Electronic transport properties of graphene/Al2O3 (0001) interface

Detalhes bibliográficos
Autor(a) principal: Gusmão, M. S.
Data de Publicação: 2018
Outros Autores: Ghosh, Angsula [UNESP], Frota, H. O.
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UNESP
Texto Completo: http://dx.doi.org/10.1016/j.cap.2017.10.008
http://hdl.handle.net/11449/175365
Resumo: The electronic structure and transport properties of a single layer of graphene (Gr) on α-Al2O3 surface are studied using the density functional theory (DFT). We present three models that take into account the atom at the termination of the alumina surface: a) Al atoms, with the center of the Gr hexagon directly over an Al atom; b) Al atoms, with a carbon directly positioned above an Al atom; c) oxygen atoms. Two processes of geometric optimization were used: (i) All the atoms of the supercell were allowed to move in accordance with the BFGS quasi-Newton algorithm; (ii) The atoms of the three topmost layers of the α-Al2O3 (0001) slab, including the C atoms, were allowed to move, whereas the atoms of the remaining layers were frozen in their respective atomic bulk positions. The first two models preserve qualitatively the electronic structure of the pristine Gr using the geometric optimization process (i) whereas, in the third model this structure was lost due to a significant charge transfer between the carbon and oxygen atoms irrespective of the optimization procedure. However, models (a) and (b) with the optimization (ii) reveal a p-type semiconducting behavior.
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spelling Electronic transport properties of graphene/Al2O3 (0001) interfaceAluminaDFTGrapheneTransport propertiesThe electronic structure and transport properties of a single layer of graphene (Gr) on α-Al2O3 surface are studied using the density functional theory (DFT). We present three models that take into account the atom at the termination of the alumina surface: a) Al atoms, with the center of the Gr hexagon directly over an Al atom; b) Al atoms, with a carbon directly positioned above an Al atom; c) oxygen atoms. Two processes of geometric optimization were used: (i) All the atoms of the supercell were allowed to move in accordance with the BFGS quasi-Newton algorithm; (ii) The atoms of the three topmost layers of the α-Al2O3 (0001) slab, including the C atoms, were allowed to move, whereas the atoms of the remaining layers were frozen in their respective atomic bulk positions. The first two models preserve qualitatively the electronic structure of the pristine Gr using the geometric optimization process (i) whereas, in the third model this structure was lost due to a significant charge transfer between the carbon and oxygen atoms irrespective of the optimization procedure. However, models (a) and (b) with the optimization (ii) reveal a p-type semiconducting behavior.Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Department of Physics Federal University of AmazonasSão Paulo State University(Unesp) Institute for Theoretical Physics (IFT)São Paulo State University(Unesp) Institute for Theoretical Physics (IFT)Federal University of AmazonasUniversidade Estadual Paulista (Unesp)Gusmão, M. S.Ghosh, Angsula [UNESP]Frota, H. O.2018-12-11T17:15:31Z2018-12-11T17:15:31Z2018-01-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article90-95application/pdfhttp://dx.doi.org/10.1016/j.cap.2017.10.008Current Applied Physics, v. 18, n. 1, p. 90-95, 2018.1567-1739http://hdl.handle.net/11449/17536510.1016/j.cap.2017.10.0082-s2.0-850318249062-s2.0-85031824906.pdfScopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengCurrent Applied Physics0,647info:eu-repo/semantics/openAccess2023-12-03T06:11:20Zoai:repositorio.unesp.br:11449/175365Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T19:21:34.740023Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false
dc.title.none.fl_str_mv Electronic transport properties of graphene/Al2O3 (0001) interface
title Electronic transport properties of graphene/Al2O3 (0001) interface
spellingShingle Electronic transport properties of graphene/Al2O3 (0001) interface
Gusmão, M. S.
Alumina
DFT
Graphene
Transport properties
title_short Electronic transport properties of graphene/Al2O3 (0001) interface
title_full Electronic transport properties of graphene/Al2O3 (0001) interface
title_fullStr Electronic transport properties of graphene/Al2O3 (0001) interface
title_full_unstemmed Electronic transport properties of graphene/Al2O3 (0001) interface
title_sort Electronic transport properties of graphene/Al2O3 (0001) interface
author Gusmão, M. S.
author_facet Gusmão, M. S.
Ghosh, Angsula [UNESP]
Frota, H. O.
author_role author
author2 Ghosh, Angsula [UNESP]
Frota, H. O.
author2_role author
author
dc.contributor.none.fl_str_mv Federal University of Amazonas
Universidade Estadual Paulista (Unesp)
dc.contributor.author.fl_str_mv Gusmão, M. S.
Ghosh, Angsula [UNESP]
Frota, H. O.
dc.subject.por.fl_str_mv Alumina
DFT
Graphene
Transport properties
topic Alumina
DFT
Graphene
Transport properties
description The electronic structure and transport properties of a single layer of graphene (Gr) on α-Al2O3 surface are studied using the density functional theory (DFT). We present three models that take into account the atom at the termination of the alumina surface: a) Al atoms, with the center of the Gr hexagon directly over an Al atom; b) Al atoms, with a carbon directly positioned above an Al atom; c) oxygen atoms. Two processes of geometric optimization were used: (i) All the atoms of the supercell were allowed to move in accordance with the BFGS quasi-Newton algorithm; (ii) The atoms of the three topmost layers of the α-Al2O3 (0001) slab, including the C atoms, were allowed to move, whereas the atoms of the remaining layers were frozen in their respective atomic bulk positions. The first two models preserve qualitatively the electronic structure of the pristine Gr using the geometric optimization process (i) whereas, in the third model this structure was lost due to a significant charge transfer between the carbon and oxygen atoms irrespective of the optimization procedure. However, models (a) and (b) with the optimization (ii) reveal a p-type semiconducting behavior.
publishDate 2018
dc.date.none.fl_str_mv 2018-12-11T17:15:31Z
2018-12-11T17:15:31Z
2018-01-01
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
format article
status_str publishedVersion
dc.identifier.uri.fl_str_mv http://dx.doi.org/10.1016/j.cap.2017.10.008
Current Applied Physics, v. 18, n. 1, p. 90-95, 2018.
1567-1739
http://hdl.handle.net/11449/175365
10.1016/j.cap.2017.10.008
2-s2.0-85031824906
2-s2.0-85031824906.pdf
url http://dx.doi.org/10.1016/j.cap.2017.10.008
http://hdl.handle.net/11449/175365
identifier_str_mv Current Applied Physics, v. 18, n. 1, p. 90-95, 2018.
1567-1739
10.1016/j.cap.2017.10.008
2-s2.0-85031824906
2-s2.0-85031824906.pdf
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Current Applied Physics
0,647
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv 90-95
application/pdf
dc.source.none.fl_str_mv Scopus
reponame:Repositório Institucional da UNESP
instname:Universidade Estadual Paulista (UNESP)
instacron:UNESP
instname_str Universidade Estadual Paulista (UNESP)
instacron_str UNESP
institution UNESP
reponame_str Repositório Institucional da UNESP
collection Repositório Institucional da UNESP
repository.name.fl_str_mv Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)
repository.mail.fl_str_mv
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