Please use this identifier to cite or link to this item: http://hdl.handle.net/10773/35862
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dc.contributor.authorSharma, Dhananjay K.pt_PT
dc.contributor.authorFateixa, Sarapt_PT
dc.contributor.authorHortigüela, María J.pt_PT
dc.contributor.authorVidyasagar, Reddithotapt_PT
dc.contributor.authorOtero-Irurueta, Gonzalopt_PT
dc.contributor.authorNogueira, Helena I. S.pt_PT
dc.contributor.authorSingh, Manoj Kumarpt_PT
dc.contributor.authorKholkin, Andreipt_PT
dc.date.accessioned2023-01-18T17:54:22Z-
dc.date.available2023-01-18T17:54:22Z-
dc.date.issued2017-05-
dc.identifier.issn0921-4526pt_PT
dc.identifier.urihttp://hdl.handle.net/10773/35862-
dc.description.abstractTuning the band-gap of graphene is a current need for real device applications. Copper (Cu) as a substrate plays a crucial role in graphene deposition. Here we report the fabrication of in-situ nitrogen (N) doped graphene via chemical vapor deposition (CVD) technique and the effect of Cu substrate thickness on the growth mechanism. The ratio of intensities of G and D peaks was used to evaluate the defect concentration based on local activation model associated with the distortion of the crystal lattice due to incorporation of nitrogen atoms into graphene lattice. The results suggest that Cu substrate of 20μm in thickness exhibits higher defect density (1.86×1012 cm−2) as compared to both 10 and 25 μm thick substrates (1.23×1012 cm−2 and 3.09×1011 cm−2, respectively). Furthermore, High Resolution -X-ray Photoelectron Spectroscopy (HR-XPS) precisely affirms ~0.4 at% of nitrogen intercalations in graphene. Our results show that the substitutional type of nitrogen doping dominates over the pyridinic configuration. In addition, X-ray diffraction (XRD) shows all the XRD peaks associated with carbon. However, the peak at ~24° is suppressed by the substrate peaks (Cu). These results suggest that nitrogen atoms can be efficiently incorporated into the graphene using thinner copper substrates, rather than the standard 25 μm ones. This is important for tailoring the properties by graphene required for microelectronic applications.pt_PT
dc.language.isoengpt_PT
dc.publisherElsevierpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/FARH/SFRH%2FBPD%2F93547%2F2013/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/POR_CENTRO/SFRH%2FBPD%2F104887%2F2014/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/6817 - DCRRNI ID/UID%2FEMS%2F00481%2F2013/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/Investigador FCT/IF%2F01054%2F2015%2FCP1302%2FCT0020/PTpt_PT
dc.relationinfo:eu-repo/grantAgreement/FCT/6817 - DCRRNI ID/UID%2FCTM%2F50011%2F2013/PTpt_PT
dc.rightsrestrictedAccesspt_PT
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/pt_PT
dc.subjectGraphenept_PT
dc.subjectNitrogen-dopingpt_PT
dc.subjectDefectspt_PT
dc.subjectRamanpt_PT
dc.subjectSpectroscopy (HR-XPS)pt_PT
dc.subjectHigh Resolution-X-ray Photoelectronpt_PT
dc.subjectCVDpt_PT
dc.titleDefect concentration in nitrogen-doped graphene grown on Cu substrate: a thickness effectpt_PT
dc.typearticlept_PT
dc.description.versionpublishedpt_PT
dc.peerreviewedyespt_PT
degois.publication.firstPage62pt_PT
degois.publication.lastPage68pt_PT
degois.publication.titlePhysica B: Condensed Matterpt_PT
degois.publication.volume513pt_PT
dc.identifier.doi10.1016/j.physb.2017.03.004pt_PT
Appears in Collections:TEMA - Artigos
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