2004
DOI: 10.1016/j.jmmm.2003.12.1154
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Transport properties of Yb0.8Y0.2InCu4 under high pressure

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Cited by 2 publications
(2 citation statements)
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“…An application of pressure shifts T v (P ) to lower temperatures 41,42,43,44 without changing the properties of the hightemperature state. For T ≥ T v (P ), the susceptibility and the specific heat of YbInCu 4 can be explained by the crystal field (CF) theory of independent f states 45 split by ∆ CF ≃ 40 K into an excited quartet and two nearly degenerate doublets.…”
Section: The T0 ≫Tk Casementioning
confidence: 99%
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“…An application of pressure shifts T v (P ) to lower temperatures 41,42,43,44 without changing the properties of the hightemperature state. For T ≥ T v (P ), the susceptibility and the specific heat of YbInCu 4 can be explained by the crystal field (CF) theory of independent f states 45 split by ∆ CF ≃ 40 K into an excited quartet and two nearly degenerate doublets.…”
Section: The T0 ≫Tk Casementioning
confidence: 99%
“…Since the specific heat coefficient and the A coefficient of the resistivity are much larger for P ≥ P c than for P ≤ P c , we speculate that the transition in the MO phase is accompanied by an increase of Kondo coupling. As regards the doping, replacing Yb with Y or Lu ions 42,47 produces similar effects as pressure, i.e., doping stabilizes the LM configuration and shifts T c to lower temperatures. In Eu-based intermetallics, the valence-change transition exhibits similar features 11,12 as in YbInCu 4 , except T v is higher (T v ≥ 100 K) and the valence state of Eu ions changes almost completely [from 2 + (f 7 ) to 3 + (f 6 )].…”
Section: The T0 ≫Tk Casementioning
confidence: 99%