Nematic phase in two-dimensional frustrated systems with power-law decaying interactions

Detalhes bibliográficos
Autor(a) principal: Barci, Daniel G.
Data de Publicação: 2013
Outros Autores: Ribeiro, Leonardo Rodrigues, Stariolo, Daniel Adrian
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRGS
Texto Completo: http://hdl.handle.net/10183/101838
Resumo: We address the problem of orientational order in frustrated interaction systems as a function of the relative range of the competing interactions. We study a spin model Hamiltonian with short-range ferromagnetic interaction competing with an antiferromagnetic component that decays as a power law of the distance between spins, 1/rα. These systems may develop a nematic phase between the isotropic disordered and stripe phases.We evaluate the nematic order parameter using a self-consistent mean-field calculation. Our main result indicates that the nematic phase exists, at mean-field level, provided 0 < α < 4. We analytically compute the nematic critical temperature and show that it increases with the range of the interaction, reaching its maximum near α ∼ 0.5.We also compute a coarse-grained effective Hamiltonian for long wavelength fluctuations. For 0 < α < 4 the inverse susceptibility develops a set of continuous minima at wave vectors | k| = k0(α) which dictate the long-distance physics of the system. For α → 4, k0 → 0, making the competition between interactions ineffective for greater values of α.
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spelling Barci, Daniel G.Ribeiro, Leonardo RodriguesStariolo, Daniel Adrian2014-08-26T09:26:20Z20131539-3755http://hdl.handle.net/10183/101838000898229We address the problem of orientational order in frustrated interaction systems as a function of the relative range of the competing interactions. We study a spin model Hamiltonian with short-range ferromagnetic interaction competing with an antiferromagnetic component that decays as a power law of the distance between spins, 1/rα. These systems may develop a nematic phase between the isotropic disordered and stripe phases.We evaluate the nematic order parameter using a self-consistent mean-field calculation. Our main result indicates that the nematic phase exists, at mean-field level, provided 0 < α < 4. We analytically compute the nematic critical temperature and show that it increases with the range of the interaction, reaching its maximum near α ∼ 0.5.We also compute a coarse-grained effective Hamiltonian for long wavelength fluctuations. For 0 < α < 4 the inverse susceptibility develops a set of continuous minima at wave vectors | k| = k0(α) which dictate the long-distance physics of the system. For α → 4, k0 → 0, making the competition between interactions ineffective for greater values of α.application/pdfengPhysical review. E, Statistical, nonlinear, and soft matter physics. Vol. 87, no. 6 (June 2013), 062119, 7 p.AntiferromagnetismoFerromagnetismoModelo de isingFrustração (Física)Suscetibilidade magnéticaHamiltonianos de spinCálculos SCFNematic phase in two-dimensional frustrated systems with power-law decaying interactionsEstrangeiroinfo: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:UFRGSORIGINAL000898229.pdf000898229.pdfTexto completo (inglês)application/pdf201165http://www.lume.ufrgs.br/bitstream/10183/101838/1/000898229.pdf746dfce20751b7ad6ed15f1516710866MD51TEXT000898229.pdf.txt000898229.pdf.txtExtracted Texttext/plain35765http://www.lume.ufrgs.br/bitstream/10183/101838/2/000898229.pdf.txtf675bef7aa4dc01019d9f55b00b3f8d1MD52THUMBNAIL000898229.pdf.jpg000898229.pdf.jpgGenerated Thumbnailimage/jpeg2191http://www.lume.ufrgs.br/bitstream/10183/101838/3/000898229.pdf.jpge8b979e1a4e6b603da6c4a97bcf54ba4MD5310183/1018382018-10-22 09:29:32.527oai:www.lume.ufrgs.br:10183/101838Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2018-10-22T12:29:32Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
title Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
spellingShingle Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
Barci, Daniel G.
Antiferromagnetismo
Ferromagnetismo
Modelo de ising
Frustração (Física)
Suscetibilidade magnética
Hamiltonianos de spin
Cálculos SCF
title_short Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
title_full Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
title_fullStr Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
title_full_unstemmed Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
title_sort Nematic phase in two-dimensional frustrated systems with power-law decaying interactions
author Barci, Daniel G.
author_facet Barci, Daniel G.
Ribeiro, Leonardo Rodrigues
Stariolo, Daniel Adrian
author_role author
author2 Ribeiro, Leonardo Rodrigues
Stariolo, Daniel Adrian
author2_role author
author
dc.contributor.author.fl_str_mv Barci, Daniel G.
Ribeiro, Leonardo Rodrigues
Stariolo, Daniel Adrian
dc.subject.por.fl_str_mv Antiferromagnetismo
Ferromagnetismo
Modelo de ising
Frustração (Física)
Suscetibilidade magnética
Hamiltonianos de spin
Cálculos SCF
topic Antiferromagnetismo
Ferromagnetismo
Modelo de ising
Frustração (Física)
Suscetibilidade magnética
Hamiltonianos de spin
Cálculos SCF
description We address the problem of orientational order in frustrated interaction systems as a function of the relative range of the competing interactions. We study a spin model Hamiltonian with short-range ferromagnetic interaction competing with an antiferromagnetic component that decays as a power law of the distance between spins, 1/rα. These systems may develop a nematic phase between the isotropic disordered and stripe phases.We evaluate the nematic order parameter using a self-consistent mean-field calculation. Our main result indicates that the nematic phase exists, at mean-field level, provided 0 < α < 4. We analytically compute the nematic critical temperature and show that it increases with the range of the interaction, reaching its maximum near α ∼ 0.5.We also compute a coarse-grained effective Hamiltonian for long wavelength fluctuations. For 0 < α < 4 the inverse susceptibility develops a set of continuous minima at wave vectors | k| = k0(α) which dictate the long-distance physics of the system. For α → 4, k0 → 0, making the competition between interactions ineffective for greater values of α.
publishDate 2013
dc.date.issued.fl_str_mv 2013
dc.date.accessioned.fl_str_mv 2014-08-26T09:26:20Z
dc.type.driver.fl_str_mv Estrangeiro
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dc.identifier.uri.fl_str_mv http://hdl.handle.net/10183/101838
dc.identifier.issn.pt_BR.fl_str_mv 1539-3755
dc.identifier.nrb.pt_BR.fl_str_mv 000898229
identifier_str_mv 1539-3755
000898229
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dc.language.iso.fl_str_mv eng
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dc.relation.ispartof.pt_BR.fl_str_mv Physical review. E, Statistical, nonlinear, and soft matter physics. Vol. 87, no. 6 (June 2013), 062119, 7 p.
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