Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities

Autores
Trobo, Marta Liliana; Albano, Ezequiel Vicente
Año de publicación
2016
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
Fixed vacancies (non-magnetic impurities) are placed along the centre of Ising strips in order to study the wetting behaviour in this confined system, by means of numerical simulations analysed with the aid of finite size scaling and thermodynamic integration methods. By considering strips of size L x M (L ≪ M) where short-range competitive surface fields (Hs) act along the M-direction, we observe localization–delocalization transitions of the interface between magnetic domains of different orientation (driven by the corresponding surface fields), which are the precursors of the wetting transitions that occur in the thermodynamic limit. By placing vacancies or equivalently non-magnetic impurities along the centre of the sample, we found that for low vacancy densities the wetting transitions are of second order, while by increasing the concentration of vacancies the transitions become of first order. Second- and first-order lines meet in tricritical wetting points (H tric sw, tric T tric w), where Hsw tric and T w tric are the magnitude of the surface field and the temperature, respectively. In the phase diagram, tricritical points shift from the high temperature and weak surface field regime at large vacancy densities to the T → 0, Hsw tric → 1 limit for low vacancy densities. By comparing the locations of the tricritical points with those corresponding to the case of mobile impurities, we conclude that in order to observe similar effects, in the latter the required density of impurities is much smaller (e.g. by a factor 3–5). Furthermore, a proper density of non magnetic impurities placed along the centre of a strip can effectively pin rather flat magnetic interfaces for suitable values of the competing surface fields and temperature.
Instituto de Física de Líquidos y Sistemas Biológicos
Materia
Física
Tricritical wetting
Confined matterials
Interfaces
Nivel de accesibilidad
acceso abierto
Condiciones de uso
http://creativecommons.org/licenses/by-nc-sa/4.0/
Repositorio
SEDICI (UNLP)
Institución
Universidad Nacional de La Plata
OAI Identificador
oai:sedici.unlp.edu.ar:10915/102542

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spelling Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impuritiesTrobo, Marta LilianaAlbano, Ezequiel VicenteFísicaTricritical wettingConfined matterialsInterfacesFixed vacancies (non-magnetic impurities) are placed along the centre of Ising strips in order to study the wetting behaviour in this confined system, by means of numerical simulations analysed with the aid of finite size scaling and thermodynamic integration methods. By considering strips of size L x M (L ≪ M) where short-range competitive surface fields (H<sub>s</sub>) act along the M-direction, we observe localization–delocalization transitions of the interface between magnetic domains of different orientation (driven by the corresponding surface fields), which are the precursors of the wetting transitions that occur in the thermodynamic limit. By placing vacancies or equivalently non-magnetic impurities along the centre of the sample, we found that for low vacancy densities the wetting transitions are of second order, while by increasing the concentration of vacancies the transitions become of first order. Second- and first-order lines meet in tricritical wetting points (H tric sw, tric T tric w), where Hsw tric and T w tric are the magnitude of the surface field and the temperature, respectively. In the phase diagram, tricritical points shift from the high temperature and weak surface field regime at large vacancy densities to the T → 0, Hsw tric → 1 limit for low vacancy densities. By comparing the locations of the tricritical points with those corresponding to the case of mobile impurities, we conclude that in order to observe similar effects, in the latter the required density of impurities is much smaller (e.g. by a factor 3–5). Furthermore, a proper density of non magnetic impurities placed along the centre of a strip can effectively pin rather flat magnetic interfaces for suitable values of the competing surface fields and temperature.Instituto de Física de Líquidos y Sistemas Biológicos2016-02info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf125001-125010http://sedici.unlp.edu.ar/handle/10915/102542enginfo:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/48101info:eu-repo/semantics/altIdentifier/url/http://iopscience.iop.org/article/10.1088/0953-8984/28/12/125001/metainfo:eu-repo/semantics/altIdentifier/issn/0953-8984info:eu-repo/semantics/altIdentifier/doi/10.1088/0953-8984/28/12/125001info:eu-repo/semantics/altIdentifier/hdl/11336/48101info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/4.0/Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-09-03T10:52:20Zoai:sedici.unlp.edu.ar:10915/102542Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-09-03 10:52:21.178SEDICI (UNLP) - Universidad Nacional de La Platafalse
dc.title.none.fl_str_mv Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
title Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
spellingShingle Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
Trobo, Marta Liliana
Física
Tricritical wetting
Confined matterials
Interfaces
title_short Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
