Klicpera Milan, Adroja Devashibhai T, Vlášková Kristina, Boehm Martin, Mutka Hannu, Ouladdiaf Bachir, Guidi Tatiana, Javorský Pavel
Charles University , Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 12116 Prague 2, Czech Republic.
ISIS Facility, Rutherford Appleton Laboratory , Chilton, Didcot, Oxon OX11 0QX, United Kingdom.
Inorg Chem. 2017 Nov 6;56(21):12839-12847. doi: 10.1021/acs.inorgchem.7b01521. Epub 2017 Oct 6.
CeCuAl crystallizing in the tetragonal BaNiSn-type structure and CeCuAl solid solutions were investigated by means of elastic and inelastic neutron scattering. Powder neutron diffraction brought information on both temperature evolution of crystallographic parameters and magnetic order at low temperatures. No structural change was observed in the investigated temperature range from 1.5 to 300 K. Weak magnetic peaks outside nuclear Bragg positions observed in solid solutions with 0.90 ≤ x ≤ 1.10 were described by the propagation vector k = (0.40 + δ, 0.60 + δ, 0), where δ ≈ 0.02 and δ ≈ 0.01. The magnetic structure of CeCuAl consists of two components: an anti-ferromagnetic one described by the same k and a ferromagnetic one with k = (0, 0, 0) and magnetic moments lying within the tetragonal basal plane. The evolution of magnetic excitations as a function of Cu-Al concentration in CeCuAl was studied by inelastic neutron scattering. The measured spectra of CeCuAl and the solution with x = 0.95 point to a three-magnetic-peak energy scheme, while only two excitations are expected from the local symmetry conditions on Ce atoms. The standard two-peak spectrum of crystal electric field excitations was observed for Cu-Al substitutions further from the 1:1:3 stoichiometry (x = 0.75 and 1.10). The intermediate concentrations (x = 0.90 and 1.05) exhibit spectra on the border between the former cases with a less clear pronounced first inelastic magnetic peak. The observed behavior is discussed considering the evolution of structural parameters in the CeCuAl system and the coupling between the lattice vibrations and the crystal electric field excitations.
通过弹性和非弹性中子散射研究了以四方BaNiSn型结构结晶的CeCuAl及其固溶体。粉末中子衍射给出了低温下晶体学参数的温度演化和磁有序的信息。在1.5至300 K的研究温度范围内未观察到结构变化。在0.90≤x≤1.10的固溶体中,在核布拉格位置之外观察到的弱磁峰由传播矢量k = (0.40 + δ, 0.60 + δ, 0)描述,其中δ≈0.02且δ≈0.01。CeCuAl的磁结构由两个分量组成:一个由相同k描述的反铁磁分量和一个k = (0, 0, 0)且磁矩位于四方基面内的铁磁分量。通过非弹性中子散射研究了CeCuAl中磁激发随Cu - Al浓度的演化。CeCuAl及其x = 0.95的固溶体的测量光谱指向一个三磁峰能量方案,而根据Ce原子的局部对称条件仅预期有两个激发。对于偏离1:1:3化学计量比(x = 0.75和1.10)的Cu - Al替代,观察到了晶体电场激发的标准双峰光谱。中间浓度(x = 0.90和1.05)的光谱处于前两种情况之间的边界,第一个非弹性磁峰不太明显。考虑到CeCuAl系统中结构参数的演化以及晶格振动与晶体电场激发之间的耦合,对观察到的行为进行了讨论。