Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit

Autores
Allub, Roberto Jose
Año de publicación
2013
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
The lowest excitation energy and the magnetic correlations 〈S1·S2 〉 between two magnetic impurities are analyzed within the two-magnetic-impurity model Hamiltonian. The model includes two magnetic ions that can exist in two valence states and a band of conduction electrons. The two localized states represent the ground states of the ionic configurations (5f)^n and (5f)^(n+1) , assumed to be a doublet and a triplet, respectively. In the zero band-width limit, three parameters characterize this model: the energy difference between the magnetic configurations (Δ), the localized-extended-state hybridization energy (V), and the relationship between the Fermi wavelength and the distance r between the magnetic ions (φ = k_ (F)· r ). For φ →0, the strong coupling regime takes place and the physics that governs the ground state depends on Δ/V. For V<<−Δ, the highest spin configuration is favored, and the model shows a triplet ground state and the coexistence of strong ferromagnetic (F) correlations between the impurities with the Kondo physics of two magnetic impurities. For V <−Δ, with major charge fluctuations between the magnetic configurations, a singlet ground state occurs and antiferromagnetic (AF) correlations between the impurities appear. When φ increases, the decoupling of the impurities proceeds and 〈S1·S2 〉decreases, finally for φ=π/2 the decoupled limit takes place and the model is reduced to two independent ions (〈S1·S2 〉= 0). For a narrow region of Δ/V, when φ increases, the model shows the crossover from singlet (AF) ground state to triplet (F) ground state.


Fil: Allub, Roberto Jose. Comision Nacional de Energia Atomica. Gerencia del Area de Investigaciones y Aplicaciones no Nucleares. Gerencia de Fisica (CAB); Argentina
Materia
Local Moment
Kondo Effect
Heavy Fermions
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/17931

