论文标题

R2RHSI3(r = gd,tb和dy)中的磁和传输异常,类似于外来磁性天空GD2PDSI3

Magnetic and transport anomalies in R2RhSi3 (R= Gd, Tb, and Dy), resembling those of an exotic magnetic skyrmion Gd2PdSi3

论文作者

Kumar, Ram, Iyer, Kartik K, Paulose, P. L., Sampathkumaran, E. V.

论文摘要

我们已经对金属间化合物的多晶形式,R2RHSI3(R = GD,TB和DY)进行了磁化,热容量,电气和磁化测量测量(2-300 K),在Alb2衍生的六边形结构中形成,具有三角形R网络。这项工作主要是由于磁性天际造成的大约二十年的五十年之后,对GD2PDSI3的兴趣复兴。我们在这里报告说,这些化合物的特征是双反铁磁转变(GD的T_N = 13.5和12 K,TB的13.5和6.5 k;对于Dy的6.5和2.5),但抗Fiferromagnerism似乎很复杂。所有这些化合物共有的最显着的观察结果是:(i)数据中有许多模仿GD2PDSI3的特征,包括等温磁化的两个场诱导的变化,好像有两个元磁过渡远低于T_N。鉴于这种性质的这种相似之处,我们推测这些基于RH的材料为研究中心对称结构中的仔细综合大厅效应提供了一个很好的操场,其起源位于磁性磁性的三角形晶格中。 (ii)在所有情况下,电子散射随温度降低的贡献,与GD2PDSI3相似,因此作为由于几何沮丧而导致金属系统中经典自旋液相的理论预测的示例。

We have carried out magnetization, heat capacity, electrical and magnetoresistance measurements (2-300 K) for the polycrystalline form of intermetallic compounds, R2RhSi3 (R= Gd, Tb, and Dy), forming in a AlB2 derived hexagonal structure with a triangular R network. This work was primarily motivated by a revival of interest on Gd2PdSi3 after about two decades in the field of Toplogical Hall Effect due to magnetic skyrmions. We report here that these compounds are characterized by double antiferromagnetic transitions (T_N= 13.5 and 12 K for Gd, 13.5 and 6.5 K for Tb; 6.5 and 2.5 for Dy), but antiferromagnerism seems to be complex. The most notable observations common to all these compounds are: (i) There are many features in the data mimicking those seen for Gd2PdSi3, including the two field-induced changes in isothermal magnetization as though there are two metamagnetic transitions well below T_N. In view of such a resemblance of the properties, we speculate that these Rh-based materials offer a good playground to study toplogical Hall effect in a centrosymmetric structure, with its origin lying in triangular lattice of magnetic R ions; (ii) There is an increasing contribution of electronic scattering with decreasing temperature towards T_N in all cases, similar to Gd2PdSi3, thereby serving as examples for a theoretical prediction for a classical spin-liquid phase in metallic systems due to geometrical frustration.

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