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On the origin of exciton formation in dye doped Alq(3) OLEDs

dc.contributor.authorGomez, J. A.
dc.contributor.authorCastro, F. A.
dc.contributor.authorNueesch, F.
dc.contributor.authorZuppiroli, L.
dc.contributor.authorGraeff, Carlos Frederico de Oliveira [UNESP]
dc.contributor.institutionUniversidade de São Paulo (USP)
dc.contributor.institutionNatl Phys Lab
dc.contributor.institutionEmpa
dc.contributor.institutionEcole Polytech Fed Lausanne
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-20T13:26:17Z
dc.date.available2014-05-20T13:26:17Z
dc.date.issued2012-09-01
dc.description.abstractElectrically Detected Magnetic Resonance (EDMR) was used to investigate the influence of dye doping on spin-dependent exciton formation in aluminum (III) 8-hydroxyquinoline (Alq(3)) based Organic Light Emitting Diodes (OLEDs) with different device structures. 4-(dicyanomethylene)-2-methyl-6-{2-[(4-diphenylamino)-phenyl]ethyl}-4H-pyran (DCM-TPA) and 5,6,11,12-tetraphenylnaphthacene (Rubrene) were used as dopants. Results at room temperature show significant differences on the EDMR spectra (g-factor and linewidth) of doped and undoped devices. Signals from DCM-TPA and Rubrene dye doped OLEDs showed strong temperature dependence, with signal intensity increasing by 2 orders of magnitude below 200 K for DCM-TPA dye doped OLEDs and increasing by similar to 1 order of magnitude below 225 K for the Rubrene dye doped device, while undoped devices shows almost no temperature dependence. By adding a "spacer" layer of undoped Alq(3) at the recombination zone, changes in bias voltage were used to shift the recombination from doped to undoped region and correlate that with changes in the EDMR spectrum. Our results are indicating that charge trapping on the dopant followed by recombination is the main mechanism of light emission in the investigated devices.en
dc.description.affiliationFFCLRP USP, Dept Fis, BR-14040901 São Paulo, Brazil
dc.description.affiliationNatl Phys Lab, Div Mat, Teddington TW11 0LW, Middx, England
dc.description.affiliationEmpa, Swiss Fed Labs Mat Testing & Res, Lab Funct Polymers, CH-8600 Dubendorf, Switzerland
dc.description.affiliationEcole Polytech Fed Lausanne, Inst Mat, Lab Optoelect Mat Mol, CH-1015 Lausanne, Switzerland
dc.description.affiliationFC UNESP, Dept Fis, BR-17033360 São Paulo, Brazil
dc.description.affiliationUnespFC UNESP, Dept Fis, BR-17033360 São Paulo, Brazil
dc.description.sponsorshipFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
dc.description.sponsorshipConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
dc.description.sponsorshipCoordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)
dc.format.extent727-731
dc.identifierhttp://dx.doi.org/10.1007/s00339-012-6957-8
dc.identifier.citationApplied Physics A-materials Science & Processing. New York: Springer, v. 108, n. 3, p. 727-731, 2012.
dc.identifier.doi10.1007/s00339-012-6957-8
dc.identifier.issn0947-8396
dc.identifier.orcid0000-0003-0162-8273
dc.identifier.urihttp://hdl.handle.net/11449/8445
dc.identifier.wosWOS:000307255100030
dc.language.isoeng
dc.publisherSpringer
dc.relation.ispartofApplied Physics A-materials Science & Processing
dc.relation.ispartofjcr1.604
dc.relation.ispartofsjr0,481
dc.rights.accessRightsAcesso restrito
dc.sourceWeb of Science
dc.titleOn the origin of exciton formation in dye doped Alq(3) OLEDsen
dc.typeArtigo
dcterms.licensehttp://www.springer.com/open+access/authors+rights?SGWID=0-176704-12-683201-0
dcterms.rightsHolderSpringer
dspace.entity.typePublication
unesp.author.lattes5268607684223281[5]
unesp.author.orcid0000-0003-0162-8273[5]
unesp.campusUniversidade Estadual Paulista (UNESP), Faculdade de Ciências, Baurupt
unesp.departmentFísica - FCpt

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