Colin Claire V, Tao Quanzheng, Opagiste Christine, Balou Rafik, Rosen Johanna, Ouisse Thierry, Petříček Václav
Institut Néel, Université Grenoble Alpes & CNRS, Grenoble, 38042, France.
Department of Physics, Chemistry and Biology (IFM), Linkopings Universitet, Linköping, SE-58183, Sweden.
Acta Crystallogr B Struct Sci Cryst Eng Mater. 2025 Feb 1;81(Pt 1):37-46. doi: 10.1107/S2052520624011053. Epub 2025 Jan 23.
The magnetic structures of the Ho-based i-MAX phase (MoHo)GaC were studied with neutron powder diffraction at low temperature. (MoHo)GaC crystallizes in the orthorhombic space group Cmcm. The material undergoes two successive antiferromagnetic transitions at T = 10 K and T = 7.2 K. The magnetic structure below T is incommensurate with the propagation vector k = (0, k, 0) with k = 0.696 (1) at 9 K. For the analysis of the magnetic structure, a group-theoretical approach based on the space group of the nuclear structure and its subgroups was employed. A model in the (3+1)D superspace group Cmcm.1'(0β0)s0ss yielded the most accurate results in neutron powder diffraction refinements. The determined structure was found to be an incommensurate longitudinal amplitude-modulated magnetic structure. Below T, additional magnetic satellites develop. They could be indexed by a propagation vector k = (τ, 0, 0) with the τ value increasing below T until it stabilizes at approximately 3 K at 0.075. A magnetic structure determination considering two propagation vectors k and k was carried out using the superspace formalism by building the corresponding (3+2)D model. The determination was based on the observation that the additional magnetic peaks emerge exclusively in the vicinity of the incommensurate magnetic peaks with propagation vector k, and not in the vicinity of nuclear peaks. This indicates that only mixed-index reflections were observed, and not reflections purely related to k. The magnetic superspace group (MSSG) that was determined is Amma.1' (0,β,0)00s0 (0,0,γ)ss0s. The structure can be described as a longitudinal amplitude-modulated structure, which itself is amplitude-modulated in a perpendicular direction. This represents a very unusual case of a 2-k magnetic structure with no symmetry relation between the propagation vectors.
在低温下,利用中子粉末衍射对Ho基i-MAX相(MoHo)GaC的磁性结构进行了研究。(MoHo)GaC结晶于正交空间群Cmcm。该材料在T = 10 K和T = 7.2 K时经历两次连续的反铁磁转变。低于T时的磁性结构与传播矢量k = (0, k, 0) 非公度,在9 K时k = 0.696 (1)。为了分析磁性结构,采用了基于核结构空间群及其子群的群论方法。在(3 + 1)D超空间群Cmcm.1'(0β0)s0ss中的一个模型在中子粉末衍射精修中给出了最准确的结果。确定的结构是一种非公度纵向振幅调制磁性结构。低于T时,会出现额外的磁性卫星峰。它们可以用传播矢量k = (τ, 0, 0) 进行索引,τ值在低于T时增加,直到在大约3 K时稳定在0.075。通过构建相应的(3 + 2)D模型,使用超空间形式主义对考虑两个传播矢量k和k的磁性结构进行了确定。该确定基于这样的观察:额外的磁性峰仅出现在具有传播矢量k的非公度磁性峰附近,而不出现在核峰附近。这表明只观察到了混合指数反射,而没有纯粹与k相关的反射。确定的磁性超空间群(MSSG)是Amma.1' (0,β,0)00s0 (0,0,γ)ss0s。该结构可以描述为一种纵向振幅调制结构,其本身在垂直方向上进行振幅调制。这代表了一种非常特殊的2-k磁性结构情况,其中传播矢量之间没有对称关系。