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
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/17931
Ver los metadatos del registro completo
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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 Técnicas2025-11-05T09:56:12Zoai: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:34982025-11-05 09:56:13.088CONICET 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 |
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eng |
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eng |
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openAccess |
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Elsevier Science |
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Elsevier Science |
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