Modelagem de nanotubos de nitreto de gálio
| Ano de defesa: | 2016 |
|---|---|
| Autor(a) principal: | |
| Orientador(a): | |
| Banca de defesa: | , |
| Tipo de documento: | Dissertação |
| Tipo de acesso: | Acesso aberto |
| Idioma: | por |
| Instituição de defesa: |
Universidade Estadual de Goiás
|
| Programa de Pós-Graduação: |
Programa de Pós-Graduação Stricto sensu em Ciências Moleculares
|
| Departamento: |
UEG ::Coordenação de Mestrado Ciências Moleculares
|
| País: |
Brasil
|
| Palavras-chave em Português: | |
| Palavras-chave em Inglês: | |
| Área do conhecimento CNPq: | |
| Link de acesso: | http://www.bdtd.ueg.br/handle/tede/287 |
Resumo: | Nanotubes can be classified with respect to their symmetry in chiral and achiral (armchair and zigzag). Several methods have been used to nanotubes synthesis, thus it is expected that the structures obtained have different structural characteristics (diameter, length and wall thickness). In this work we studied single wall gallium nitride nanotubes, the models were obtained through winding a plane of atoms, using algorithms written in Shell Bash programming language for Linux. Two methods were used to generate the planes of gallium nitride. The first is based on graphene structure, where Ga and N atoms replaced the carbon atoms. The second is based on the plane (0001) of hexagonal phase from gallium nitride crystal (wurtzite). The optimization of atoms coordinates was made using the PM7 semiempirical method. It was observed that after optimization there was a small distortion at the edges of models to compensate the effects of free valences, reducing the Ga-N bond distance. The optimized coordinates were collected and used in ab initio calculations, Hartree-Fock (RHF) and Density Functional Theory (B3LYP) with the basis sets 3-21G, 6-31G, 6-31G(d, p) and 6-311G. The energy difference |HOMO-LUMO| was calculated, revealing that tis property is strongly linked to the geometry of the unsaturated nanotubes. Analyzing the density of states and the orbital contributions it was found that the achiral models show similar bands, however some orbitals between HOMO and LUMO decrease the band distance, for zigzag models. The Mulliken charges distribution and dipole moments have shown that the armchair structures are non-polar, while the zigzag structures are polar. |
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Santos, José Divino doshttp://lattes.cnpq.br/2279900314020119Rosseto, RenatoVargas, Marcos dos Reishttp://lattes.cnpq.br/4458336046440816Sodré, Johnathan Mendes2020-04-07T16:00:07Z2016-02-26SOBRÉ, Johnathan Mendes. Modelagem de nanotubos de nitreto de gálio. 2016. 144 f. Dissertação (Mestrado em Ciências Moleculares) - Câmpus Central - Sede: Anápolis - CET, Universidade Estadual de Goiás, Anápolis.http://www.bdtd.ueg.br/handle/tede/287Nanotubes can be classified with respect to their symmetry in chiral and achiral (armchair and zigzag). Several methods have been used to nanotubes synthesis, thus it is expected that the structures obtained have different structural characteristics (diameter, length and wall thickness). In this work we studied single wall gallium nitride nanotubes, the models were obtained through winding a plane of atoms, using algorithms written in Shell Bash programming language for Linux. Two methods were used to generate the planes of gallium nitride. The first is based on graphene structure, where Ga and N atoms replaced the carbon atoms. The second is based on the plane (0001) of hexagonal phase from gallium nitride crystal (wurtzite). The optimization of atoms coordinates was made using the PM7 semiempirical method. It was observed that after optimization there was a small distortion at the edges of models to compensate the effects of free valences, reducing the Ga-N bond distance. The optimized coordinates were collected and used in ab initio calculations, Hartree-Fock (RHF) and Density Functional Theory (B3LYP) with the basis sets 3-21G, 6-31G, 6-31G(d, p) and 6-311G. The energy difference |HOMO-LUMO| was calculated, revealing that tis property is strongly linked to the geometry of the unsaturated nanotubes. Analyzing the density of states and the orbital contributions it was found that the achiral models show similar bands, however some orbitals between HOMO and LUMO decrease the band distance, for zigzag models. The Mulliken charges distribution and dipole moments have shown that the armchair structures are non-polar, while the zigzag