Modulation of electronic properties in laterally and commensurately repeating graphene and boron nitride composite nanostructures

buir.contributor.authorÇıracı, Salim
buir.contributor.authorDurgun, Engin
buir.contributor.orcidÇıracı, Salim|0000-0001-8023-9860
dc.citation.epage13256en_US
dc.citation.issueNumber23en_US
dc.citation.spage13248en_US
dc.citation.volumeNumber119en_US
dc.contributor.authorÖzçelik, V. O.en_US
dc.contributor.authorDurgun, Enginen_US
dc.contributor.authorÇıracı, Salimen_US
dc.date.accessioned2016-02-08T09:50:22Z
dc.date.available2016-02-08T09:50:22Z
dc.date.issued2015en_US
dc.departmentDepartment of Physicsen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.departmentNanotechnology Research Center (NANOTAM)en_US
dc.description.abstractGraphene and hexagonal boron nitride (h-BN) nanoribbons of diverse widths and edge geometries are laterally repeated to form commensurate, single-layer, hybrid honeycomb structures. The resulting composite materials appear as continuous, one atom thick stripes of graphene and BN having the average mechanical properties of constituent structures. However, depending on the widths of constituent stripes they can be metal or semiconductor with band gaps in the energy range of the visible light. These two-dimensional (2D) composite materials allow strong dimensionality in electrical conductivity and undergo transition from 2D to one-dimensional (1D) metal in a 2D medium, resulting in multichannel narrow conductors. As for the composite ribbons, such as one dielectric BN stripe placed between two graphene stripes with bare zigzag edges, charge separation of opposite polarity is possible under applied electric field and they exhibit resonant tunneling effects at nanoscale. Graphene/BN composite materials also form stable single-wall nanotubes with zigzag or armchair geometries.en_US
dc.description.provenanceMade available in DSpace on 2016-02-08T09:50:22Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2015en
dc.identifier.doi10.1021/acs.jpcc.5b01598en_US
dc.identifier.issn1932-7447
dc.identifier.urihttp://hdl.handle.net/11693/21725
dc.language.isoEnglishen_US
dc.publisherAmerican Chemical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1021/acs.jpcc.5b01598en_US
dc.source.titleJournal of Physical Chemistry Cen_US
dc.subjectBoron nitrideen_US
dc.subjectComposite materialsen_US
dc.subjectElectric fieldsen_US
dc.subjectElectronic propertiesen_US
dc.subjectEnergy gapen_US
dc.subjectHoneycomb structuresen_US
dc.subjectNitridesen_US
dc.subjectResonant tunnelingen_US
dc.subjectYarnen_US
dc.subjectCharge separationsen_US
dc.subjectComposite nanostructuresen_US
dc.subjectElectrical conductivityen_US
dc.subjectEnergy rangesen_US
dc.subjectHexagonal boron nitride (h-BN)en_US
dc.subjectNarrow conductorsen_US
dc.subjectSingle wall nanotubesen_US
dc.subjectTwo Dimensional (2 D)en_US
dc.subjectGrapheneen_US
dc.titleModulation of electronic properties in laterally and commensurately repeating graphene and boron nitride composite nanostructuresen_US
dc.typeArticleen_US

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