Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity

Detalhes bibliográficos
Autor(a) principal: VICTOR NOCRATO MOURA
Data de Publicação: 2017
Tipo de documento: Dissertação
Idioma: por
Título da fonte: Biblioteca Digital de Teses e Dissertações da UFC
Texto Completo: http://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=19046
Resumo: In recent years, several experiments have been reported in which interface superconductivity was observed in heterostructures of different materials, inclunding non-superconductors. The origin of this superconductivity has not yet been elucidated and there is no well-established theory to explain this phenomenon. In 2015 a model based on the Ginzburg-Landau theory was proposed that would explain the interface superconductivity phenomenon assuming a system with two order parameters. It has been proposed that the order parameter characterizing the bulk material with a defective or doped layer permits the formation of a second parameter which competes with the former and prevails over it in the vicinity of the interface. The superconductivity at the interface is then explained by the growth of this second order parameter only in this region, remaining still ``hidden" inside the bulk. The model was applied to a one-dimensional system with an interface, which presented a surprising result: the ``hidden" superconductivity appers in quantized critical temperatures, this allowing the existence of several eigenstates of the system, with different critical temperatures. In this dissertation, we use this model and investigate the unfolding of hidden superconductivity and its quantized temperatures. We observe that the interfaces resemble one-dimensional quantum wells, with the critical temperature playing the role of the energy in the quantum case. Following this idea we use numerical methods to solve the Ginzburg-Landau equations for a system with an arbitrary number of parallel interfaces. Our results show that in this case, the critical temperatures are quantized and degenerate when the interfaces are very separated, but it has its degeneracy broken when we approach the interfaces, as it happens in a lattice of square wells. We then proposed a tight-binding model to estimate critical temperatures on parallel interfaces and verified the validity of this approximation through the numerical solution of the complete problem. We also analyze the vortex states for a square two-dimensional defect, verifying the possibility of creating or destroying vortices in the region of `` hidden" superconductivity through an external magnetic field.
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spelling info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/masterThesisGinzbutrg-Landau theory with hidden order parameter applied to interface superconductivityTEORIA DE GINZBURG-LANDAU COM PARÃMETRO DE ORDEM ESCONDIDO APLICADA AO ESTUDO DA SUPERCONDUTIVIDADE DE INTERFACE2017-02-21Andrey Chaves0061931730204931812376VICTOR NOCRATO MOURAUniversidade Federal do CearÃPrograma de PÃs-GraduaÃÃo em FÃsicaUFCBR teoria de Ginzburg-Landau supercondutividade de interface temperatura crÃtica. teoria de Ginzburg-Landau supercondutividade de interface temperatura crÃtica.Ginzburg-Landau Theory interface superconductivity critical temperatureGinzburg-Landau Theory interface superconductivity critical temperatureFISICA DA MATERIA CONDENSADAFISICA DA MATERIA CONDENSADAIn recent years, several experiments have been reported in which interface superconductivity was observed in heterostructures of different materials, inclunding non-superconductors. The origin of this superconductivity has not yet been elucidated and there is no well-established theory to explain this phenomenon. In 2015 a model based on the Ginzburg-Landau theory was proposed that would explain the interface superconductivity phenomenon assuming a system with two order parameters. It has been proposed that the order parameter characterizing the bulk material with a defective or doped layer permits the formation of a second parameter which competes with the former and prevails over it in the vicinity of the interface. The superconductivity at the interface is then explained by the growth of this second order parameter only in this region, remaining still ``hidden" inside the bulk. The model was applied to a one-dimensional system with an interface, which presented a surprising result: the ``hidden" superconductivity appers in quantized critical temperatures, this allowing the existence of several eigenstates of the system, with different critical temperatures. In this dissertation, we use this model and investigate the unfolding of hidden superconductivity and its quantized temperatures. We observe that the interfaces resemble one-dimensional quantum wells, with the critical temperature playing the role of the energy in the quantum case. Following this idea we use numerical methods to solve the