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Neutron diffraction study of the magnetic ordering in the series R_2BaNiO_5 (R = Rare Earth)

机译:R_2BaNiO_5序列(R =稀土)中的磁序的中子衍射研究

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A neutron diffraction study, as a function of temperature, of the title compounds is presented. The whole family (space group Immm, a ≈ 3.8 A, b ≈ 5.8 A, c ≈ 11.3 A) is structurally characterised by the presence of flattened NiO_6 octahedra that form chains along the a-axis, giving rise to a strong Ni-O-Ni antiferromagnetic interaction. Whereas for Y-compound only strong 1D correlations exist above 1.5 K, presenting the Haldane gap characteristic of 1D AF chain with integer spin, 3D AF ordering is established simultaneously for both R and Ni sublattices at temperatures depending on the rare earth size and magnetic moment. The magnetic structures of R_2BaNiO_5 (R = Nd, Tb, Dy, Ho, Er and Tm) have been determined and refined as a function of temperature. The whole family orders with a magnetic structure characterised by the temperature-independent propagation vector k = (1/2, 0, 1/2). At 1.5 K the directions of the magnetic moments differ because of the different anisotropy of the rare earth ions. Except for Tm and Yb (which does not order above 1.5 K), the magnetic moment of the R~(3+) cations are close to the free-ion value. The magnetic moment of Ni~(2+) is around 1.4 μ_B, the strong reduction with respect to the free-ion value is probably due to a combination of low-dimensional quantum effects and covalency. The thermal evolution of the magnetic structures from T_N down to 1.5 K is studied in detail. A smooth re-orientation, governed by the magnetic anisotropy of R~(3+), seems to occur below and very close to T_N in some of these compounds: the Ni moment rotates from nearly parallel to the a-axis toward the c-axis following the R moments. We demonstrate that for setting up the 3D magnetic ordering the R-R exchange interactions cannot be neglected.
机译:给出了标题化合物随温度变化的中子衍射研究。整个家庭(空间群Immm,a≈3.8 A,b≈5.8 A,c≈11.3 A)的结构特征是存在扁平的NiO_6八面体,沿a轴形成链,从而产生强的Ni-O -Ni反铁磁相互作用。而对于Y化合物,在1.5 K以上仅存在强1D相关性,这表明1D AF链具有整数自旋的Haldane间隙特征,而R和Ni亚晶格在取决于稀土尺寸和磁矩的温度下同时建立了3D AF有序化。 R_2BaNiO_5的磁性结构(R = Nd,Tb,Dy,Ho,Er和Tm)已确定并随温度变化而细化。整个家庭订购的磁性结构的特征是与温度无关的传播矢量k =(1/2,0,1/2)。在1.5 K时,由于稀土离子的各向异性不同,磁矩的方向也不同。除Tm和Yb(在1.5 K以上不排序)外,R〜(3+)阳离子的磁矩接近于自由离子值。 Ni〜(2+)的磁矩约为1.4μB,相对于自由离子值的大幅降低可能归因于低维量子效应和共价性的结合。详细研究了磁性结构从T_N到1.5 K的热演化。在某些化合物中,由R〜(3+)的磁各向异性控制的平滑重取向似乎发生在T_N以下且非常接近T_N:Ni力矩从几乎平行于a轴的方向旋转到c-轴跟随R力矩。我们证明,对于设置3D磁性排序,R-R交换相互作用不可忽略。

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