Electronic transport properties of graphene/Al2O3 (0001) interface
Autor(a) principal: | |
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Data de Publicação: | 2018 |
Outros Autores: | , |
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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Repositório Institucional da UNESP |
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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 |
|
_version_ |
1808128230469664768 |