Solution on the bethe lattice of a hard core athermal gas with two kinds of particles

Detalhes bibliográficos
Autor(a) principal: Oliveira, Tiago J.
Data de Publicação: 2011
Outros Autores: Stilck, Jürgen F.
Tipo de documento: Artigo
Idioma: eng
Título da fonte: LOCUS Repositório Institucional da UFV
Texto Completo: https://doi.org/10.1063/1.3658045
http://www.locus.ufv.br/handle/123456789/19316
Resumo: Athermal lattice gases of particles with first neighbor exclusion have been studied for a long time as simple models exhibiting a fluid-solid transition. At low concentration the particles occupy randomly both sublattices, but as the concentration is increased one of the sublattices is occupied preferentially. Here, we study a mixed lattice gas with excluded volume interactions only in the grand-canonical formalism with two kinds of particles: small ones, which occupy a single lattice site and large ones, which, when placed on a site, do not allow other particles to occupy its first neighbors also. We solve the model on a Bethe lattice of arbitrary coordination number q. In the parameter space defined by the activities of both particles, at low values of the activity of small particles (z1) we find a continuous transition from the fluid to the solid phase as the activity of large particles (z2) is increased. At higher values of z1 the transition becomes discontinuous, both regimes are separated by a tricritical point. The critical line has a negative slope at z1 = 0 and displays a minimum before reaching the tricritical point, so that a re-entrant behavior is observed for constant values of z2 in the region of low density of small particles. The isobaric curves of the total density of particles as a function of the density or the activity of small particles show a minimum in the fluid phase.
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spelling Oliveira, Tiago J.Stilck, Jürgen F.2018-05-03T18:08:31Z2018-05-03T18:08:31Z2011-10-141089-7690https://doi.org/10.1063/1.3658045http://www.locus.ufv.br/handle/123456789/19316Athermal lattice gases of particles with first neighbor exclusion have been studied for a long time as simple models exhibiting a fluid-solid transition. At low concentration the particles occupy randomly both sublattices, but as the concentration is increased one of the sublattices is occupied preferentially. Here, we study a mixed lattice gas with excluded volume interactions only in the grand-canonical formalism with two kinds of particles: small ones, which occupy a single lattice site and large ones, which, when placed on a site, do not allow other particles to occupy its first neighbors also. We solve the model on a Bethe lattice of arbitrary coordination number q. In the parameter space defined by the activities of both particles, at low values of the activity of small particles (z1) we find a continuous transition from the fluid to the solid phase as the activity of large particles (z2) is increased. At higher values of z1 the transition becomes discontinuous, both regimes are separated by a tricritical point. The critical line has a negative slope at z1 = 0 and displays a minimum before reaching the tricritical point, so that a re-entrant behavior is observed for constant values of z2 in the region of low density of small particles. The isobaric curves of the total density of particles as a function of the density or the activity of small particles show a minimum in the fluid phase.engThe Journal of Chemical Physicsv. 135, p. 1845021-1845027, nov. 2011American Institute of Physicsinfo:eu-repo/semantics/openAccessSolutionBethe latticeHard core athermal gas with two kinds of particlesSolution on the bethe lattice of a hard core athermal gas with two kinds of particlesinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleapplication/pdfreponame:LOCUS Repositório Institucional da UFVinstname:Universidade Federal de Viçosa (UFV)instacron:UFVORIGINALartigo.pdfartigo.pdftexto completoapplication/pdf617378https://locus.ufv.br//bitstream/123456789/19316/1/artigo.pdff6b5468888f9b836b4979c94d00a5880MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://locus.ufv.br//bitstream/123456789/19316/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52THUMBNAILartigo.pdf.jpgartigo.pdf.jpgIM Thumbnailimage/jpeg4250https://locus.ufv.br//bitstream/123456789/19316/3/artigo.pdf.jpg5a1dba059d21945bb78abb1563b408ccMD53123456789/193162018-05-03 23:00:39.045oai:locus.ufv.br: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Repositório InstitucionalPUBhttps://www.locus.ufv.br/oai/requestfabiojreis@ufv.bropendoar:21452018-05-04T02:00:39LOCUS Repositório Institucional da UFV - Universidade Federal de Viçosa (UFV)false
dc.title.en.fl_str_mv Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
title Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
spellingShingle Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
Oliveira, Tiago J.
Solution
Bethe lattice
Hard core athermal gas with two kinds of particles
title_short Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
title_full Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
title_fullStr Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
title_full_unstemmed Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
title_sort Solution on the bethe lattice of a hard core athermal gas with two kinds of particles
author Oliveira, Tiago J.
author_facet Oliveira, Tiago J.
Stilck, Jürgen F.
author_role author
author2 Stilck, Jürgen F.
author2_role author
dc.contributor.author.fl_str_mv Oliveira, Tiago J.
Stilck, Jürgen F.
dc.subject.pt-BR.fl_str_mv Solution
Bethe lattice
Hard core athermal gas with two kinds of particles
topic Solution
Bethe lattice
Hard core athermal gas with two kinds of particles
description Athermal lattice gases of particles with first neighbor exclusion have been studied for a long time as simple models exhibiting a fluid-solid transition. At low concentration the particles occupy randomly both sublattices, but as the concentration is increased one of the sublattices is occupied preferentially. Here, we study a mixed lattice gas with excluded volume interactions only in the grand-canonical formalism with two kinds of particles: small ones, which occupy a single lattice site and large ones, which, when placed on a site, do not allow other particles to occupy its first neighbors also. We solve the model on a Bethe lattice of arbitrary coordination number q. In the parameter space defined by the activities of both particles, at low values of the activity of small particles (z1) we find a continuous transition from the fluid to the solid phase as the activity of large particles (z2) is increased. At higher values of z1 the transition becomes discontinuous, both regimes are separated by a tricritical point. The critical line has a negative slope at z1 = 0 and displays a minimum before reaching the tricritical point, so that a re-entrant behavior is observed for constant values of z2 in the region of low density of small particles. The isobaric curves of the total density of particles as a function of the density or the activity of small particles show a minimum in the fluid phase.
publishDate 2011
dc.date.issued.fl_str_mv 2011-10-14
dc.date.accessioned.fl_str_mv 2018-05-03T18:08:31Z
dc.date.available.fl_str_mv 2018-05-03T18:08:31Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
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status_str publishedVersion
dc.identifier.uri.fl_str_mv https://doi.org/10.1063/1.3658045
http://www.locus.ufv.br/handle/123456789/19316
dc.identifier.issn.none.fl_str_mv 1089-7690
identifier_str_mv 1089-7690
url https://doi.org/10.1063/1.3658045
http://www.locus.ufv.br/handle/123456789/19316
dc.language.iso.fl_str_mv eng
language eng
dc.relation.ispartofseries.pt-BR.fl_str_mv v. 135, p. 1845021-1845027, nov. 2011
dc.rights.driver.fl_str_mv American Institute of Physics
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rights_invalid_str_mv American Institute of Physics
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dc.publisher.none.fl_str_mv The Journal of Chemical Physics
publisher.none.fl_str_mv The Journal of Chemical Physics
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