1986
DOI: 10.1143/jpsj.55.1294
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Coherent Kondo State in a Dense Kondo Substance: CexLa1-xCu6

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Cited by 175 publications
(64 citation statements)
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“…Generally, in heavy-fermion materials, isovalent substitution of magnetic ions with non-magnetic ones leads to a crossover from a coherent Kondo lattice to the dilute Kondo impurity regime, as it was shown for Ce 1−x La x Cu 6 [53][54][55][56]. Lanthanum doping of CeB 6 suppresses both AFM and AFQ phases and induces a new multipolar-ordered phase IV beyond a quantum critical point (QCP) at x ≈ 0.3, presumably of octupolar character [57][58][59].…”
Section: Introductionmentioning
confidence: 85%
“…Generally, in heavy-fermion materials, isovalent substitution of magnetic ions with non-magnetic ones leads to a crossover from a coherent Kondo lattice to the dilute Kondo impurity regime, as it was shown for Ce 1−x La x Cu 6 [53][54][55][56]. Lanthanum doping of CeB 6 suppresses both AFM and AFQ phases and induces a new multipolar-ordered phase IV beyond a quantum critical point (QCP) at x ≈ 0.3, presumably of octupolar character [57][58][59].…”
Section: Introductionmentioning
confidence: 85%
“…For example, in Ce x La 1−x Cu 6 , it is reported that LaCu 6 evolves to CeCu 6 without magnetic order and the residual resistivity has a maximum around x = 0.5. 60 The difference from the Ce x La 1−x Ru 2 Si 2 system may come from the following fact. The crystal structure of LaCu 6 is monoclinic, while that of CeCu 6 is orthorhombic at room temperature.…”
Section: Magnetic Phase Diagrams Of Cerumentioning
confidence: 99%
“…The electron-magnon coupling ͉g k ជ͉ 2 for ferromagnetic system is independent 35 of k ជ . In the limit of ប k ជ /2k B T ӷ 1, the leading term of electron-magnon resistivity in the anisotropic ferromagnetic material FM can be written as…”
Section: Appendix A: Ferromagnetic Casementioning
confidence: 99%