论文标题
非饱和磁力,异常大厅效应和磁量子振荡
Nonsaturating magnetoresistance, anomalous Hall effect, and magnetic quantum oscillations in ferromagnetic semimetal PrAlSi
论文作者
论文摘要
与其非磁性模拟Laalsi相比,我们报告了对单晶Pralsi的结构,磁,运输和热力学特性的全面研究。 Pralsi在$ t_c $ = 17.8 K处表现出铁磁过渡,但是在较低温度下是两个弱相变。基于DC和AC磁敏感性测量值,我们提出两个以下$ t_c $的磁性磁相或铁磁群集玻璃杯。当磁性玻璃状态被小场抑制时,出现了几种显着的特征。其中包括一个线性的,不饱和的磁场抗性作为场的函数,它让人联想到拓扑或电荷补偿的半学,以及大于$ \ sim $ 2000 $ω^{ - 1} $ cm $ $ cm $ $^{ - 1} $的大型异常的霍尔电导率。特定的热测量表明,非kramer双重基态和相对较低的晶体电场分裂的pr $^{3+} $少于100 k的乘数。在laalsi中,shubnikov-de Hass振荡不存在,而Laalsi则在pralsi中显然在pralsi中显然在pralsi中显然在pralsi中,均与$ usef $ n usisual pralsial pralsi uscy usectial $ nyus flation $ nyus prysection $ hass。它从25 K的$ f $ = 18吨增加到2 K的$ f $ = 33吨,暗示在冷却到有序阶段时,它暗示了新兴的费米口袋。这些结果表明,Pralsi是一个新的系统,其中一个可能的相对论费米斯的费米口袋与磁性强烈耦合。 $ F $和传统带之间是否涉及杂交仍然是一个有趣的开放问题。
We report a comprehensive investigation of the structural, magnetic, transport and thermodynamic properties of a single crystal PrAlSi, in comparison to its nonmagnetic analogue LaAlSi. PrAlSi exhibits a ferromagnetic transition at $T_C$ = 17.8 K which, however, is followed by two weak phase transitions at lower temperatures. Based on the combined dc and ac magnetic susceptibility measurements, we propose the two reentrant magnetic phases below $T_C$ to be spin glasses or ferromagnetic cluster glasses. When the magnetic glassy states are suppressed by small field, several remarkable features appear. These include a linear, nonsaturating magnetoresistance as a function of field that is reminiscent of a topological or charge-compensated semimetal, and a large anomalous Hall conductivity amounting to $\sim$2000 $Ω^{-1}$cm$^{-1}$. Specific-heat measurements indicate a non-Kramers doublet ground state and a relatively low crystal electric field splitting of the Pr$^{3+}$ multiplets of less than 100 K. Shubnikov-de Hass oscillations are absent in LaAlSi, whereas they are clearly observed below about 25 K in PrAlSi, with an unusual temperature dependence of the dominating oscillation frequency $F$. It increases from $F$ = 18 T at 25 K to $F$ = 33 T at 2 K, hinting at an emerging Fermi pocket upon cooling into the ordered phase. These results suggest that PrAlSi is a new system where a small Fermi pocket of likely relativistic fermions is strongly coupled to magnetism. Whether hybridization between $f$ and conduction band is also involved remains an intriguing open problem.