Comparisons of surface and optical properties of the heavily carbon-doped GaN nanocrystalline films deposited by thermionic vacuum arc method

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In this paper, heavily C-doped GaN samples were deposited on glass and PET substrates by the thermionic vacuum arc (TVA) method, for the first time. Microstructure, surface and optical properties of the carbon-doped GaN samples were investigated by X-ray diffraction (XRD), field emission scanning electron microscopy, atomic force microscopy, and UV–Vis spectrophotometer. According to XRD pattern, fullerene (C60) structures were able to deposit in doped samples, for the first time. The fullerene structures were detected at heavily carbon-doped GaN. The obtained band gap changes of heavily carbon-doped GaN samples are determined. The band gap of CGaN on PET substrate decreased to a lower value, about 100 meV. The band gaps were shifted to the lowest wavelengths towards the edge of the UV region by heavily doped carbon. (002) and (004) peaks for GaN were also detected.

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AlanDeğerDil
dc.contributor.authorPat, Suat
dc.contributor.authorÖzen, Soner
dc.contributor.authorŞenay, Volkan
dc.contributor.authorKorkmaz, Şadan
dc.date.accessioned2026-10-29T19:11:13.858643068Z
dc.date.available2026-10-29T19:11:13.858643068Z
dc.date.issued2016
dc.description.abstractIn this paper, heavily C-doped GaN samples were deposited on glass and PET substrates by the thermionic vacuum arc (TVA) method, for the first time. Microstructure, surface and optical properties of the carbon-doped GaN samples were investigated by X-ray diffraction (XRD), field emission scanning electron microscopy, atomic force microscopy, and UV–Vis spectrophotometer. According to XRD pattern, fullerene (C60) structures were able to deposit in doped samples, for the first time. The fullerene structures were detected at heavily carbon-doped GaN. The obtained band gap changes of heavily carbon-doped GaN samples are determined. The band gap of CGaN on PET substrate decreased to a lower value, about 100 meV. The band gaps were shifted to the lowest wavelengths towards the edge of the UV region by heavily doped carbon. (002) and (004) peaks for GaN were also detected.
dc.description.sponsorshipESOGU BAP Commission, (201619A217)
dc.identifier.doi10.1016/j.vacuum.2016.08.013
dc.identifier.endpage42
dc.identifier.issn0042-207X
dc.identifier.scopus2-s2.0-84983732557
dc.identifier.startpage38
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/bayburt/13616
dc.identifier.volume133
dc.identifier.wosWOS:000385327000007
dc.language.isoen
dc.publisherElsevier Ltd
dc.relation.ispartofVacuum
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subjectC<sub>60</sub>-doped GaN
dc.subjectDoped GaN
dc.subjectOptical properties
dc.subjectSurface properties
dc.subject.classificationMaterials Science, Multidisciplinary
dc.subject.classificationPhysics, Applied
dc.subject.classificationMaterials Science
dc.subject.classificationPhysics
dc.subject.otherAtomic force microscopy
dc.subject.otherCarbon films
dc.subject.otherEnergy gap
dc.subject.otherField emission microscopes
dc.subject.otherFullerenes
dc.subject.otherGallium nitride
dc.subject.otherNanocrystals
dc.subject.otherScanning electron microscopy
dc.subject.otherSubstrates
dc.subject.otherSurface properties
dc.subject.otherVacuum applications
dc.subject.otherVacuum technology
dc.subject.otherX ray diffraction
dc.subject.otherDoped GaN
dc.subject.otherField emission scanning electron microscopy
dc.subject.otherFullerene structure
dc.subject.otherHeavily doped
dc.subject.otherNano-crystalline films
dc.subject.otherPET substrate
dc.subject.otherThermionic vacuum arc methods
dc.subject.otherXRD patterns
dc.subject.otherOptical properties
dc.titleComparisons of surface and optical properties of the heavily carbon-doped GaN nanocrystalline films deposited by thermionic vacuum arc method
dc.typeArticle
rdl.citation.openalex7
rdl.citation.scopus6
rdl.citation.wos5
rdl.oa.statusclosed
rdl.scopus.quartileQ2
rdl.source.indexSCOPUS
rdl.source.indexWOS
rdl.wos.indexScience Citation Index Expanded (SCI-EXPANDED)