On the phase transition for some percolation models in random environments

Detalhes bibliográficos
Ano de defesa: 2019
Autor(a) principal: Marcos Vinícius Araújo Sá lattes
Orientador(a): Remy de Paiva Sanchis lattes, Marcelo Richard Hilário
Banca de defesa: Augusto Quadros Teixeira, Glauco Valle da Silva Coelho, Hubert Lacoin, Paulo Cupertino de Lima
Tipo de documento: Tese
Tipo de acesso: Acesso aberto
Idioma: eng
Instituição de defesa: Universidade Federal de Minas Gerais
Programa de Pós-Graduação: Programa de Pós-Graduação em Matemática
Departamento: ICX - DEPARTAMENTO DE MATEMÁTICA
País: Brasil
Palavras-chave em Português:
Link de acesso: http://hdl.handle.net/1843/50999
Resumo: In this thesis we consider two percolation models in random environments and we are interested in their phase transition phenomenon. The first percolation model we study is defined on the cubic lattice featuring columnar disorder. This model is defined in two steps: first the vertical columns of $\mathbb{Z}^3$ are removed independently with probability $1-\rho$ and, in the second step, the bonds connecting sites in the remaining sub-lattice are declared open with probability $p$, independently. Our result shows that there exists $\delta>0$ such that $p_c(\rho)<1/2-\delta$ for any $\rho>\rho_c$, where $\rho_c$ denotes the critical point of site percolation in $\mathbb{Z}^2$. The second model is defined on a horizontally stretched square lattice, which is a generalized version of $\mathbb{Z}^2_+$ obtained by stretching the distances between its columns according to a positive random variable $\xi$. In this model the probability of a bond being declared open will decay exponentially according to its length. Our result shows the existence of a phase transition when $\mathbb{E}(\xi^\eta)<\infty$, for some $\eta>1$, and the absence of phase transition when $\mathbb{E}(\xi^\eta)=\infty$ for some $\eta<1$.
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spelling Remy de Paiva Sanchishttp://lattes.cnpq.br/1582551703060830Marcelo Richard HilárioAugusto Quadros TeixeiraGlauco Valle da Silva CoelhoHubert LacoinPaulo Cupertino de Limahttp://lattes.cnpq.br/0158987925235945Marcos Vinícius Araújo Sá2023-03-17T16:33:11Z2023-03-17T16:33:11Z2019-11-22http://hdl.handle.net/1843/50999In this thesis we consider two percolation models in random environments and we are interested in their phase transition phenomenon. The first percolation model we study is defined on the cubic lattice featuring columnar disorder. This model is defined in two steps: first the vertical columns of $\mathbb{Z}^3$ are removed independently with probability $1-\rho$ and, in the second step, the bonds connecting sites in the remaining sub-lattice are declared open with probability $p$, independently. Our result shows that there exists $\delta>0$ such that $p_c(\rho)<1/2-\delta$ for any $\rho>\rho_c$, where $\rho_c$ denotes the critical point of site percolation in $\mathbb{Z}^2$. The second model is defined on a horizontally stretched square lattice, which is a generalized version of $\mathbb{Z}^2_+$ obtained by stretching the distances between its columns according to a positive random variable $\xi$. In this model the probability of a bond being declared open will decay exponentially according to its length. Our result shows the existence of a phase transition when $\mathbb{E}(\xi^\eta)<\infty$, for some $\eta>1$, and the absence of phase transition when $\mathbb{E}(\xi^\eta)=\infty$ for some $\eta<1$.Nesta tese nós consideramos dois modelos de percolação em ambientes aleatórios e estamos interessados em seus fenômenos de transição de fase. O primeiro modelo de percolação estudado é na rede cúbica apresentando desordem colunar. Este modelo é definido em dois passos: primeiro as colunas verticais de $\mathbb{Z}^3$ são removidas independentemente com probabilidade $1-\rho$ e, no segundo passo, os elos conectando sítios na sub-rede remanescente são declarados abertos com probabilidade $p$ de modo independente. Nosso resultado mostra que existe $\delta>0$ tal que o ponto crítico $p_c(\rho)<1/2-\delta$ para todo $\rho>\rho_c$, onde $\rho_c$ denota o ponto crítico da percolação de sítios em $\mathbb{Z}^2$. O segundo modelo é na rede quadrada esticada horizontalmente, que consiste de uma versão generalizada de $\mathbb{Z}^2_+$ obtida ao se esticar a distância entre suas colunas, segundo uma variável aleatória positiva $\xi$. Neste modelo a probabilidade de um elo ser declarado aberto decairá exponencialmente segundo seu comprimento. Nosso resultado mostra a existência da transição de fase quando $\mathbb{E}(\xi^\eta)<\infty$, para algum $\eta>1$, e a ausência quando $\mathbb{E}(\xi^\eta)=\infty$, para algum $\eta<1$.CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível SuperiorengUniversidade Federal de Minas GeraisPrograma de Pós-Graduação em MatemáticaUFMGBrasilICX - DEPARTAMENTO DE MATEMÁTICAMatemática – TesesPercolação – TesesTransição de fase – TesesCampos aleatórios – TesesGrupo de renormalização– TesesPercolationPhase transitionRandom environmentsRenormalizationMultiscale analysisOn the phase transition for some percolation models in random environmentsA transição de fase para alguns modelos de percolação em ambientes aleatóriosinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisinfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFMGinstname:Universidade Federal de Minas Gerais (UFMG)instacron:UFMGORIGINALOn_the_phase_transition_for_some_percolation_models_in_random_environments.pdfOn_the_phase_transition_for_some_percolation_models_in_random_environments.pdfapplication/pdf889861https://repositorio.ufmg.br/bitstream/1843/50999/1/On_the_phase_transition_for_some_percolation_models_in_random_environments.pdf7802e4ae9c7f3ee83fa65be75d5407a4MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-82118https://repositorio.ufmg.br/bitstream/1843/50999/2/license.txtcda590c95a0b51b4d15f60c9642ca272MD521843/509992023-03-17 13:33:12.2oai:repositorio.ufmg.br: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ório de PublicaçõesPUBhttps://repositorio.ufmg.br/oaiopendoar:2023-03-17T16:33:12Repositório Institucional da UFMG - Universidade Federal de Minas Gerais (UFMG)false
