Please use this identifier to cite or link to this item: https://libjncir.jncasr.ac.in/xmlui/handle/10572/2580
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dc.contributor.authorKumar, Pramod
dc.contributor.authorVidhyadhiraja, N. S.
dc.date.accessioned2017-02-21T09:35:41Z-
dc.date.available2017-02-21T09:35:41Z-
dc.date.issued2014
dc.identifier.citationKumar, P; Vidhyadhiraja, NS, Kondo-hole substitution in heavy fermions: Dynamics and transport. Physical Review B 2014, 90 (23), 235133 http://dx.doi.org/10.1103/PhysRevB.90.235133en_US
dc.identifier.citationPhysical Review Ben_US
dc.identifier.citation90en_US
dc.identifier.citation23en_US
dc.identifier.issn1098-0121
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/2580-
dc.descriptionRestricted Accessen_US
dc.description.abstractKondo-hole substitution is a unique probe for exploring the interplay of interactions, f-electron dilution, and disorder in heavy-fermion materials. Within the diluted periodic Anderson model, we investigate the changes in single-particle dynamics as well as response functions, as a function of Kondo-hole concentration (x) and temperature. We show that the spectral weight transfers due to Kondo-hole substitution have characteristics that are different from those induced by temperature; the dc resistivity crosses over from a highly nonmonotonic form with a coherence peak in the x -> 0 limit to a monotonic single-impurity-like form that saturates at low temperature. The thermopower exhibits a characteristic maximum as a function of temperature, the value of which changes sign with increasing x, and its location is shown to correspond to a low energy scale of the system. The Hall coefficient also changes sign with increasing x at zero temperature and is highly temperature dependent for all x. As x is increased beyond a certain x(c), the Drude peak and the mid-infrared peak in the optical conductivity vanish almost completely; a peak in the optical scattering rate melts and disappears eventually. We discuss the above-mentioned changes in the properties in terms of a crossover from coherent, Kondo lattice behavior to single-impurity-like, incoherent behavior with increasing x. A comparison of theory with experiments carried out for the dc resistivity and the thermopower of Ce1-xLaxB6 yields good agreement.en_US
dc.description.uri1550-235Xen_US
dc.description.urihttp://dx.doi.org/10.1103/PhysRevB.90.235133en_US
dc.language.isoEnglishen_US
dc.publisherAmerican Physical Societyen_US
dc.rights@American Physical Society, 2014en_US
dc.subjectCondensed Matter Physicsen_US
dc.subjectPeriodic Anderson Modelen_US
dc.subjectMean-Field Theoryen_US
dc.subjectInfinite Dimensionsen_US
dc.subjectLiquid Behavioren_US
dc.subjectRenormalization-Groupen_US
dc.subjectIntermediate Valenceen_US
dc.subjectQuantum Criticalityen_US
dc.subjectElectron-Systemsen_US
dc.subjectMetalsen_US
dc.subjectTemperatureen_US
dc.titleKondo-hole substitution in heavy fermions: Dynamics and transporten_US
dc.typeArticleen_US
Appears in Collections:Research Articles (Vidhyadhiraja N. S.)

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