title_full Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
title_fullStr Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
title_full_unstemmed Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
title_sort Tricritical wetting in the two-dimensional Ising magnet due to the presence of localized non-magnetic impurities
dc.creator.none.fl_str_mv Trobo, Marta Liliana
Albano, Ezequiel Vicente
author Trobo, Marta Liliana
author_facet Trobo, Marta Liliana
Albano, Ezequiel Vicente
author_role author
author2 Albano, Ezequiel Vicente
author2_role author
dc.subject.none.fl_str_mv Física
Tricritical wetting
Confined matterials
Interfaces
topic Física
Tricritical wetting
Confined matterials
Interfaces
dc.description.none.fl_txt_mv Fixed vacancies (non-magnetic impurities) are placed along the centre of Ising strips in order to study the wetting behaviour in this confined system, by means of numerical simulations analysed with the aid of finite size scaling and thermodynamic integration methods. By considering strips of size L x M (L ≪ M) where short-range competitive surface fields (H<sub>s</sub>) act along the M-direction, we observe localization–delocalization transitions of the interface between magnetic domains of different orientation (driven by the corresponding surface fields), which are the precursors of the wetting transitions that occur in the thermodynamic limit. By placing vacancies or equivalently non-magnetic impurities along the centre of the sample, we found that for low vacancy densities the wetting transitions are of second order, while by increasing the concentration of vacancies the transitions become of first order. Second- and first-order lines meet in tricritical wetting points (H tric sw, tric T tric w), where Hsw tric and T w tric are the magnitude of the surface field and the temperature, respectively. In the phase diagram, tricritical points shift from the high temperature and weak surface field regime at large vacancy densities to the T → 0, Hsw tric → 1 limit for low vacancy densities. By comparing the locations of the tricritical points with those corresponding to the case of mobile impurities, we conclude that in order to observe similar effects, in the latter the required density of impurities is much smaller (e.g. by a factor 3–5). Furthermore, a proper density of non magnetic impurities placed along the centre of a strip can effectively pin rather flat magnetic interfaces for suitable values of the competing surface fields and temperature.
Instituto de Física de Líquidos y Sistemas Biológicos
description Fixed vacancies (non-magnetic impurities) are placed along the centre of Ising strips in order to study the wetting behaviour in this confined system, by means of numerical simulations analysed with the aid of finite size scaling and thermodynamic integration methods. By considering strips of size L x M (L ≪ M) where short-range competitive surface fields (H<sub>s</sub>) act along the M-direction, we observe localization–delocalization transitions of the interface between magnetic domains of different orientation (driven by the corresponding surface fields), which are the precursors of the wetting transitions that occur in the thermodynamic limit. By placing vacancies or equivalently non-magnetic impurities along the centre of the sample, we found that for low vacancy densities the wetting transitions are of second order, while by increasing the concentration of vacancies the transitions become of first order. Second- and first-order lines meet in tricritical wetting points (H tric sw, tric T tric w), where Hsw tric and T w tric are the magnitude of the surface field and the temperature, respectively. In the phase diagram, tricritical points shift from the high temperature and weak surface field regime at large vacancy densities to the T → 0, Hsw tric → 1 limit for low vacancy densities. By comparing the locations of the tricritical points with those corresponding to the case of mobile impurities, we conclude that in order to observe similar effects, in the latter the required density of impurities is much smaller (e.g. by a factor 3–5). Furthermore, a proper density of non magnetic impurities placed along the centre of a strip can effectively pin rather flat magnetic interfaces for suitable values of the competing surface fields and temperature.
publishDate 2016
dc.date.none.fl_str_mv 2016-02
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
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format article
status_str publishedVersion
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dc.language.none.fl_str_mv eng
language eng
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info:eu-repo/semantics/altIdentifier/issn/0953-8984
info:eu-repo/semantics/altIdentifier/doi/10.1088/0953-8984/28/12/125001
info:eu-repo/semantics/altIdentifier/hdl/11336/48101
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
http://creativecommons.org/licenses/by-nc-sa/4.0/
Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)
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rights_invalid_str_mv http://creativecommons.org/licenses/by-nc-sa/4.0/
Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)
dc.format.none.fl_str_mv application/pdf
125001-125010
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repository.name.fl_str_mv SEDICI (UNLP) - Universidad Nacional de La Plata
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