1996
DOI: 10.1007/bf02570277
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Low temperature hall effect and thermopower of YbCu4Au and YbCu4Pd

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“…5, 6, and 7͒ show a striking similarity to those of YbCu 4 Au and YbCu 4 Pd. 20,31,32 The latter compounds are described as magnetic KL systems with transition temperatures T N Ͻ1 K, 33 Kondo temperatures T K Ӎ0.5 K, 34 and low-lying CEF excited levels separated by an energy ⌬ CEF Ӎ45 K from the GS doublet. 34 We propose that in the case of Yb 2 Rh 3 Al 9 and Yb 2 Ir 3 Al 9 the respective hightemperature maxima in (T) and minima in TEP are due to the interaction of Kondo-type incoherent scattering on lowlying CEF levels situated at ⌬ CEF Ӎ30 K. This is supported by the features observed in the transport properties, where Kondo-type correlations are responsible for the enhanced logarithmic increase of (T) and the enhanced negative values of TEP ͑cf.…”
Section: Analysis and Discussionmentioning
confidence: 99%
“…5, 6, and 7͒ show a striking similarity to those of YbCu 4 Au and YbCu 4 Pd. 20,31,32 The latter compounds are described as magnetic KL systems with transition temperatures T N Ͻ1 K, 33 Kondo temperatures T K Ӎ0.5 K, 34 and low-lying CEF excited levels separated by an energy ⌬ CEF Ӎ45 K from the GS doublet. 34 We propose that in the case of Yb 2 Rh 3 Al 9 and Yb 2 Ir 3 Al 9 the respective hightemperature maxima in (T) and minima in TEP are due to the interaction of Kondo-type incoherent scattering on lowlying CEF levels situated at ⌬ CEF Ӎ30 K. This is supported by the features observed in the transport properties, where Kondo-type correlations are responsible for the enhanced logarithmic increase of (T) and the enhanced negative values of TEP ͑cf.…”
Section: Analysis and Discussionmentioning
confidence: 99%