Monte Carlo simulations of two-dimensional hard core lattice gases
Autor(a) principal: | |
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Data de Publicação: | 2007 |
Outros Autores: | , |
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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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 |
dc.type.driver.fl_str_mv |
Estrangeiro info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10183/204962 |
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0021-9606 |
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000593902 |
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0021-9606 000593902 |
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http://hdl.handle.net/10183/204962 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
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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info:eu-repo/semantics/openAccess |
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openAccess |
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