structures are polar.Os nanotubos podem ser classificados com relação a sua simetria em quirais e aquirais (armchair e zigzag). Diversas metodologias vêm sendo utilizadas para a síntese de nanotubos, logo, espera-se que as estruturas obtidas apresentem diferentes características estruturais (diâmetro, comprimento e espessura da parede). Neste trabalho foram estudados os nanotubos de nitreto de gálio de parede simples, os modelos foram obtidos através do enrolamento de um plano de átomos, utilizando algoritmos escritos em linguagem de programação Shell Bash do Linux. Foram utilizadas duas metodologias para gerar os planos de nitreto de gálio. A primeira baseia-se na estrutura do grafeno, onde os átomos de Ga e N substituíram os átomos de C, a segunda baseia-se no plano (0001) do cristal de GaN na fase hexagonal (wurtzita). A partir das coordenadas dos átomos foi feita a otimização dos modelos utilizando o método semi-empírico PM7. Observou-se que após a otimização houve uma pequena distorção nas extremidades dos modelos para compensar os efeitos das valências livres, reduzindo a distância de ligação Ga-N. As coordenadas otimizadas foram coletadas e utilizadas nos cálculos ab initio, Hartree-Fock (RHF) e Teoria do Funcional da Densidade (B3LYP) com os conjuntos de base 3-21G, 6-31G, 6-31G(d,p) e 6-311G. A diferença de energia |HOMO-LUMO| foi calculada, sendo possível observar que esta propriedade está fortemente ligada a geometria dos nanotubos insaturados. Analisando a densidade de estados e as contribuições orbitais verificou-se que os modelos aquirais apresentam bandas similares, porém alguns orbitais entre as regiões do HOMO e do LUMO reduz a distância entre as bandas, para os modelos zigzag. As distribuições das cargas de Mulliken e os momentos de dipolo demostraram que as estruturas armchair são apolares, enquanto que as estruturas zigzag são polares, para os modelos obtidos pelas duas metodologias.Submitted by Sandra Barbosa (sandrabarbosa632@gmail.com) on 2020-04-07T12:33:04Z No. of bitstreams: 2 license.txt: 2138 bytes, checksum: 77209788b6548b0520e61e670bd90d68 (MD5) Johnathan_Mendes_Sodre.pdf: 7218507 bytes, checksum: df5c936d2b5cd8c7a38552008603cfd5 (MD5)Approved for entry into archive by Sandra Barbosa (sandrabarbosa632@gmail.com) on 2020-04-07T16:00:07Z (GMT) No. of bitstreams: 2 license.txt: 2138 bytes, checksum: 77209788b6548b0520e61e670bd90d68 (MD5) Johnathan_Mendes_Sodre.pdf: 7218507 bytes, checksum: df5c936d2b5cd8c7a38552008603cfd5 (MD5)Made available in DSpace on 2020-04-07T16:00:07Z (GMT). No. of bitstreams: 2 license.txt: 2138 bytes, checksum: 77209788b6548b0520e61e670bd90d68 (MD5) Johnathan_Mendes_Sodre.pdf: 7218507 bytes, checksum: df5c936d2b5cd8c7a38552008603cfd5 (MD5) Previous issue date: 2016-02-26application/pdfporUniversidade Estadual de GoiásPrograma de Pós-Graduação Stricto sensu em Ciências MolecularesUEGBrasilUEG ::Coordenação de Mestrado Ciências MolecularesNitreto de GálioNanotubosQuímica teóricaPropriedades eletrônicasMétodos mecânico-quânticosNanotubesGallium nitrideTheoretical chemistryElectronic propertiesQuantum mechanic methodsQUIMICA::FISICO-QUIMICAModelagem de nanotubos de nitreto de gálioinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/masterThesis-8570043875938568561500500600-8026445747564223438-6794069463227071484info:eu-repo/semantics/openAccessreponame:Biblioteca Digital Brasileira de Teses e Dissertações da UEGinstname:Universidade Estadual de Goiás (UEG)instacron:UEGORIGINALJohnathan_Mendes_Sodre.pdfJohnathan_Mendes_Sodre.pdfapplication/pdf7218507http://10.20.60.80:8080/tede/bitstream/tede/287/2/Johnathan_Mendes_Sodre.pdfdf5c936d2b5cd8c7a38552008603cfd5MD52LICENSElicense.txtlicense.txttext/plain; charset=utf-82138http://10.20.60.80:8080/tede/bitstream/tede/287/1/license.txt77209788b6548b0520e61e670bd90d68MD51tede/2872020-12-02 15:42:59.578oai:tede2: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Biblioteca Digital de Teses e Dissertaçõeshttps://www.bdtd.ueg.br/PUBhttps://www.bdtd.ueg.br/oai/requestbibliotecaunucet@ueg.br||opendoar:2020-12-02T18:42:59Biblioteca Digital Brasileira de Teses e Dissertações da UEG - Universidade Estadual de Goiás (UEG)false |
| dc.title.por.fl_str_mv |
Modelagem de nanotubos de nitreto de gálio |
| title |
Modelagem de nanotubos de nitreto de gálio |
| spellingShingle |
Modelagem de nanotubos de nitreto de gálio Sodré, Johnathan Mendes Nitreto de Gálio Nanotubos Química teórica Propriedades eletrônicas Métodos mecânico-quânticos Nanotubes Gallium nitride Theoretical chemistry Electronic properties Quantum mechanic methods QUIMICA::FISICO-QUIMICA |
