The structure of the bulk and the (001) surface of V2O5: a DFT+U study
- Autores
- Ranea, Víctor Alejandro; Dammig Quiña, Pablo Leandro
- Año de publicación
- 2016
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- GGA(PW91)+U is applied to the calculation of the structure (lattice parameters) and the electronic structure of theV2O5 bulk and its (001) surface for different values of U eff used in the literature (0.0, 3.0 and 6.6 eV). Similar surface lattice parameters are calculated for the (001) surface and for the bulk, as well as similar electronic structures. The calculated lattice parameters (a and b for the surface and a, b and c for the bulk) are in good agreement with experimental results. It seems that there is no strong correlation between the calculated lattice parameters and the value of Ueff. The calculated width of the valence band keeps the value of 5 eVfor the three studied Ueff. However, the energy gap between the valence and the conduction bands increases with the value of Ueff. Ueff=3.0 eV seems to be the most adequate value to describe the energy gap after comparison with experimental results. Electronic density contour plots indicate that for a larger (smaller) Ueff the accumulated charge in the V-O(1) bond is overestimated (underestimated). The contour plots (in the a direction) show that the charge distribution V-O(3) is less correlated with Ueff than the charge distribution V-O(1), where as charge distribution V-O(2) seems not to be corretaled with Ueff. The energy gap between the valence and the conduction bands seems to be strongly related with the charge distribution in the V-O(1) bond. The V-O(1) bond stability seems to be correlated with U eff. However, the stability of the V-O(2) and V-O (3) bonds seems not to be strongly affected by U eff.
Instituto de Investigaciones Fisicoquímicas Teóricas y Aplicadas - Materia
-
Química
Density functional theory
Divanadium pentoxide surface
Electronic structure
Energy gap
Lattice constants - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by-nc-sa/4.0/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/100417
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The structure of the bulk and the (001) surface of V2O5: a DFT+U studyRanea, Víctor AlejandroDammig Quiña, Pablo LeandroQuímicaDensity functional theoryDivanadium pentoxide surfaceElectronic structureEnergy gapLattice constantsGGA(PW91)+U is applied to the calculation of the structure (lattice parameters) and the electronic structure of theV<sub>2</sub>O<sub>5</sub> bulk and its (001) surface for different values of U <sub>eff</sub> used in the literature (0.0, 3.0 and 6.6 eV). Similar surface lattice parameters are calculated for the (001) surface and for the bulk, as well as similar electronic structures. The calculated lattice parameters (a and b for the surface and a, b and c for the bulk) are in good agreement with experimental results. It seems that there is no strong correlation between the calculated lattice parameters and the value of U<sub>eff</sub>. The calculated width of the valence band keeps the value of 5 eVfor the three studied U<sub>eff</sub>. However, the energy gap between the valence and the conduction bands increases with the value of U<sub>eff</sub>. U<sub>eff</sub>=3.0 eV seems to be the most adequate value to describe the energy gap after comparison with experimental results. Electronic density contour plots indicate that for a larger (smaller) U<sub>eff</sub> the accumulated charge in the V-O(1) bond is overestimated (underestimated). The contour plots (in the a direction) show that the charge distribution V-O(3) is less correlated with U<sub>eff</sub> than the charge distribution V-O(1), where as charge distribution V-O(2) seems not to be corretaled with U<sub>eff</sub>. The energy gap between the valence and the conduction bands seems to be strongly related with the charge distribution in the V-O(1) bond. The V-O(1) bond stability seems to be correlated with U <sub>eff</sub>. However, the stability of the V-O(2) and V-O (3) bonds seems not to be strongly affected by U <sub>eff</sub>.Instituto de Investigaciones Fisicoquímicas Teóricas y Aplicadas2016-08info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf8500501-8500511http://sedici.unlp.edu.ar/handle/10915/100417enginfo:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/62297info:eu-repo/semantics/altIdentifier/url/http://iopscience.iop.org/article/10.1088/2053-1591/3/8/085005/metainfo:eu-repo/semantics/altIdentifier/issn/2053-1591info:eu-repo/semantics/altIdentifier/doi/10.1088/2053-1591/3/8/085005info:eu-repo/semantics/altIdentifier/hdl/11336/62297info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/4.0/Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-10-15T11:12:10Zoai:sedici.unlp.edu.ar:10915/100417Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-10-15 11:12:10.417SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
title |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
spellingShingle |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study Ranea, Víctor Alejandro Química Density functional theory Divanadium pentoxide surface Electronic structure Energy gap Lattice constants |
title_short |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
