Resistivity of the Two-Channel Kondo Model in Infinite Dimensions

dc.creatorCox, D. L.
dc.date1994-05-17
dc.date1994-05-20
dc.date.accessioned2026-07-07T08:58:50Z
dc.date.available2026-07-07T08:58:50Z
dc.descriptionAnalytic results for the resistivity of the two-channel Kondo lattice in a particular infinite dimensional limit (Lorentzian density of states) are presented. It is argued that in the absence of symmetry breaking phase transitions or applied fields there is a residual resistivity at zero temperature due to the spin disorder scattering off of the two-channel screening clouds. This may explain the unusual resistivity of UBe$_{13}$. For the same limit the single channel Kondo lattice is an insulator states at particle hole symmetry and half filling, but metallic away from particle-hole symmetry or in applied magnetic field.
dc.description(5 Pages, REVTEX format, one postscript figure to be stripped off and printed separately)
dc.identifierhttps://arxiv.org/abs/cond-mat/9405049
dc.identifierhttp://arxiv.org/abs/cond-mat/9405049
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/147484
dc.subjectCondensed Matter
dc.titleResistivity of the Two-Channel Kondo Model in Infinite Dimensions
dc.typetext

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