Abstract

The orthorhombic compound NdFe2_2Al10_{10} has been studied by powder and single-crystal neutron diffraction. Below TNT_N = 3.9 K, the Nd3+^{3+} magnetic moments order in a double-kk [k1=(0,34,0)\mathbf{k}_1 = (0, \frac{3}{4}, 0), k2=(0,14,0)\mathbf{k}_2 = (0, \frac{1}{4}, 0)] collinear magnetic structure, whose unit cell consists of four orthorhombic units in the bb direction.The refinements show that this structure consists of (0 1 0) ferromagnetic planes stacked along bb, in which the moments are oriented parallel to aa (the easy anisotropy axis according to bulk magnetization measurements) and nearly equal in magnitude (≈1.7−1.9 μB\approx 1.7-1.9\ μ_B). The alternating 8-plane sequence providing the best agreement to the data turns out to be that which yields the lowest exchange energy if one assumes antiferromagnetic near-neighbor exchange interactions with J1≫J2,J3J_1 \gg J_2, J_3. With increasing temperature, the single-crystal measurements indicate the suppression of the k2\mathbf{k}_2 component at T=2.7T = 2.7 K, supporting the idea that the anomalies previously observed around 2--2.5 K result from a squaring transition. In a magnetic field applied along the aa axis, the magnetic Bragg satellites disappear at Hc=2.45H_c = 2.45 T, in agreement with earlier measurements. Comparisons are made with related magnetic orders occurring in CeT2T_2Al10_{10} (TT: Ru, Os) and TbFe2_2Al10_{10}.

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