Monte Carlo simulations of two-dimensional hard core lattice gases

Detalhes bibliográficos
Autor(a) principal: Fernandes, Heitor Carpes Marques
Data de Publicação: 2007
Outros Autores: Arenzon, Jeferson Jacob, Levin, Yan
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRGS
Texto Completo: http://hdl.handle.net/10183/204962
Resumo: Monte Carlo simulations are used to study lattice gases of particles with extended hard cores on a two-dimensional square lattice. Exclusions of one and up to five nearest neighbors (NN) are considered. These can be mapped onto hard squares of varying side length, λ (in lattice units), tilted by some angle with respect to the original lattice. In agreement with earlier studies, the 1NN exclusion undergoes a continuous order-disorder transition in the Ising universality class. Surprisingly, we find that the lattice gas with exclusions of up to second nearest neighbors (2NN) also undergoes a continuous phase transition in the Ising universality class, while the Landau–Lifshitz theory predicts that this transition should be in the universality class of the XY model with cubic anisotropy. The lattice gas of 3NN exclusions is found to undergo a discontinuous order-disorder transition, in agreement with the earlier transfer matrix calculations and the Landau–Lifshitz theory. On the other hand, the gas of 4NN exclusions once again exhibits a continuous phase transition in the Ising universality class—contradicting the predictions of the Landau–Lifshitz theory. Finally, the lattice gas of 5NN exclusions is found to undergo a discontinuous phase transition.
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spelling Fernandes, Heitor Carpes MarquesArenzon, Jeferson JacobLevin, Yan2020-01-28T04:11:02Z20070021-9606http://hdl.handle.net/10183/204962000593902Monte Carlo simulations are used to study lattice gases of particles with extended hard cores on a two-dimensional square lattice. Exclusions of one and up to five nearest neighbors (NN) are considered. These can be mapped onto hard squares of varying side length, λ (in lattice units), tilted by some angle with respect to the original lattice. In agreement with earlier studies, the 1NN exclusion undergoes a continuous order-disorder transition in the Ising universality class. Surprisingly, we find that the lattice gas with exclusions of up to second nearest neighbors (2NN) also undergoes a continuous phase transition in the Ising universality class, while the Landau–Lifshitz theory predicts that this transition should be in the universality class of the XY model with cubic anisotropy. The lattice gas of 3NN exclusions is found to undergo a discontinuous order-disorder transition, in agreement with the earlier transfer matrix calculations and the Landau–Lifshitz theory. On the other hand, the gas of 4NN exclusions once again exhibits a continuous phase transition in the Ising universality class—contradicting the predictions of the Landau–Lifshitz theory. Finally, the lattice gas of 5NN exclusions is found to undergo a discontinuous phase transition.application/pdfengThe journal of chemical physics. New York. Vol. 126, no. 11 (Mar. 2007), 114508, 11 p.Método de Monte CarloTransformacoes de ordem-desordemGás de redeTransformações de faseSistemas bidimensionaisMonte Carlo simulations of two-dimensional hard core lattice gasesEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT000593902.pdf.txt000593902.pdf.txtExtracted Texttext/plain56525http://www.lume.ufrgs.br/bitstream/10183/204962/2/000593902.pdf.txte5bc8c0a5f5e86cfb56bbe3d90023cacMD52ORIGINAL000593902.pdfTexto completo (inglês)application/pdf1510191http://www.lume.ufrgs.br/bitstream/10183/204962/1/000593902.pdf1c4be370e157b464be3dc2327420cc1cMD5110183/2049622023-08-02 03:31:18.658732oai:www.lume.ufrgs.br:10183/204962Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-08-02T06:31:18Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv Monte Carlo simulations of two-dimensional hard core lattice gases
title Monte Carlo simulations of two-dimensional hard core lattice gases
spellingShingle Monte Carlo simulations of two-dimensional hard core lattice gases
Fernandes, Heitor Carpes Marques
Método de Monte Carlo
Transformacoes de ordem-desordem
Gás de rede
Transformações de fase
Sistemas bidimensionais
title_short Monte Carlo simulations of two-dimensional hard core lattice gases
title_full Monte Carlo simulations of two-dimensional hard core lattice gases
title_fullStr Monte Carlo simulations of two-dimensional hard core lattice gases
title_full_unstemmed Monte Carlo simulations of two-dimensional hard core lattice gases
title_sort Monte Carlo simulations of two-dimensional hard core lattice gases
author Fernandes, Heitor Carpes Marques
author_facet Fernandes, Heitor Carpes Marques
Arenzon, Jeferson Jacob
Levin, Yan
author_role author
author2 Arenzon, Jeferson Jacob
Levin, Yan
author2_role author
author
dc.contributor.author.fl_str_mv Fernandes, Heitor Carpes Marques
Arenzon, Jeferson Jacob
Levin, Yan
dc.subject.por.fl_str_mv Método de Monte Carlo
Transformacoes de ordem-desordem
Gás de rede
Transformações de fase
Sistemas bidimensionais
topic Método de Monte Carlo
Transformacoes de ordem-desordem
Gás de rede
Transformações de fase
Sistemas bidimensionais
description Monte Carlo simulations are used to study lattice gases of particles with extended hard cores on a two-dimensional square lattice. Exclusions of one and up to five nearest neighbors (NN) are considered. These can be mapped onto hard squares of varying side length, λ (in lattice units), tilted by some angle with respect to the original lattice. In agreement with earlier studies, the 1NN exclusion undergoes a continuous order-disorder transition in the Ising universality class. Surprisingly, we find that the lattice gas with exclusions of up to second nearest neighbors (2NN) also undergoes a continuous phase transition in the Ising universality class, while the Landau–Lifshitz theory predicts that this transition should be in the universality class of the XY model with cubic anisotropy. The lattice gas of 3NN exclusions is found to undergo a discontinuous order-disorder transition, in agreement with the earlier transfer matrix calculations and the Landau–Lifshitz theory. On the other hand, the gas of 4NN exclusions once again exhibits a continuous phase transition in the Ising universality class—contradicting the predictions of the Landau–Lifshitz theory. Finally, the lattice gas of 5NN exclusions is found to undergo a discontinuous phase transition.
publishDate 2007
dc.date.issued.fl_str_mv 2007
dc.date.accessioned.fl_str_mv 2020-01-28T04:11:02Z
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dc.identifier.issn.pt_BR.fl_str_mv 0021-9606
dc.identifier.nrb.pt_BR.fl_str_mv 000593902
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dc.relation.ispartof.pt_BR.fl_str_mv The journal of chemical physics. New York. Vol. 126, no. 11 (Mar. 2007), 114508, 11 p.
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