Low temperature magnetic phase diagram of the cubic non-Fermi liquid system Celn(3-x)Sn(x)

cnea.localizacionCentro Atómico Bariloche
cnea.tipodocumentoARTÍCULO CIENTÍFICO
dc.contributor.authorPedrazzini, P.
dc.contributor.authorBerisso, M.G.
dc.contributor.authorCaroca-Canales, N.
dc.contributor.authorDeppe, M.
dc.contributor.authorGeibel, C.
dc.contributor.authorSereni, J.G.
dc.contributor.cneaproductorGerencia Física. Departamento Materia Condensada. División Bajas Temperaturas
dc.date.accessioned2024-05-07T13:37:01Z
dc.date.available2024-05-07T13:37:01Z
dc.date.issued2004-04-00
dc.description.abstractIn this paper we report a comprehensive study of the magnetic susceptibility (X), resistivity (ρ), and specific heat (Cp), down to 0.5 K of the cubic CeIn3-x Sn x alloy. The ground state of this system evolves from antiferromagnetic (AF) in CeIn3 (TN=10.2K) to intermediate-valent in CeSn3, and represents the first example of a Ce-lattice cubic non-Fermi liquid (NFL) system where TN (x) can be traced down to T = 0 over more than a decade of temperature. Our results indicate that the disappearance of the AF state occurs near xc≈0.7, although already at x≈0.4 significant modifications of the magnetic ground state are observed. Between these concentrations, clear NFL signatures are observed, such as ρ(T) ≈ ρ0 + ATn (with n < 1.5) and Cp (T)α‒ Tln (T) dependencies. Within the ordered phase a first order phase transition occurs for 0.25 < x < 0.5. With larger Sn doping, different weak ρ(T) dependencies are observed at low temperatures between x = 1 and x = 3 while Cp/T shows only a weak temperature dependence.
dc.description.institutionalaffiliationFil.: Pedrazzini, P. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
dc.description.institutionalaffiliationFil.: Gómez Berisso, M. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
dc.description.institutionalaffiliationFil.: Sereni, J.G. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina
dc.description.institutionalaffiliationexternalFil.: Caroca-Canales, N. Max-Planck Institute for Chemical Physics of Solids; Alemania
dc.description.institutionalaffiliationexternalFil.: Deppe, M. Max-Planck Institute for Chemical Physics of Solids; Alemania
dc.description.institutionalaffiliationexternalFil.: Geibel, C. Max-Planck Institute for Chemical Physics of Solids; Alemania
dc.description.recordsetsectionProducción científica
dc.description.recordsetseriesContribución a revistas científicas
dc.format.extent7 p.
dc.identifier.citationThe European Physical Journal B – Condensed Matter. Vol. 38, no. 3 (2004), p. 445-450
dc.identifier.doihttp://dx.doi.org/10.1140/epjb/e2004-00138-5
dc.identifier.issn1434-6036
dc.identifier.issn1434-6028
dc.identifier.urihttps://nuclea.cnea.gob.ar/handle/20.500.12553/5366
dc.language.ISO639-3eng
dc.publisherSpringer
dc.relation.ispartofv. 38, n. 4
dc.relation.ispartofseriesThe European Physical Journal B Condensed Matter and Complex Systems
dc.rights.accesslevelinfo:eu-repo/semantics/openAccess
dc.rights.urihttps://creativecommons.org/licenses/by-nc-sa/4.0/
dc.subject.fordCIENCIAS NATURALES
dc.subject.fordCIENCIAS FÍSICAS
dc.subject.inisCOMPUESTOS INTERMETALICOS
dc.subject.inisFERMIONES
dc.subject.inisEFECTO KONDO
dc.subject.keywordIntermetallic compounds
dc.subject.keywordHeavy fermions
dc.subject.keywordKondo effect
dc.titleLow temperature magnetic phase diagram of the cubic non-Fermi liquid system Celn(3-x)Sn(x)
dc.typeARTÍCULO
dc.type.openaireinfo:eu-repo/semantics/article
dc.type.snrdinfo:ar-repo/semantics/artículo
dc.type.versioninfo:eu-repo/semantics/publishedVersion

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