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Quantum magnetisms in uniform triangular lattices Li2AMo3O8 (A = In Sc)

机译:均匀三角形格子Li2AMo3O8(A = InSc)中的量子磁性

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摘要

Molecular based spin-1/2 triangular lattice systems such as LiZn2Mo3O8 have attracted research interest. Distortions, defects, and intersite disorder are suppressed in such molecular-based magnets, and intrinsic geometrical frustration gives rise to unconventional and unexpected ground states. Li2AMo3O8 (A = In or Sc) is such a compound where spin-1/2 Mo3O13 clusters in place of Mo ions form the uniform triangular lattice. Their ground states are different according to the A site. Li2InMo3O8 undergoes conventional 120° long-range magnetic order below TN = 12 K whereas isomorphic Li2ScMo3O8 exhibits no long-range magnetic order down to 0.5 K. Here, we report exotic magnetisms in Li2InMo3O8 and Li2ScMo3O8 investigated by muon spin rotation (μSR) and inelastic neutron scattering (INS) spectroscopies using polycrystalline samples. Li2InMo3O8 and Li2ScMo3O8 show completely different behaviors observed in both μSR and INS measurements, representing their different ground states. Li2InMo3O8 exhibits spin wave excitation which is quantitatively described by the nearest neighbor anisotropic Heisenberg model based on the 120° spin structure. In contrast, Li2ScMo3O8 undergoes short-range magnetic order below 4 K with quantum-spin-liquid-like magnetic fluctuations down to the base temperature. Origin of the different ground states is discussed in terms of anisotropies of crystal structures and magnetic interactions.
机译:基于分子的自旋1/2三角晶格系统(例如LiZn2Mo3O8)引起了研究兴趣。在这种基于分子的磁体中,畸变,缺陷和位点间的杂乱得到了抑制,并且固有的几何受挫导致非常规的和出乎意料的基态。 Li 2 AMo 3 O 8(A 1 = In或Sc)是这样的化合物,其中自旋1/2 Mo 3 O 13簇代替Mo离子形成均匀的三角形晶格。根据A站点,它们的基态不同。 Li2InMo3O8在TN = 12 K以下经历常规的120°长程磁序,而同构Li2ScMo3O8在低至0.5 K时没有长程磁序。在这里,我们报道Li2InMo 3 O 中的外来磁性利用μon自旋旋转(μSR)和非弹性中子散射(INS)光谱学研究8 和Li 2 ScMo 3 O 8 多晶样品。 Li 2 InMo 3 O 8 和Li 2 ScMo 3 O 图8 显示了在μSR和INS测量中观察到的完全不同的行为,表示它们的不同基态。 Li 2 InMo 3 O 8 表现出自旋波激发,其由基于120°自旋结构的最近邻各向异性海森堡模型定量描述。相比之下,Li 2 ScMo 3 O 8 在4 K以下经历短程磁阶,量子自旋液体状磁波动下降到基准温度。根据晶体结构的各向异性和磁相互作用来讨论不同基态的起源。

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