论文标题

(MN,CO)SI的物理特性

Physical properties of (Mn,Co)Si

论文作者

Petrova, A. E., Gavrilkin, S. Y., Rybalchenko, G. V., Zibrov, I. P., Stishov, S. M.

论文摘要

我们已经成长并表征了三个共掺杂的MNSI样本,并研究了它们的物理特性(磁化和磁化易感性,热容量和电阻)。所有三个样品均显示非弗米液体物理特性。从文献数据和当前的结果来看,杂质(CO和FE)消除了第一阶相变峰并扩散波动最大值,以使其低温部分有效地达到零温度,而波动不可避免地成为量子。样品的热容量低温分支的行为表明,可以通过温度的简单功率函数来描述从经典波动到量子波动的逐渐过渡,指数少于一个。 $dρ/dt $数据通常支持此建议。热容量指数的值立即导致差异$ C_P/T $,因此与有效的电子质量不同。我们发现,在大浓度的掺杂剂中,没有不同的相变点。我们观察到的是螺旋波动的云,该螺旋波动扩散在浓度范围的范围和温度范围内,它们变成接近0〜k的量子。

We have grown and characterized three samples of Co doped MnSi and studied their physical properties (magnetization and magnetic susceptibility, heat capacity and electrical resistance). All three samples show non-Fermi liquid physical properties. From literature data and current results follow that impurities (Co and Fe) eliminate the first order phase transition peaks and spread the fluctuation maxima in such a way that its low temperature part effectively reaches the zero temperature, where the fluctuations inevitably become quantum. The behavior of low temperature branches of the heat capacity of the samples suggests that a gradual transition from classical to quantum fluctuations can be described by a simple power function of temperature with the exponent less than one. The $dρ/dT$ data generally support this suggestion. The values of the heat capacity exponents immediately lead to the diverging ratio $C_p/T$ and hence to the diverging effective electron mass. We found out that at large concentration of the dopant there are no distinct phase transition points. What we observe is a cloud of the helical fluctuations spreading over a significant range of concentrations and temperatures, which become quantum close to 0~K.

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