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dc.contributor.authorFloriano, Emerson-
dc.contributor.authorScalvi, Luis-
dc.contributor.authorSambrano, Julio Ricardo-
dc.date.accessioned2016-03-02T13:03:35Z-
dc.date.accessioned2016-10-25T21:33:06Z-
dc.date.available2016-03-02T13:03:35Z-
dc.date.available2016-10-25T21:33:06Z-
dc.date.issued2014-
dc.identifierhttp://dx.doi.org/10.2174/18779468113036660030-
dc.identifier.citationCurrent Physical Chemistry, v. 4, n. 1, p. 15-20, 2014.-
dc.identifier.issn1877-9468-
dc.identifier.urihttp://hdl.handle.net/11449/135625-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/135625-
dc.description.abstractWe have used the periodic quantum-mechanical method with density functional theory at the B3LYP hybrid functional level in order to study the doping of SnO2 with pentavalent Sb5+. The 72-atom 2x3x2 supercell SnO2 (Sn24O48) was employed in the calculations. For the SnO2:4%Sb , one atom of Sn was replaced by one Sb atom. For the SnO2:8%Sb, two atoms of Sn were replaced by two Sb atoms. The Sb doping leads to an enhancement in the electrical conductivity of this material, because these ions substitute Sn4+ in the SnO2 matrix, leading to an electronic density rise in the conduction band, due to the donor-like behavior of the doping atom. This result shows that the bandgap magnitude depends on the doping concentration, because the energy value found for SnO2:4%Sb was 2.8eV whereas for SnO2:8%Sb it was 2.7eV. It was also verified that the difference between the Fermi level and the bottom of the conduction band is directly related to the doping concentration. - See more at: http://www.eurekaselect.com/117255/article#sthash.Z5ezhCQD.dpufen
dc.format.extent15-20-
dc.language.isoeng-
dc.sourceCurrículo Lattes-
dc.subjectBandgapen
dc.subjectDFTen
dc.subjectFermi Levelen
dc.subjectt in dioxideen
dc.titleA theoretical analysis of Sb5+ incorporation in highly doped SnO2 matrixen
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationUniversidade Estadual Paulista Júlio de Mesquita Filho, Departamento de Matemática, Faculdade de Ciências de Bauru, Bauru, AV. Luis Edmundo Carrijo Coube s/n, Vargem Limpa, CEP 17033360, SP, Brasil|Universidade Estadual Paulista Júlio de Mesquita Filho, Departamento de física, Faculdade de Ciências de Bauru, Bauru, AV. Luis Edmundo Carrijo Coube s/n, Vargem Limpa, CEP 17033360, SP, Brasil-
dc.description.affiliationUnespUniversidade Estadual Paulista Júlio de Mesquita Filho, Departamento de Matemática, Faculdade de Ciências de Bauru, Bauru, AV. Luis Edmundo Carrijo Coube s/n, Vargem Limpa, CEP 17033360, SP, Brasil|Universidade Estadual Paulista Júlio de Mesquita Filho, Departamento de física, Faculdade de Ciências de Bauru, Bauru, AV. Luis Edmundo Carrijo Coube s/n, Vargem Limpa, CEP 17033360, SP, Brasil-
dc.identifier.doi10.2174/18779468113036660030-
dc.rights.accessRightsAcesso restrito-
dc.relation.ispartofCurrent Physical Chemistry-
dc.identifier.lattes6284168579617066-
Appears in Collections:Artigos, TCCs, Teses e Dissertações da Unesp

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