Utilize este identificador para referenciar este registo: https://hdl.handle.net/1822/47699

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dc.contributor.authorCerqueira, M. F.por
dc.contributor.authorVieira, L. G.por
dc.contributor.authorAlves, A.por
dc.contributor.authorCorreia, R.por
dc.contributor.authorHuber, M.por
dc.contributor.authorAndreev, A.por
dc.contributor.authorBonanni, A.por
dc.contributor.authorVasilevskiy, Mikhailpor
dc.date.accessioned2017-11-23T11:29:20Z-
dc.date.available2017-11-23T11:29:20Z-
dc.date.issued2017-
dc.identifier.citationJournal of Physics D: Applied Physics 50, 365103 (2017)por
dc.identifier.issn0022-3727por
dc.identifier.urihttps://hdl.handle.net/1822/47699-
dc.description.abstractRaman spectroscopy, with both resonant and non-resonant excitation, and infra-red (IR) spectroscopy, in the attenuated total reflection (ATR) configuration, was employed to study lattice vibration modes in a set of carbon-doped GaN (GaN:C) epilayers grown by metalorganic vapour phase epitaxy (MOVPE). We analyse Raman and IR-ATR spectra from the point of view of possible effects of the carbon doping, namely: (i) local vibration mode of C atom in a N sublattice (whose frequency we theoretically estimate as 768 cm-1 using an isotope defect model), and (ii) shift in the positions of longitudinal modes owing to the phonon-plasmon coupling. We find only some indirect hints of the doping effect on the resonant Raman spectra. However, we show theoretically and confirm experimentally that the IR-ATR spectroscopy can be a much more sensitive tool for this purpose, at least for the considered structures. A weak perturbation of the dielectric function of GaN:C, caused by the substitutional carbon impurity, is shown to produce a measurable dip in the ATR reflectivity spectra at ≈ 770 cm-1, for both p- and s-polarizations. Moreover, it influences a specific (guided-wave-type) mode observed at ≈ 737 cm-1, originating from the GaN layer, which appears in the narrow frequency window where the real parts of the two components of the dielectric tensor of the hexagonal crystal have the opposite signs. This interpretation is supported by our modelling of the whole multilayer structure using a transfer matrix formalism.por
dc.description.sponsorshipThis work was supported by FEDER through the COMPETE Program and by the Portuguese Foundation for Science and Technology (FCT) in the framework of the Strategic Financing UID/FIS/04650/2013 and Infineon Technologies Austria AG.por
dc.language.isoengpor
dc.publisherIOP Publishingpor
dc.relationinfo:eu-repo/grantAgreement/FCT/5876/147414/PTpor
dc.rightsopenAccesspor
dc.subjectRaman spectroscopypor
dc.subjectATR-IR spectroscopypor
dc.subjectPhononpor
dc.subjectPolaritonpor
dc.subjectCarbon dopingpor
dc.subjectGallium nitridepor
dc.titleRaman and IR-ATR spectroscopy studies of heteroepitaxial structures with a GaN:C top layerpor
dc.typearticlepor
dc.peerreviewedyespor
dc.relation.publisherversionhttps://doi.org/10.1088/1361-6463/aa7c4bpor
oaire.citationStartPage365103por
oaire.citationEndPage365115por
oaire.citationIssue36por
oaire.citationVolume50por
dc.identifier.eissn1361-6463por
dc.identifier.doi10.1088/1361-6463/aa7c4bpor
dc.subject.fosCiências Naturais::Ciências Físicaspor
dc.description.publicationversioninfo:eu-repo/semantics/publishedVersionpor
dc.subject.wosScience & Technologypor
sdum.journalJournal of Physics D: Applied Physicspor
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