Underscreened Kondo lattice model applied to heavy fermion uranium compounds
dc.contributor.author | Perkins, Natalia B. | pt_BR |
dc.contributor.author | Núñez-Regueiro, M.D. | pt_BR |
dc.contributor.author | Coqblin, Bernard | pt_BR |
dc.contributor.author | Iglesias, Jose Roberto | pt_BR |
dc.date.accessioned | 2014-10-14T02:13:01Z | pt_BR |
dc.date.issued | 2007 | pt_BR |
dc.identifier.issn | 1098-0121 | pt_BR |
dc.identifier.uri | http://hdl.handle.net/10183/104515 | pt_BR |
dc.description.abstract | We present theoretical results for the underscreened Kondo lattice model with localized S=1 spins coupled to a conduction band through a Kondo coupling, JK, and interacting among them ferromagnetically. We use a fermionic representation for the spin operators and expand the Hamiltonian in terms of bosonic fields. For large values of JK, we obtain a ferromagnetically ordered solution and a Kondo regime with a Kondo temperature, TK, larger than the Curie temperature, TC. This finding suggests a scenario for a coexistence of Kondo effect and ferromagnetic order. In some uranium compounds, such as UTe or UCu0.9Sb2, this kind of coexistence has been experimentally observed: they order ferromagnetically with a Curie temperature of order TC 100 K and exhibit a Kondo behavior for T TC. The proposed underscreened Kondo lattice model accounts well for the coexistence between magnetic order and Kondo behavior and yields to a new “ferromagnetic Doniach diagram.” | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | eng | pt_BR |
dc.relation.ispartof | Physical review. B, Condensed matter and materials physics. New York. Vol. 76, no. 12 (Sept. 2007), 125101 12p. | pt_BR |
dc.rights | Open Access | en |
dc.subject | Fermions | pt_BR |
dc.subject | Compostos de urânio | pt_BR |
dc.subject | Efeito kondo | pt_BR |
dc.title | Underscreened Kondo lattice model applied to heavy fermion uranium compounds | pt_BR |
dc.type | Artigo de periódico | pt_BR |
dc.identifier.nrb | 000616570 | pt_BR |
dc.type.origin | Estrangeiro | pt_BR |
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