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DC Field | Value | Language |
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dc.contributor.author | Kumar, Pramod | |
dc.contributor.author | Vidhyadhiraja, N. S. | |
dc.date.accessioned | 2017-02-21T09:35:41Z | - |
dc.date.available | 2017-02-21T09:35:41Z | - |
dc.date.issued | 2014 | |
dc.identifier.citation | Kumar, 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.90.235133 | en_US |
dc.identifier.citation | Physical Review B | en_US |
dc.identifier.citation | 90 | en_US |
dc.identifier.citation | 23 | en_US |
dc.identifier.issn | 1098-0121 | |
dc.identifier.uri | https://libjncir.jncasr.ac.in/xmlui/10572/2580 | - |
dc.description | Restricted Access | en_US |
dc.description.abstract | Kondo-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.uri | 1550-235X | en_US |
dc.description.uri | http://dx.doi.org/10.1103/PhysRevB.90.235133 | en_US |
dc.language.iso | English | en_US |
dc.publisher | American Physical Society | en_US |
dc.rights | @American Physical Society, 2014 | en_US |
dc.subject | Condensed Matter Physics | en_US |
dc.subject | Periodic Anderson Model | en_US |
dc.subject | Mean-Field Theory | en_US |
dc.subject | Infinite Dimensions | en_US |
dc.subject | Liquid Behavior | en_US |
dc.subject | Renormalization-Group | en_US |
dc.subject | Intermediate Valence | en_US |
dc.subject | Quantum Criticality | en_US |
dc.subject | Electron-Systems | en_US |
dc.subject | Metals | en_US |
dc.subject | Temperature | en_US |
dc.title | Kondo-hole substitution in heavy fermions: Dynamics and transport | en_US |
dc.type | Article | en_US |
Appears in Collections: | Research Articles (Vidhyadhiraja N. S.) |
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135.pdf Restricted Access | 2.28 MB | Adobe PDF | View/Open Request a copy |
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