Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study

Autores
Guisandez, Leandro Eduardo; Zarragoicoechea, Guillermo Jorge; Albano, Ezequiel Vicente
Año de publicación
2013
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
The critical behaviour of the Ising ferromagnet confined in pores of radius R and length L is studied by means of Monte Carlo computer simulations. Quasi-cylindrical pores are obtained by replicating n-times a triangular lattice disc of radius R, where L = na and a is the spacing between consecutive replications. So, spins placed at the surface of the pores have less nearest-neighbours (NN) as compared to 8 NN for spins in the bulk. These “missing neighbour” effects undergone by surface spins cause a strong suppression of surface ordering, leading to an ordinary surface transition. Also, the effect propagates into the bulk for small tubes (R ≤ 12) and the effective critical temperature of the pores is shifted towards lower values than in the bulk case. By applying the standard finite-size scaling theory, subsequently supported by numerical data, we concluded that data collapse of relevant observables, e.g., magnetization (m), susceptibility, specific heat, etc., can only be observed by comparing simulation results obtained by keeping the aspect ratio C ≡ R/L constant. Also, by extrapolating “effective” R-dependent critical temperatures to the thermodynamic limit (R → ∞, C fixed), we obtained TC(∞) = 6.208(4). As suggested by finite-size scaling arguments, the magnetization is measured at the critical point scales according to |m| TcR β ν ∝ R L 1 2 , where β and ν are the standard exponents for the order parameter and the correlation length, respectively. Furthermore, it is shown that close to criticality the axial correlation length decreases exponentially with the distance. That result is the signature of the formation of (randomly distributed) alternating domains of different magnetization, which can be directly observed by means of snapshot configurations, whose typical length (ξ ) is given by the characteristic length of the exponential decay of correlations. Moreover, we show that at criticality ξ = 0.43(2)R.
Instituto de Física de Líquidos y Sistemas Biológicos
Consejo Nacional de Investigaciones Científicas y Técnicas
Comisión de Investigaciones Científicas de la provincia de Buenos Aires
Materia
Física
Propiedades de materiales confinados
Transiciones de fase
Fenómenos críticos
Simulaciones numéricas
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:10915/98462

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repository_id_str 1329
network_name_str SEDICI (UNLP)
spelling Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo studyGuisandez, Leandro EduardoZarragoicoechea, Guillermo JorgeAlbano, Ezequiel VicenteFísicaPropiedades de materiales confinadosTransiciones de faseFenómenos críticosSimulaciones numéricasThe critical behaviour of the Ising ferromagnet confined in pores of radius R and length L is studied by means of Monte Carlo computer simulations. Quasi-cylindrical pores are obtained by replicating n-times a triangular lattice disc of radius R, where L = na and a is the spacing between consecutive replications. So, spins placed at the surface of the pores have less nearest-neighbours (NN) as compared to 8 NN for spins in the bulk. These “missing neighbour” effects undergone by surface spins cause a strong suppression of surface ordering, leading to an ordinary surface transition. Also, the effect propagates into the bulk for small tubes (R ≤ 12) and the effective critical temperature of the pores is shifted towards lower values than in the bulk case. By applying the standard finite-size scaling theory, subsequently supported by numerical data, we concluded that data collapse of relevant observables, e.g., magnetization (m), susceptibility, specific heat, etc., can only be observed by comparing simulation results obtained by keeping the aspect ratio C ≡ R/L constant. Also, by extrapolating “effective” R-dependent critical temperatures to the thermodynamic limit (R → ∞, C fixed), we obtained TC(∞) = 6.208(4). As suggested by finite-size scaling arguments, the magnetization is measured at the critical point scales according to |m| TcR β ν ∝ R L 1 2 , where β and ν are the standard exponents for the order parameter and the correlation length, respectively. Furthermore, it is shown that close to criticality the axial correlation length decreases exponentially with the distance. That result is the signature of the formation of (randomly distributed) alternating domains of different magnetization, which can be directly observed by means of snapshot configurations, whose typical length (ξ ) is given by the characteristic length of the exponential decay of correlations. Moreover, we show that at criticality ξ = 0.43(2)R.Instituto de Física de Líquidos y Sistemas BiológicosConsejo Nacional de Investigaciones Científicas y TécnicasComisión de Investigaciones Científicas de la provincia de Buenos Aires2013-10info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/98462enginfo:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/2404info:eu-repo/semantics/altIdentifier/issn/0021-9606info:eu-repo/semantics/altIdentifier/doi/10.1063/1.4821826info:eu-repo/semantics/altIdentifier/hdl/11336/2404info: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:UNLP2025-10-15T11:11:54Zoai:sedici.unlp.edu.ar:10915/98462Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-10-15 11:11:54.969SEDICI (UNLP) - Universidad Nacional de La Platafalse
dc.title.none.fl_str_mv Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
title Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
spellingShingle Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
Guisandez, Leandro Eduardo
Física
Propiedades de materiales confinados
Transiciones de fase
Fenómenos críticos
Simulaciones numéricas
title_short Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
title_full Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
title_fullStr Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
title_full_unstemmed Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
title_sort Critical behaviour of the Ising ferromagnet confined in quasi-cylindrical pores: A Monte Carlo study
dc.creator.none.fl_str_mv Guisandez, Leandro Eduardo
Zarragoicoechea, Guillermo Jorge
Albano, Ezequiel Vicente
author Guisandez, Leandro Eduardo
author_facet Guisandez, Leandro Eduardo
Zarragoicoechea, Guillermo Jorge
Albano, Ezequiel Vicente
author_role author
author2 Zarragoicoechea, Guillermo Jorge
Albano, Ezequiel Vicente
author2_role author
author
dc.subject.none.fl_str_mv Física
Propiedades de materiales confinados
Transiciones de fase
Fenómenos críticos
Simulaciones numéricas
topic Física
Propiedades de materiales confinados
Transiciones de fase
Fenómenos críticos
Simulaciones numéricas
dc.description.none.fl_txt_mv The critical behaviour of the Ising ferromagnet confined in pores of radius R and length L is studied by means of Monte Carlo computer simulations. Quasi-cylindrical pores are obtained by replicating n-times a triangular lattice disc of radius R, where L = na and a is the spacing between consecutive replications. So, spins placed at the surface of the pores have less nearest-neighbours (NN) as compared to 8 NN for spins in the bulk. These “missing neighbour” effects undergone by surface spins cause a strong suppression of surface ordering, leading to an ordinary surface transition. Also, the effect propagates into the bulk for small tubes (R ≤ 12) and the effective critical temperature of the pores is shifted towards lower values than in the bulk case. By applying the standard finite-size scaling theory, subsequently supported by numerical data, we concluded that data collapse of relevant observables, e.g., magnetization (m), susceptibility, specific heat, etc., can only be observed by comparing simulation results obtained by keeping the aspect ratio C ≡ R/L constant. Also, by extrapolating “effective” R-dependent critical temperatures to the thermodynamic limit (R → ∞, C fixed), we obtained TC(∞) = 6.208(4). As suggested by finite-size scaling arguments, the magnetization is measured at the critical point scales according to |m| TcR β ν ∝ R L 1 2 , where β and ν are the standard exponents for the order parameter and the correlation length, respectively. Furthermore, it is shown that close to criticality the axial correlation length decreases exponentially with the distance. That result is the signature of the formation of (randomly distributed) alternating domains of different magnetization, which can be directly observed by means of snapshot configurations, whose typical length (ξ ) is given by the characteristic length of the exponential decay of correlations. Moreover, we show that at criticality ξ = 0.43(2)R.
Instituto de Física de Líquidos y Sistemas Biológicos
Consejo Nacional de Investigaciones Científicas y Técnicas
Comisión de Investigaciones Científicas de la provincia de Buenos Aires
description The critical behaviour of the Ising ferromagnet confined in pores of radius R and length L is studied by means of Monte Carlo computer simulations. Quasi-cylindrical pores are obtained by replicating n-times a triangular lattice disc of radius R, where L = na and a is the spacing between consecutive replications. So, spins placed at the surface of the pores have less nearest-neighbours (NN) as compared to 8 NN for spins in the bulk. These “missing neighbour” effects undergone by surface spins cause a strong suppression of surface ordering, leading to an ordinary surface transition. Also, the effect propagates into the bulk for small tubes (R ≤ 12) and the effective critical temperature of the pores is shifted towards lower values than in the bulk case. By applying the standard finite-size scaling theory, subsequently supported by numerical data, we concluded that data collapse of relevant observables, e.g., magnetization (m), susceptibility, specific heat, etc., can only be observed by comparing simulation results obtained by keeping the aspect ratio C ≡ R/L constant. Also, by extrapolating “effective” R-dependent critical temperatures to the thermodynamic limit (R → ∞, C fixed), we obtained TC(∞) = 6.208(4). As suggested by finite-size scaling arguments, the magnetization is measured at the critical point scales according to |m| TcR β ν ∝ R L 1 2 , where β and ν are the standard exponents for the order parameter and the correlation length, respectively. Furthermore, it is shown that close to criticality the axial correlation length decreases exponentially with the distance. That result is the signature of the formation of (randomly distributed) alternating domains of different magnetization, which can be directly observed by means of snapshot configurations, whose typical length (ξ ) is given by the characteristic length of the exponential decay of correlations. Moreover, we show that at criticality ξ = 0.43(2)R.
publishDate 2013
dc.date.none.fl_str_mv 2013-10
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info:eu-repo/semantics/altIdentifier/doi/10.1063/1.4821826
info:eu-repo/semantics/altIdentifier/hdl/11336/2404
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
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