title_full |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
title_fullStr |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
title_full_unstemmed |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
title_sort |
The structure of the bulk and the (001) surface of V2O5: a DFT+U study |
dc.creator.none.fl_str_mv |
Ranea, Víctor Alejandro Dammig Quiña, Pablo Leandro |
author |
Ranea, Víctor Alejandro |
author_facet |
Ranea, Víctor Alejandro Dammig Quiña, Pablo Leandro |
author_role |
author |
author2 |
Dammig Quiña, Pablo Leandro |
author2_role |
author |
dc.subject.none.fl_str_mv |
Química Density functional theory Divanadium pentoxide surface Electronic structure Energy gap Lattice constants |
topic |
Química Density functional theory Divanadium pentoxide surface Electronic structure Energy gap Lattice constants |
dc.description.none.fl_txt_mv |
GGA(PW91)+U is applied to the calculation of the structure (lattice parameters) and the electronic structure of theV<sub>2</sub>O<sub>5</sub> bulk and its (001) surface for different values of U <sub>eff</sub> used in the literature (0.0, 3.0 and 6.6 eV). Similar surface lattice parameters are calculated for the (001) surface and for the bulk, as well as similar electronic structures. The calculated lattice parameters (a and b for the surface and a, b and c for the bulk) are in good agreement with experimental results. It seems that there is no strong correlation between the calculated lattice parameters and the value of U<sub>eff</sub>. The calculated width of the valence band keeps the value of 5 eVfor the three studied U<sub>eff</sub>. However, the energy gap between the valence and the conduction bands increases with the value of U<sub>eff</sub>. U<sub>eff</sub>=3.0 eV seems to be the most adequate value to describe the energy gap after comparison with experimental results. Electronic density contour plots indicate that for a larger (smaller) U<sub>eff</sub> the accumulated charge in the V-O(1) bond is overestimated (underestimated). The contour plots (in the a direction) show that the charge distribution V-O(3) is less correlated with U<sub>eff</sub> than the charge distribution V-O(1), where as charge distribution V-O(2) seems not to be corretaled with U<sub>eff</sub>. The energy gap between the valence and the conduction bands seems to be strongly related with the charge distribution in the V-O(1) bond. The V-O(1) bond stability seems to be correlated with U <sub>eff</sub>. However, the stability of the V-O(2) and V-O (3) bonds seems not to be strongly affected by U <sub>eff</sub>. Instituto de Investigaciones Fisicoquímicas Teóricas y Aplicadas |
description |
GGA(PW91)+U is applied to the calculation of the structure (lattice parameters) and the electronic structure of theV<sub>2</sub>O<sub>5</sub> bulk and its (001) surface for different values of U <sub>eff</sub> used in the literature (0.0, 3.0 and 6.6 eV). Similar surface lattice parameters are calculated for the (001) surface and for the bulk, as well as similar electronic structures. The calculated lattice parameters (a and b for the surface and a, b and c for the bulk) are in good agreement with experimental results. It seems that there is no strong correlation between the calculated lattice parameters and the value of U<sub>eff</sub>. The calculated width of the valence band keeps the value of 5 eVfor the three studied U<sub>eff</sub>. However, the energy gap between the valence and the conduction bands increases with the value of U<sub>eff</sub>. U<sub>eff</sub>=3.0 eV seems to be the most adequate value to describe the energy gap after comparison with experimental results. Electronic density contour plots indicate that for a larger (smaller) U<sub>eff</sub> the accumulated charge in the V-O(1) bond is overestimated (underestimated). The contour plots (in the a direction) show that the charge distribution V-O(3) is less correlated with U<sub>eff</sub> than the charge distribution V-O(1), where as charge distribution V-O(2) seems not to be corretaled with U<sub>eff</sub>. The energy gap between the valence and the conduction bands seems to be strongly related with the charge distribution in the V-O(1) bond. The V-O(1) bond stability seems to be correlated with U <sub>eff</sub>. However, the stability of the V-O(2) and V-O (3) bonds seems not to be strongly affected by U <sub>eff</sub>. |
publishDate |
2016 |
dc.date.none.fl_str_mv |
2016-08 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://sedici.unlp.edu.ar/handle/10915/100417 |
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http://sedici.unlp.edu.ar/handle/10915/100417 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/62297 info:eu-repo/semantics/altIdentifier/url/http://iopscience.iop.org/article/10.1088/2053-1591/3/8/085005/meta info:eu-repo/semantics/altIdentifier/issn/2053-1591 info:eu-repo/semantics/altIdentifier/doi/10.1088/2053-1591/3/8/085005 info:eu-repo/semantics/altIdentifier/hdl/11336/62297 |
dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) |
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openAccess |
rights_invalid_str_mv |
http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) |
dc.format.none.fl_str_mv |
application/pdf 8500501-8500511 |
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