Ginzburg-Landau equations for a system with an arbitrary number of parallel interfaces. Our results show that in this case, the critical temperatures are quantized and degenerate when the interfaces are very separated, but it has its degeneracy broken when we approach the interfaces, as it happens in a lattice of square wells. We then proposed a tight-binding model to estimate critical temperatures on parallel interfaces and verified the validity of this approximation through the numerical solution of the complete problem. We also analyze the vortex states for a square two-dimensional defect, verifying the possibility of creating or destroying vortices in the region of `` hidden" superconductivity through an external magnetic field.Nos Ãltimos anos foram reportados diversos experimentos em que a supercondutividade de interface foi observada em heteroestruturas de diferentes materiais, inclusive em nÃo-supercondutores extit{a priori}. A origem dessa supercondutividade ainda nÃo foi elucidada e nÃo existe uma teoria bem estabelecida para explicar esse fenÃmeno. Em 2015 foi proposto um modelo com base na teoria de Ginzburg-Landau que explicaria o fenÃmeno de supercondutividade de interface assumindo um sistema com dois parÃmetros de ordem. Foi proposto que o parÃmetro de ordem que caracteriza o material extit{bulk} com uma camada defeituosa, ou dopada, permite a formaÃÃo de um segundo parÃmetro que compete com o primeiro e prevalece sobre ele nas proximidades da interface. A supercondutividade na interface à entÃo explicada pelo crescimento deste segundo parÃmetro de ordem apenas nesta regiÃo, permancecendo ainda ``escondido" dentro do extit{bulk}. O modelo foi aplicado para um sistema unidimensional com uma interface, apresentando um resultado surpreendente: a supercondutividade escondida aparece em temperaturas crÃticas quantizadas, podendo entÃo existir vÃrios autoestados do sistema, com diferentes temperaturas crÃticas. Nessa dissertaÃÃo utilizamos esse modelo e investigamos os desdobramentos da supercondutividade escondida e suas temperaturas quantizadas. Percebemos que as interfaces assemelham-se com poÃos quÃnticos unidimensionais, com a temperatura crÃtica fazendo o anÃlogo ao da energia no caso quÃntico. Seguindo essa ideia utilizamos mÃtodos numÃricos para resolver as equaÃÃes de Ginzburg-Landau para um sistema com um nÃmero arbitrÃrio de interface paralelas. Nossos resultados mostram que neste caso, as temperaturas crÃticas, alÃm de quantizadas, sÃo degeneradas quando as interfaces estÃo muito separadas, mas tem essa degenerescÃncia quebrada quando aproximamos as interfaces, como ocorre em uma rede de poÃos quadrados. Propusemos entÃo um modelo tipo extit{tight-binding} para estimar temperaturas crÃticas em interfaces paralelas e verificamos a validade dessa aproximaÃÃo atravÃs da soluÃÃo numÃrica do problema completo. Analisamos tambÃm os estados de vÃrtices para um defeito bidimensional quadrado, verificando a possibilidade de se criar ou destruir vÃrtices na regiÃo de supercondutividade escondida atravÃs de um campo magnÃtico externo.Conselho Nacional de Desenvolvimento CientÃfico e TecnolÃgicohttp://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=19046application/pdfinfo:eu-repo/semantics/openAccessporreponame:Biblioteca Digital de Teses e Dissertações da UFCinstname:Universidade Federal do Cearáinstacron:UFC2019-01-21T11:31:49Zmail@mail.com -
dc.title.en.fl_str_mv Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
dc.title.alternative.pt.fl_str_mv TEORIA DE GINZBURG-LANDAU COM PARÃMETRO DE ORDEM ESCONDIDO APLICADA AO ESTUDO DA SUPERCONDUTIVIDADE DE INTERFACE
title Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
spellingShingle Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
VICTOR NOCRATO MOURA
teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
Ginzburg-Landau Theory
interface superconductivity
critical temperature
Ginzburg-Landau Theory
interface superconductivity
critical temperature
FISICA DA MATERIA CONDENSADA
FISICA DA MATERIA CONDENSADA
title_short Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
title_full Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
title_fullStr Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
title_full_unstemmed Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
title_sort Ginzbutrg-Landau theory with hidden order parameter applied to interface superconductivity
author VICTOR NOCRATO MOURA
author_facet VICTOR NOCRATO MOURA
author_role author
dc.contributor.advisor1.fl_str_mv Andrey Chaves
dc.contributor.advisor1ID.fl_str_mv 00619317302
dc.contributor.authorID.fl_str_mv 04931812376
dc.contributor.author.fl_str_mv VICTOR NOCRATO MOURA
contributor_str_mv Andrey Chaves
dc.subject.por.fl_str_mv teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
topic teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
teoria de Ginzburg-Landau
supercondutividade de interface
temperatura crÃtica.
