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Neutron Powder Diffraction Study on the Crystal and Magnetic Structures of BiCrO3

机译:BiCrO3晶体和磁性结构的中子粉末衍射研究

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摘要

The crystal and magnetic structures of poly crystalline BiCrO3 were determined by the Rietveld method from neutron diffraction data measured at temperatures from 7 to 490 K. BiCrO3 crystallizes in the orthorhombic system above 420 K (space group Pnma; Z = 4; a = 5.54568(12) A, b = 7.7577(2) A, and c = 5.42862(12) A at 490 K) in the GdFeO3-type structure. Below 420 K down to 7 K, a monoclinic structure is stable with C2/c symmetry (a = 9.4641(4) A, b = 5.4790(2) A, c = 9.5850(4) A, and β = 108.568(3)° at 7 K). A possible model for antiferromagnetic order below T_N = 109 K is proposed with a propagation vector of k = (0, 0, 0). In this model, magnetic moments of Cr~(3+) ions are coupled antiferromagnetically in all directions, forming a G-type antiferromagnetic structure. Refined magnetic moments at 7, 50, and 80 K are 2.55(2)μ_B, 2.43(2)μ_B, and 2.09(2)μ_B, respectively. The structure refinements revealed no deviation from stoichiometry in BiCrO3.
机译:多晶BiCrO3的晶体和磁性结构是通过Rietveld方法根据在7至490 K温度下测量的中子衍射数据确定的。Z = 4;在 490 K) 时,a = 5.54568(12) A、b = 7.7577(2) A、c = 5.42862(12) A,在 490 K) 时为 GdFeO3 型结构。在420 K以下至7 K,单斜晶系结构稳定,C2/c对称性(7 K时a = 9.4641(4) A,b = 5.4790(2) A,c = 9.5850(4) A,β = 108.568(3)°)。提出了低于 T_N = 109 K 的反铁磁阶数的可能模型,传播矢量为 k = (0, 0, 0)。该模型中,Cr~(3+)离子的磁矩在各个方向上反铁磁耦合,形成G型反铁磁结构。7、50 和 80 K 的精细磁矩分别为 2.55(2)μ_B、2.43(2)μ_B 和 2.09(2)μ_B。结构改进显示 BiCrO3 与化学计量没有偏差。

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