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Density functional theory calculations on graphene/α-SiO(2)(0001) interface

In this work, the graphene/α-SiO(2)(0001) interface is calculated using density functional theory. On the oxygen-terminated SiO(2 )surface, atomic structure reconstruction occurs at the graphene/SiO(2 )interface to eliminate the dangling bonds. The interface interaction is 77 meV/C atom, which indic...

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Detalles Bibliográficos
Autores principales: Ao, Zhimin, Jiang, Man, Wen, Zi, Li, Sean
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer 2012
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3305479/
https://www.ncbi.nlm.nih.gov/pubmed/22373326
http://dx.doi.org/10.1186/1556-276X-7-158
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author Ao, Zhimin
Jiang, Man
Wen, Zi
Li, Sean
author_facet Ao, Zhimin
Jiang, Man
Wen, Zi
Li, Sean
author_sort Ao, Zhimin
collection PubMed
description In this work, the graphene/α-SiO(2)(0001) interface is calculated using density functional theory. On the oxygen-terminated SiO(2 )surface, atomic structure reconstruction occurs at the graphene/SiO(2 )interface to eliminate the dangling bonds. The interface interaction is 77 meV/C atom, which indicates that van der Waals force dominates the interaction, but it is stronger than the force between the graphene layers in graphite. The distance between graphene and the SiO(2 )surface is 2.805 Å, which is smaller than the 3.4 Å interlayer distance of graphite. In addition, the SiO(2 )substrate induces p-type doping in graphene and opens a small gap of 0.13 eV at the Dirac point of graphene, which is desirable for electronic device applications.
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spelling pubmed-33054792012-03-16 Density functional theory calculations on graphene/α-SiO(2)(0001) interface Ao, Zhimin Jiang, Man Wen, Zi Li, Sean Nanoscale Res Lett Nano Express In this work, the graphene/α-SiO(2)(0001) interface is calculated using density functional theory. On the oxygen-terminated SiO(2 )surface, atomic structure reconstruction occurs at the graphene/SiO(2 )interface to eliminate the dangling bonds. The interface interaction is 77 meV/C atom, which indicates that van der Waals force dominates the interaction, but it is stronger than the force between the graphene layers in graphite. The distance between graphene and the SiO(2 )surface is 2.805 Å, which is smaller than the 3.4 Å interlayer distance of graphite. In addition, the SiO(2 )substrate induces p-type doping in graphene and opens a small gap of 0.13 eV at the Dirac point of graphene, which is desirable for electronic device applications. Springer 2012-02-28 /pmc/articles/PMC3305479/ /pubmed/22373326 http://dx.doi.org/10.1186/1556-276X-7-158 Text en Copyright ©2012 Ao et al; licensee Springer. http://creativecommons.org/licenses/by/2.0 This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Nano Express
Ao, Zhimin
Jiang, Man
Wen, Zi
Li, Sean
Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title_full Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title_fullStr Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title_full_unstemmed Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title_short Density functional theory calculations on graphene/α-SiO(2)(0001) interface
title_sort density functional theory calculations on graphene/α-sio(2)(0001) interface
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3305479/
https://www.ncbi.nlm.nih.gov/pubmed/22373326
http://dx.doi.org/10.1186/1556-276X-7-158
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