Ginzburg-Landau Theory
interface superconductivity
critical temperature
Ginzburg-Landau Theory
interface superconductivity
critical temperature
FISICA DA MATERIA CONDENSADA
FISICA DA MATERIA CONDENSADA
dc.subject.eng.fl_str_mv Ginzburg-Landau Theory
interface superconductivity
critical temperature
Ginzburg-Landau Theory
interface superconductivity
critical temperature
dc.subject.cnpq.fl_str_mv FISICA DA MATERIA CONDENSADA
FISICA DA MATERIA CONDENSADA
dc.description.sponsorship.fl_txt_mv Conselho Nacional de Desenvolvimento CientÃfico e TecnolÃgico
dc.description.abstract.por.fl_txt_mv In recent years, several experiments have been reported in which interface superconductivity was observed in heterostructures of different materials, inclunding non-superconductors. The origin of this superconductivity has not yet been elucidated and there is no well-established theory to explain this phenomenon. In 2015 a model based on the Ginzburg-Landau theory was proposed that would explain the interface superconductivity phenomenon assuming a system with two order parameters. It has been proposed that the order parameter characterizing the bulk material with a defective or doped layer permits the formation of a second parameter which competes with the former and prevails over it in the vicinity of the interface. The superconductivity at the interface is then explained by the growth of this second order parameter only in this region, remaining still ``hidden" inside the bulk. The model was applied to a one-dimensional system with an interface, which presented a surprising result: the ``hidden" superconductivity appers in quantized critical temperatures, this allowing the existence of several eigenstates of the system, with different critical temperatures. In this dissertation, we use this model and investigate the unfolding of hidden superconductivity and its quantized temperatures. We observe that the interfaces resemble one-dimensional quantum wells, with the critical temperature playing the role of the energy in the quantum case. Following this idea we use numerical methods to solve the Ginzburg-Landau equations for a system with an arbitrary number of parallel interfaces. Our results show that in this case, the critical temperatures are quantized and degenerate when the interfaces are very separated, but it has its degeneracy broken when we approach the interfaces, as it happens in a lattice of square wells. We then proposed a tight-binding model to estimate critical temperatures on parallel interfaces and verified the validity of this approximation through the numerical solution of the complete problem. We also analyze the vortex states for a square two-dimensional defect, verifying the possibility of creating or destroying vortices in the region of `` hidden" superconductivity through an external magnetic field.