| title_short |
Modelagem de nanotubos de nitreto de gálio |
| title_full |
Modelagem de nanotubos de nitreto de gálio |
| title_fullStr |
Modelagem de nanotubos de nitreto de gálio |
| title_full_unstemmed |
Modelagem de nanotubos de nitreto de gálio |
| title_sort |
Modelagem de nanotubos de nitreto de gálio |
| author |
Sodré, Johnathan Mendes |
| author_facet |
Sodré, Johnathan Mendes |
| author_role |
author |
| dc.contributor.advisor1.fl_str_mv |
Santos, José Divino dos |
| dc.contributor.advisor1Lattes.fl_str_mv |
http://lattes.cnpq.br/2279900314020119 |
| dc.contributor.referee1.fl_str_mv |
Rosseto, Renato |
| dc.contributor.referee2.fl_str_mv |
Vargas, Marcos dos Reis |
| dc.contributor.authorLattes.fl_str_mv |
http://lattes.cnpq.br/4458336046440816 |
| dc.contributor.author.fl_str_mv |
Sodré, Johnathan Mendes |
| contributor_str_mv |
Santos, José Divino dos Rosseto, Renato Vargas, Marcos dos Reis |
| dc.subject.por.fl_str_mv |
Nitreto de Gálio Nanotubos Química teórica Propriedades eletrônicas Métodos mecânico-quânticos |
| topic |
Nitreto de Gálio Nanotubos Química teórica Propriedades eletrônicas Métodos mecânico-quânticos Nanotubes Gallium nitride Theoretical chemistry Electronic properties Quantum mechanic methods QUIMICA::FISICO-QUIMICA |
| dc.subject.eng.fl_str_mv |
Nanotubes Gallium nitride Theoretical chemistry Electronic properties Quantum mechanic methods |
| dc.subject.cnpq.fl_str_mv |
QUIMICA::FISICO-QUIMICA |
| description |
Nanotubes can be classified with respect to their symmetry in chiral and achiral (armchair and zigzag). Several methods have been used to nanotubes synthesis, thus it is expected that the structures obtained have different structural characteristics (diameter, length and wall thickness). In this work we studied single wall gallium nitride nanotubes, the models were obtained through winding a plane of atoms, using algorithms written in Shell Bash programming language for Linux. Two methods were used to generate the planes of gallium nitride. The first is based on graphene structure, where Ga and N atoms replaced the carbon atoms. The second is based on the plane (0001) of hexagonal phase from gallium nitride crystal (wurtzite). The optimization of atoms coordinates was made using the PM7 semiempirical method. It was observed that after optimization there was a small distortion at the edges of models to compensate the effects of free valences, reducing the Ga-N bond distance. The optimized coordinates were collected and used in ab initio calculations, Hartree-Fock (RHF) and Density Functional Theory (B3LYP) with the basis sets 3-21G, 6-31G, 6-31G(d, p) and 6-311G. The energy difference |HOMO-LUMO| was calculated, revealing that tis property is strongly linked to the geometry of the unsaturated nanotubes. Analyzing the density of states and the orbital contributions it was found that the achiral models show similar bands, however some orbitals between HOMO and LUMO decrease the band distance, for zigzag models. The Mulliken charges distribution and dipole moments have shown that the armchair structures are non-polar, while the zigzag structures are polar. |
| publishDate |
2016 |
| dc.date.issued.fl_str_mv |
2016-02-26 |
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2020-04-07T16:00:07Z |
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info:eu-repo/semantics/publishedVersion |
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info:eu-repo/semantics/masterThesis |
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masterThesis |
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publishedVersion |
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SOBRÉ, Johnathan Mendes. Modelagem de nanotubos de nitreto de gálio. 2016. 144 f. Dissertação (Mestrado em Ciências Moleculares) - Câmpus Central - Sede: Anápolis - CET, Universidade Estadual de Goiás, Anápolis. |
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http://www.bdtd.ueg.br/handle/tede/287 |
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SOBRÉ, Johnathan Mendes. Modelagem de nanotubos de nitreto de gálio. 2016. 144 f. Dissertação (Mestrado em Ciências Moleculares) - Câmpus Central - Sede: Anápolis - CET, Universidade Estadual de Goiás, Anápolis. |
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por |
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