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Ordered Magnetic Phases Of The Frustrated Spin-dimer Compound Ba_3mn_2o_8

机译:沮丧的自旋二聚体化合物Ba_3mn_2o_8的有序磁相

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摘要

Ba_3Mn_2O_8 is a spin-dimer compound based on pairs of 5-1, 3d~2, Mn~(5+) ions arranged on a triangular lattice. Antiferromagnetic intradimer exchange leads to a singlet ground state in zero field. Here we present the first results of thermodynamic measurements for single crystals probing the high-field ordered states of this material associated with closing the spin gap to the excited triplet states. Specific heat, magnetocaloric effect, and torque magnetometry measurements were performed in magnetic fields up to 32 T and temperatures down to 20 mK. For fields above H_(c1) ~ 8.7 T, these measurements reveal a single magnetic phase for H‖c but two distinct phases (approximately symmetric about the center of the phase diagram) for H ⊥ c. Analysis of the simplest possible spin Hamiltonian describing this system yields candidates for these ordered states corresponding to a simple spiral structure for H‖c and to two distinct modulated phases for H ⊥ c. Both single-ion anisotropy and geometric frustration play crucial roles in defining the phase diagram.
机译:Ba_3Mn_2O_8是基于排列在三角形晶格上的5-1、3d〜2,Mn〜(5+)离子对的自旋二聚体化合物。反铁磁性二聚体交换导致零场中的单重态基态。在这里,我们介绍了单晶热力学测量的初步结果,以探测该材料的高场有序状态,该状态与将自旋能隙闭合到激发三重态有关。比热,磁热效应和扭矩磁强法测量是在最高32 T的磁场和最低20 mK的温度下进行的。对于大于H_(c1)〜8.7 T的磁场,这些测量结果显示H′c具有单个磁相,而H′c具有两个不同的相(关于相图中心对称)。分析最简单的描述该系统的自旋哈密顿量,可以得到这些有序状态的候选项,对应于H toc的简单螺旋结构和H⊥c的两个不同调制相位。单离子各向异性和几何受挫都在定义相图中起着至关重要的作用。

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