Nos Ãltimos anos foram reportados diversos experimentos em que a supercondutividade de interface foi observada em heteroestruturas de diferentes materiais, inclusive em nÃo-supercondutores extit{a priori}. A origem dessa supercondutividade ainda nÃo foi elucidada e nÃo existe uma teoria bem estabelecida para explicar esse fenÃmeno. Em 2015 foi proposto um modelo com base na teoria de Ginzburg-Landau que explicaria o fenÃmeno de supercondutividade de interface assumindo um sistema com dois parÃmetros de ordem. Foi proposto que o parÃmetro de ordem que caracteriza o material extit{bulk} com uma camada defeituosa, ou dopada, permite a formaÃÃo de um segundo parÃmetro que compete com o primeiro e prevalece sobre ele nas proximidades da interface. A supercondutividade na interface à entÃo explicada pelo crescimento deste segundo parÃmetro de ordem apenas nesta regiÃo, permancecendo ainda ``escondido" dentro do extit{bulk}. O modelo foi aplicado para um sistema unidimensional com uma interface, apresentando um resultado surpreendente: a supercondutividade escondida aparece em temperaturas crÃticas quantizadas, podendo entÃo existir vÃrios autoestados do sistema, com diferentes temperaturas crÃticas. Nessa dissertaÃÃo utilizamos esse modelo e investigamos os desdobramentos da supercondutividade escondida e suas temperaturas quantizadas. Percebemos que as interfaces assemelham-se com poÃos quÃnticos unidimensionais, com a temperatura crÃtica fazendo o anÃlogo ao da energia no caso quÃntico. Seguindo essa ideia utilizamos mÃtodos numÃricos para resolver as equaÃÃes de Ginzburg-Landau para um sistema com um nÃmero arbitrÃrio de interface paralelas. Nossos resultados mostram que neste caso, as temperaturas crÃticas, alÃm de quantizadas, sÃo degeneradas quando as interfaces estÃo muito separadas, mas tem essa degenerescÃncia quebrada quando aproximamos as interfaces, como ocorre em uma rede de poÃos quadrados. Propusemos entÃo um modelo tipo extit{tight-binding} para estimar temperaturas crÃticas em interfaces paralelas e verificamos a validade dessa aproximaÃÃo atravÃs da soluÃÃo numÃrica do problema completo. Analisamos tambÃm os estados de vÃrtices para um defeito bidimensional quadrado, verificando a possibilidade de se criar ou destruir vÃrtices na regiÃo de supercondutividade escondida atravÃs de um campo magnÃtico externo.
description In recent years, several experiments have been reported in which interface superconductivity was observed in heterostructures of different materials, inclunding non-superconductors. The origin of this superconductivity has not yet been elucidated and there is no well-established theory to explain this phenomenon. In 2015 a model based on the Ginzburg-Landau theory was proposed that would explain the interface superconductivity phenomenon assuming a system with two order parameters. It has been proposed that the order parameter characterizing the bulk material with a defective or doped layer permits the formation of a second parameter which competes with the former and prevails over it in the vicinity of the interface. The superconductivity at the interface is then explained by the growth of this second order parameter only in this region, remaining still ``hidden" inside the bulk. The model was applied to a one-dimensional system with an interface, which presented a surprising result: the ``hidden" superconductivity appers in quantized critical temperatures, this allowing the existence of several eigenstates of the system, with different critical temperatures. In this dissertation, we use this model and investigate the unfolding of hidden superconductivity and its quantized temperatures. We observe that the interfaces resemble one-dimensional quantum wells, with the critical temperature playing the role of the energy in the quantum case. Following this idea we use numerical methods to solve the Ginzburg-Landau equations for a system with an arbitrary number of parallel interfaces. Our results show that in this case, the critical temperatures are quantized and degenerate when the interfaces are very separated, but it has its degeneracy broken when we approach the interfaces, as it happens in a lattice of square wells. We then proposed a tight-binding model to estimate critical temperatures on parallel interfaces and verified the validity of this approximation through the numerical solution of the complete problem. We also analyze the vortex states for a square two-dimensional defect, verifying the possibility of creating or destroying vortices in the region of `` hidden" superconductivity through an external magnetic field.
publishDate 2017
dc.date.issued.fl_str_mv 2017-02-21
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dc.publisher.program.fl_str_mv Programa de PÃs-GraduaÃÃo em FÃsica
dc.publisher.initials.fl_str_mv UFC
dc.publisher.country.fl_str_mv BR
publisher.none.fl_str_mv Universidade Federal do CearÃ
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