | |
dc.citation.epage | 051106-4 | en_US |
dc.citation.issueNumber | 5 | en_US |
dc.citation.spage | 051106-1 | en_US |
dc.citation.volumeNumber | 106 | en_US |
dc.contributor.author | Vempati S. | en_US |
dc.contributor.author | Ozcan, S. | en_US |
dc.contributor.author | Uyar, Tamer | en_US |
dc.date.accessioned | 2016-02-08T10:01:23Z | |
dc.date.available | 2016-02-08T10:01:23Z | |
dc.date.issued | 2015 | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.department | Nanotechnology Research Center (NANOTAM) | en_US |
dc.description.abstract | We report on controlling the optoelectronic properties of self-assembled intercalating compound of graphene oxide (GO) and HCl doped polyaniline (PANI). Optical emission and X-ray diffraction studies revealed a secondary doping phenomenon of PANI with -OH and -COOH groups of GO, which essentially arbitrate the intercalation. A control on the polarity and the magnitude of the photoresponse (PR) is harnessed by manipulating the weight ratios of PANI to GO (viz., 1:1.5 and 1:2.2 are abbreviated as PG1.5 and PG2.2, respectively), where ±PR = 100(RDark - RUV-Vis)/RDark and R corresponds to the resistance of the device in dark or UV-Vis illumination. To be precise, the PR from GO, PANI, PG1.5, and PG2.2 are +34%, -111%, -51%, and +58%, respectively. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T10:01:23Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2015 | en |
dc.identifier.doi | 10.1063/1.4907260 | en_US |
dc.identifier.issn | 0003-6951 | |
dc.identifier.uri | http://hdl.handle.net/11693/22536 | |
dc.language.iso | English | en_US |
dc.publisher | American Institute of Physics Inc. | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1063/1.4907260 | en_US |
dc.source.title | Applied Physics Letters | en_US |
dc.subject | Doping (additives) | en_US |
dc.subject | Intercalation | en_US |
dc.subject | Polyaniline | en_US |
dc.subject | X ray diffraction | en_US |
dc.subject | Doped polyaniline | en_US |
dc.subject | Graphene oxides | en_US |
dc.subject | Optical emissions | en_US |
dc.subject | Optoelectronic properties | en_US |
dc.subject | Photoresponses | en_US |
dc.subject | Self-assembled | en_US |
dc.subject | Weight ratios | en_US |
dc.subject | X-ray diffraction studies | en_US |
dc.subject | Graphene | en_US |
dc.title | Controlling the photoconductivity: graphene oxide and polyaniline self assembled intercalation | en_US |
dc.type | Article | en_US |
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