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network_name_str CONICET Digital (CONICET)
spelling Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limitAllub, Roberto JoseLocal MomentKondo EffectHeavy Fermionshttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1The lowest excitation energy and the magnetic correlations 〈S1·S2 〉 between two magnetic impurities are analyzed within the two-magnetic-impurity model Hamiltonian. The model includes two magnetic ions that can exist in two valence states and a band of conduction electrons. The two localized states represent the ground states of the ionic configurations (5f)^n and (5f)^(n+1) , assumed to be a doublet and a triplet, respectively. In the zero band-width limit, three parameters characterize this model: the energy difference between the magnetic configurations (Δ), the localized-extended-state hybridization energy (V), and the relationship between the Fermi wavelength and the distance r between the magnetic ions (φ = k_ (F)· r ). For φ →0,<style type="text/css">P { margin-bottom: 0.21cm; }</style> <style type="text/css">P { margin-bottom: 0.21cm</style> the strong coupling regime takes place and the physics that governs the ground state depends on Δ/V. For V<<−Δ, the highest spin configuration is favored, and the model shows a triplet ground state and the coexistence of strong ferromagnetic (F) correlations between the impurities with the Kondo physics of two magnetic impurities. For V <−Δ, with major charge fluctuations between the magnetic configurations, a singlet ground state occurs and antiferromagnetic (AF) correlations between the impurities appear. When φ increases, the decoupling of the impurities proceeds and 〈S1·S2 〉decreases, finally for φ=π/2 the decoupled limit takes place and the model is reduced to two independent ions (〈S1·S2 〉= 0). For a narrow region of Δ/V, when φ increases, the model shows the crossover from singlet (AF) ground state to triplet (F) ground state.<br /><br />Fil: Allub, Roberto Jose. Comision Nacional de Energia Atomica. Gerencia del Area de Investigaciones y Aplicaciones no Nucleares. Gerencia de Fisica (CAB); ArgentinaElsevier Science2013-04info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/octet-streamapplication/pdfhttp://hdl.handle.net/11336/17931Allub, Roberto Jose; Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit; Elsevier Science; Physica B: Condensed Matter; 421; 4-2013; 34-400921-4526enginfo:eu-repo/semantics/altIdentifier/doi/10.1016/j.physb.2013.04.009info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-15T14:48:31Zoai:ri.conicet.gov.ar:11336/17931instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-10-15 14:48:31.299CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
title Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
spellingShingle Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
Allub, Roberto Jose
Local Moment
Kondo Effect
Heavy Fermions
title_short Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
title_full Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
title_fullStr Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
title_full_unstemmed Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
title_sort Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit
dc.creator.none.fl_str_mv Allub, Roberto Jose
author Allub, Roberto Jose
author_facet Allub, Roberto Jose
author_role author
dc.subject.none.fl_str_mv Local Moment
Kondo Effect
Heavy Fermions
topic Local Moment
Kondo Effect
Heavy Fermions
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv The lowest excitation energy and the magnetic correlations 〈S1·S2 〉 between two magnetic impurities are analyzed within the two-magnetic-impurity model Hamiltonian. The model includes two magnetic ions that can exist in two valence states and a band of conduction electrons. The two localized states represent the ground states of the ionic configurations (5f)^n and (5f)^(n+1) , assumed to be a doublet and a triplet, respectively. In the zero band-width limit, three parameters characterize this model: the energy difference between the magnetic configurations (Δ), the localized-extended-state hybridization energy (V), and the relationship between the Fermi wavelength and the distance r between the magnetic ions (φ = k_ (F)· r ). For φ →0,<style type="text/css">P { margin-bottom: 0.21cm; }</style> <style type="text/css">P { margin-bottom: 0.21cm</style> the strong coupling regime takes place and the physics that governs the ground state depends on Δ/V. For V<<−Δ, the highest spin configuration is favored, and the model shows a triplet ground state and the coexistence of strong ferromagnetic (F) correlations between the impurities with the Kondo physics of two magnetic impurities. For V <−Δ, with major charge fluctuations between the magnetic configurations, a singlet ground state occurs and antiferromagnetic (AF) correlations between the impurities appear. When φ increases, the decoupling of the impurities proceeds and 〈S1·S2 〉decreases, finally for φ=π/2 the decoupled limit takes place and the model is reduced to two independent ions (〈S1·S2 〉= 0). For a narrow region of Δ/V, when φ increases, the model shows the crossover from singlet (AF) ground state to triplet (F) ground state.<br /><br />
Fil: Allub, Roberto Jose. Comision Nacional de Energia Atomica. Gerencia del Area de Investigaciones y Aplicaciones no Nucleares. Gerencia de Fisica (CAB); Argentina
description The lowest excitation energy and the magnetic correlations 〈S1·S2 〉 between two magnetic impurities are analyzed within the two-magnetic-impurity model Hamiltonian. The model includes two magnetic ions that can exist in two valence states and a band of conduction electrons. The two localized states represent the ground states of the ionic configurations (5f)^n and (5f)^(n+1) , assumed to be a doublet and a triplet, respectively. In the zero band-width limit, three parameters characterize this model: the energy difference between the magnetic configurations (Δ), the localized-extended-state hybridization energy (V), and the relationship between the Fermi wavelength and the distance r between the magnetic ions (φ = k_ (F)· r ). For φ →0,<style type="text/css">P { margin-bottom: 0.21cm; }</style> <style type="text/css">P { margin-bottom: 0.21cm</style> the strong coupling regime takes place and the physics that governs the ground state depends on Δ/V. For V<<−Δ, the highest spin configuration is favored, and the model shows a triplet ground state and the coexistence of strong ferromagnetic (F) correlations between the impurities with the Kondo physics of two magnetic impurities. For V <−Δ, with major charge fluctuations between the magnetic configurations, a singlet ground state occurs and antiferromagnetic (AF) correlations between the impurities appear. When φ increases, the decoupling of the impurities proceeds and 〈S1·S2 〉decreases, finally for φ=π/2 the decoupled limit takes place and the model is reduced to two independent ions (〈S1·S2 〉= 0). For a narrow region of Δ/V, when φ increases, the model shows the crossover from singlet (AF) ground state to triplet (F) ground state.<br /><br />
publishDate 2013
dc.date.none.fl_str_mv 2013-04
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/17931
Allub, Roberto Jose; Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit; Elsevier Science; Physica B: Condensed Matter; 421; 4-2013; 34-40
0921-4526
url http://hdl.handle.net/11336/17931
identifier_str_mv Allub, Roberto Jose; Magnetic correlations between two Kondo impurities with two magnetic configurations: Narrow-band limit; Elsevier Science; Physica B: Condensed Matter; 421; 4-2013; 34-40
0921-4526
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/doi/10.1016/j.physb.2013.04.009
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/octet-stream
application/pdf
dc.publisher.none.fl_str_mv Elsevier Science
publisher.none.fl_str_mv Elsevier Science
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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