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Magnetic ordering in the quaternary R2Fe2Si2C (R = Y, Gd - Tm) intermetallic compounds

机译:四元R2Fe2Si2C(R = Y,Gd-Tm)金属间化合物中的磁性排序

摘要

The magnetic ordering of the quaternary R2Fe2Si2C (Y, Gd - Tm) compounds which crystallise in the monoclinic Dy2Fe2Si2C -type structure (C2/m space group), have been studied. The studies encompass the low temperature structural, thermal and magnetic properties of R2Fe2Si2C (Gd - Tm) and the determination of their magnetic structures. The fundamental goals of this study are to understand the interplay between the exchange interaction and the crystal field effects, relevant to the overall magnetic properties, and to determine whether or not the Fe sublattice is magnetically ordered in this series of compounds.The determination of the magnetic properties of these compounds reveals two important results: (i) Gd2Fe2Si2C orders at TN = 39 K, much higher than the previously reported value of TN ~ 9 K and (ii) Dy2Fe2Si2C exhibits two magnetic transitions at low temperatures. Systematic studies on the magnetic properties of this series of compounds show that the ordering temperatures of the R2Fe2Si2C (R = Gd - Tm) compounds deviate from the expected de Gennes scaling. This deviation can be described fully if both the exchange interaction and the crystal field effect are taken into account, indicating the significant influence of the crystal field in this series.Three types of magnetic structure were found to exist in this series of compounds. While the common magnetic structure of the R2Fe2Si2C (R = Gd - Ho) compounds involves ordering of the R sublattice along the b-axis with a propagation vector k1 = [0, 0, 1/2], the magnetic structures of Er2Fe2Si2C and Tm2Fe2Si2C are characterised by the propagation vectors k2 = [1/2 , 1/2 , 0] and k3 = [0.403(1), 1/2 ,0], respectively, with the R moments lying in the ac-plane. The origin of the evolution of magnetic structure across this series is discussed, revealing that crystal field effects play an important role in modifying the propagation vector, as well as defining the direction of the R moment.Neutron diffraction refinements alone were unable to answer the question of whether or not the Fe is magnetic in R2Fe2Si2C. However, 57Fe Mossbauer experiments provide the first unequivocal evidence that the Fe atom is non-magnetic in any member of the R2Fe2Si2C compounds.
机译:研究了在单斜Dy2Fe2Si2C型结构(C2 / m空间群)中结晶的四级R2Fe2Si2C(Y,Gd-Tm)化合物的磁序。研究包括R2Fe2Si2C(Gd-Tm)的低温结构,热和磁性能以及其磁结构的确定。这项研究的基本目标是了解与整体磁性有关的交换相互作用和晶体场效应之间的相互作用,并确定在这一系列化合物中Fe亚晶格是否磁性有序。这些化合物的磁性能显示出两个重要结果:(i)TN = 39 K时的Gd2Fe2Si2C阶数,大大高于先前报道的TN〜9 K的值;(ii)Dy2Fe2Si2C在低温下表现出两个磁跃迁。对这一系列化合物的磁性的系统研究表明,R2Fe2Si2C(R = Gd-Tm)化合物的有序温度偏离了预期的de Gennes标度。如果同时考虑交换相互作用和晶体场效应,则可以充分描述该偏差,表明该系列中的晶体场具有显着影响。该系列化合物中存在三种类型的磁性结构。尽管R2Fe2Si2C(R = Gd-Ho)化合物的共同磁性结构涉及沿传播轴k1 = [0、0、1 / 2]的b子晶格沿b轴排序,但Er2Fe2Si2C和Tm2Fe2Si2C的磁性结构分别由传播矢量k2 = [1/2,1/2,0]和k3 = [0.403(1),1/2,0]来表征,R矩位于交流平面。讨论了整个系列中磁性结构演化的起源,揭示了晶体场效应在修改传播矢量以及定义R矩的方向方面起着重要作用。仅中子衍射法无法解决这个问题Fe在R2Fe2Si2C中是否是磁性的。然而,57Fe Mossbauer实验提供了第一个明确的证据,即R 2 Fe 2 Si 2 C化合物的任何成员中Fe原子都是非磁性的。

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