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CePtIn近藤晶格中的稀释和非费米液体效应。

Dilution and non-Fermi-liquid effects in the CePtIn Kondo lattice.

作者信息

Ragel F C, Plessis P de V du, Strydom A M

机构信息

School of Physics, University of the Witwatersrand, Private Bag 3, PO WITS 2050, Johannesburg, South Africa. Physics Department, University of Johannesburg, PO Box 524, Aucklandpark 2006, South Africa.

出版信息

J Phys Condens Matter. 2009 Jan 28;21(4):046008. doi: 10.1088/0953-8984/21/4/046008. Epub 2009 Jan 8.

Abstract

Measurements of electrical resistivity (ρ(T)), magnetoresistivity (MR), magnetic susceptibility (χ(T)) and heat capacity (C(P)(T)) are presented for the (Ce(1-x)La(x))PtIn alloy system of which the CePtIn parent is a known dense Kondo compound that does not order magnetically down to 50 mK. χ(T) for alloys 0≤x≤0.8 exhibits Curie-Weiss behaviour. ρ(T) results indicate a transition from a dense Kondo behaviour for 0≤x≤0.2 to a single-ion Kondo region (0.3≤x≤0.8). The Kondo energy scale as given by T(K) values calculated from MR studies and by the temperature T(max)(ρ(mag)) where the magnetic contribution to ρ(T) exhibits a maximum value, is compared with theoretical models. It is shown that the experimental results not only depend on a volume effect as given by the compressible Kondo lattice model of Lavagna but in addition confirm the more complex behaviour recently presented by Burdin and Fulde for a Kondo alloy system in which the magnetic (Ce) and non-magnetic (La) atoms are distributed randomly. Non-Fermi-liquid behaviour is predicted by Burdin and Fulde at certain critical concentrations of the alloy system and experimental evidence for this is presented through χ(T), ρ(T) and C(P)(T) measurements.

摘要

本文给出了(Ce(1-x)La(x))PtIn合金体系的电阻率(ρ(T))、磁电阻率(MR)、磁化率(χ(T))和热容(C(P)(T))的测量结果。其中,母体CePtIn是一种已知的致密近藤化合物,在低至50 mK的温度下不会发生磁有序。对于0≤x≤0.8的合金,χ(T)表现出居里-外斯行为。ρ(T)的结果表明,从0≤x≤0.2的致密近藤行为转变为单离子近藤区域(0.3≤x≤0.8)。将由MR研究计算得到的T(K)值以及磁对ρ(T)贡献呈现最大值时的温度T(max)(ρ(mag))所给出的近藤能量标度与理论模型进行了比较。结果表明,实验结果不仅取决于Lavagna的可压缩近藤晶格模型所给出的体积效应,而且还证实了Burdin和Fulde最近提出的一种近藤合金体系更为复杂的行为,其中磁性(Ce)和非磁性(La)原子随机分布。Burdin和Fulde预测在合金体系的某些临界浓度下会出现非费米液体行为,并通过χ(T)、ρ(T)和C(P)(T)测量给出了相关实验证据。

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