dc.title.pt_BR.fl_str_mv On the phase transition for some percolation models in random environments
dc.title.alternative.pt_BR.fl_str_mv A transição de fase para alguns modelos de percolação em ambientes aleatórios
title On the phase transition for some percolation models in random environments
spellingShingle On the phase transition for some percolation models in random environments
Marcos Vinícius Araújo Sá
Percolation
Phase transition
Random environments
Renormalization
Multiscale analysis
Matemática – Teses
Percolação – Teses
Transição de fase – Teses
Campos aleatórios – Teses
Grupo de renormalização– Teses
title_short On the phase transition for some percolation models in random environments
title_full On the phase transition for some percolation models in random environments
title_fullStr On the phase transition for some percolation models in random environments
title_full_unstemmed On the phase transition for some percolation models in random environments
title_sort On the phase transition for some percolation models in random environments
author Marcos Vinícius Araújo Sá
author_facet Marcos Vinícius Araújo Sá
author_role author
dc.contributor.advisor1.fl_str_mv Remy de Paiva Sanchis
dc.contributor.advisor1Lattes.fl_str_mv http://lattes.cnpq.br/1582551703060830
dc.contributor.advisor2.fl_str_mv Marcelo Richard Hilário
dc.contributor.referee1.fl_str_mv Augusto Quadros Teixeira
dc.contributor.referee2.fl_str_mv Glauco Valle da Silva Coelho
dc.contributor.referee3.fl_str_mv Hubert Lacoin
dc.contributor.referee4.fl_str_mv Paulo Cupertino de Lima
dc.contributor.authorLattes.fl_str_mv http://lattes.cnpq.br/0158987925235945
dc.contributor.author.fl_str_mv Marcos Vinícius Araújo Sá
contributor_str_mv Remy de Paiva Sanchis
Marcelo Richard Hilário
Augusto Quadros Teixeira
Glauco Valle da Silva Coelho
Hubert Lacoin
Paulo Cupertino de Lima
dc.subject.por.fl_str_mv Percolation
Phase transition
Random environments
Renormalization
Multiscale analysis
topic Percolation
Phase transition
Random environments
Renormalization
Multiscale analysis
Matemática – Teses
Percolação – Teses
Transição de fase – Teses
Campos aleatórios – Teses
Grupo de renormalização– Teses
dc.subject.other.pt_BR.fl_str_mv Matemática – Teses
Percolação – Teses
Transição de fase – Teses
Campos aleatórios – Teses
Grupo de renormalização– Teses
description In this thesis we consider two percolation models in random environments and we are interested in their phase transition phenomenon. The first percolation model we study is defined on the cubic lattice featuring columnar disorder. This model is defined in two steps: first the vertical columns of $\mathbb{Z}^3$ are removed independently with probability $1-\rho$ and, in the second step, the bonds connecting sites in the remaining sub-lattice are declared open with probability $p$, independently. Our result shows that there exists $\delta>0$ such that $p_c(\rho)<1/2-\delta$ for any $\rho>\rho_c$, where $\rho_c$ denotes the critical point of site percolation in $\mathbb{Z}^2$. The second model is defined on a horizontally stretched square lattice, which is a generalized version of $\mathbb{Z}^2_+$ obtained by stretching the distances between its columns according to a positive random variable $\xi$. In this model the probability of a bond being declared open will decay exponentially according to its length. Our result shows the existence of a phase transition when $\mathbb{E}(\xi^\eta)<\infty$, for some $\eta>1$, and the absence of phase transition when $\mathbb{E}(\xi^\eta)=\infty$ for some $\eta<1$.
publishDate 2019
dc.date.issued.fl_str_mv 2019-11-22
dc.date.accessioned.fl_str_mv 2023-03-17T16:33:11Z
dc.date.available.fl_str_mv 2023-03-17T16:33:11Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/doctoralThesis
format doctoralThesis
status_str publishedVersion
dc.identifier.uri.fl_str_mv http://hdl.handle.net/1843/50999
url http://hdl.handle.net/1843/50999
dc.language.iso.fl_str_mv eng
language eng
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.publisher.none.fl_str_mv Universidade Federal de Minas Gerais
dc.publisher.program.fl_str_mv Programa de Pós-Graduação em Matemática
dc.publisher.initials.fl_str_mv UFMG
dc.publisher.country.fl_str_mv Brasil
dc.publisher.department.fl_str_mv ICX - DEPARTAMENTO DE MATEMÁTICA
publisher.none.fl_str_mv Universidade Federal de Minas Gerais
dc.source.none.fl_str_mv reponame:Repositório Institucional da UFMG
instname:Universidade Federal de Minas Gerais (UFMG)
instacron:UFMG
instname_str Universidade Federal de Minas Gerais (UFMG)
instacron_str UFMG
institution UFMG
reponame_str Repositório Institucional da UFMG
collection Repositório Institucional da UFMG
bitstream.url.fl_str_mv https://repositorio.ufmg.br/bitstream/1843/50999/1/On_the_phase_transition_for_some_percolation_models_in_random_environments.pdf
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