Abstract

We measured the low-temperature specific heat Cp, resistivity ρ, and magnetoresistance Δρ(H)/ρ(0) for amorphous Ce50Al50 synthesized by a DC high-rate sputter method. The low-temperature Cp (T < 2 K) decreases rapidly toward 0 K and has no indication of phase transition. The value of γ0 which is extrapolated down to 0 K of the Cp/T is 117 mJ/molK2. The temperature dependence of ρ increases with decreasing temperature down to 0.6 K. We found that both a weak localization effect and a coherent Kondo state might be realized in the low-temperature region for the present alloy from the conductivity analysis. Furthermore, in the low-temperature ρ, a T2 term with a very large coefficient A was observed. The ratio of A/γ02 is 0.63 ×10-5 (μΩcm/K2)/(mJ/molK2)2 and is near the value of typical Ce-based heavy-fermion compounds. The magnetoresistances Δρ(H)/ρ(0) at 0.5 K and 2 K are almost constant in the magnetic field region of H < 10 kOe. We considered that the negative magnetoresistance effect is due to the weak localization and the positive magnetoresistance to the heavy-fermion state in the present alloy.

Highlights

  • Research on the physical properties of strongly correlated electron systems has been conducted on high-quality single crystal samples and on disordered systems

  • The low-temperature transport properties of Ce–Al bulk-metallic glasses synthesized by single-roller melt spinning were investigated by Zeng et al.[1]. They have indicated that the competition between the Kondo effect and the Ruderman–Kittel–Kasuya–Yoshida (RKKY) interaction is caused by the variation in the Ce concentration or the magnetic field

  • As we have found the large γ0 from the specific heat, the -log T dependence of ρ suggests the formation of a dense Kondo state at the low-temperature a-Ce50Al50

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Summary

Introduction

Research on the physical properties of strongly correlated electron systems has been conducted on high-quality single crystal samples and on disordered systems (quasicrystals, amorphous). A Ce–Al bulk-metallic glass is a typical example. The low-temperature transport properties of Ce–Al bulk-metallic glasses synthesized by single-roller melt spinning were investigated by Zeng et al.[1] They have indicated that the competition between the Kondo effect and the Ruderman–Kittel–Kasuya–Yoshida (RKKY) interaction is caused by the variation in the Ce concentration or the magnetic field. CeAl bulk-metallic glasses have various characteristics such as interaction change with Ce concentration, localization or delocalization of 4f -electrons, and magnetic transition by a new metastable phase

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