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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Various disordered ground states and 1/3 magnetization-plateau-like behavior in the S=1/2 Ti~(3+) kagome lattice antiferromagnets Rb_2NaTi_3F_(12), Cs_2NaTi_3F_(12), and Cs_2KTi_3F_(12)
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Various disordered ground states and 1/3 magnetization-plateau-like behavior in the S=1/2 Ti~(3+) kagome lattice antiferromagnets Rb_2NaTi_3F_(12), Cs_2NaTi_3F_(12), and Cs_2KTi_3F_(12)

机译:S = 1/2 Ti〜(3+)kagome晶格反铁磁体Rb_2NaTi_3F_(12),Cs_2NaTi_3F_(12)和Cs_2KTi_3F_(12)中的各种无序基态和1/3磁化高原行为

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摘要

We have investigated the crystal structure and magnetic properties of three kagome lattice antiferromagnets, Rb_2NaTi_3F_(12), Cs_2NaTi_3F_(12), and Cs_2KTi_3F_(12), using single crystals. These compounds represent a 5 = 1/2 kagome system consisting of magnetic Ti~(3+) ions, which is expected to have negligibly small Dzyaloshinsky-Moriya interaction. The structural analyses revealed that each of the three compounds has a slightly distorted kagome lattice. The distortion of the kagome lattice becomes small as the ionic radii of constituent alkali metals increase. All three compounds have nearly the same Weiss temperature of -45 K, and the ground states are disordered and strongly depend on the distortion. The ground states of Rb_2NaTi_3F_(12), Cs_2NaTi_3F_(12), and Cs_2KTi_3F_(12) are found to be a two-component state including approximately 1/3 nearly free spins, a gapless disordered state, and a gapped disordered state, respectively. Our experimental results suggest that the ground state of the ideal S = 1/2 Heisenberg kagome lattice antiferromagnet is gapped. In addition, the magnetization curves of Cs_2NaTi_3F_(12), and Cs_2KTi_3F_(12) show anomalies at approximately 1/3 of the full magnetic moment of Ti3+, which are a notable observation of signs of the theoretically proposed 1/3 magnetization plateau in S = 1/2 kagome antiferromagnets.
机译:我们已经使用单晶研究了三种Kagome晶格反铁磁体Rb_2NaTi_3F_(12),Cs_2NaTi_3F_(12)和Cs_2KTi_3F_(12)的晶体结构和磁性。这些化合物代表由磁性Ti〜(3+)离子组成的5 = 1/2 kagome系统,预计其Dzyaloshinsky-Moriya相互作用很小。结构分析表明,这三种化合物中的每一种均具有稍微扭曲的kagome晶格。随着组成碱金属的离子半径增加,kagome晶格的变形变小。这三种化合物的Weiss温度几乎都相同,为-45 K,基态是无序的,并且强烈依赖于畸变。发现Rb_2NaTi_3F_(12),Cs_2NaTi_3F_(12)和Cs_2KTi_3F_(12)的基态分别是包括大约1/3的近自由自旋,无间隙无序状态和带隙无序状态的两组分状态。我们的实验结果表明,理想的S = 1/2 Heisenberg kagome晶格反铁磁体的基态存在缺口。此外,Cs_2NaTi_3F_(12)和Cs_2KTi_3F_(12)的磁化曲线在Ti3 +的全磁矩的大约1/3处显示出异常,这是理论上提出的S中1/3磁化高原迹象的显着观察。 = 1/2 kagome反铁磁体。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2016年第10期|104432.1-104432.10|共10页
  • 作者单位

    Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan;

    Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan;

    Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan;

    Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan;

    Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan;

    Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan,Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan;

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