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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Partially disordered antiferromagnetism and multiferroic behavior in a frustrated Ising system CoCl_2-2SC(NH_2)_2
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Partially disordered antiferromagnetism and multiferroic behavior in a frustrated Ising system CoCl_2-2SC(NH_2)_2

机译:沮丧的Ising系统CoCl_2-2SC(NH_2)_2中的部分无序反铁磁性和多铁性行为

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摘要

We investigate partially disordered antiferromagnetism in CoCl_2-2SC(NH_2)_2, in which ab-plane hexagonal layers are staggered along the c axis rather than stacked. A robust 1β state forms in applied magnetic fields in which the spins are locked, varying as a function of neither temperature nor field. By contrast, in zero field and applied fields at higher temperatures, partial antiferromagnetic order occurs, in which free spins are available to create a Curie-like magnetic susceptibility. We report measurements of the crystallographic structure and the specific heat, magnetization, and electric polarization down to T = 50 mK and up to μ_0H = 60 T. The Co~(2+) S = 3/2 spins are Ising-like and form distorted hexagonal layers. The Ising energy scale is well separated from the magnetic exchange, and both energy scales are accessible to the measurements, allowing us to cleanly parametrize them. In transverse fields, a quantum Ising phase transition can be observed at 2 T. Finally, we find that magnetic exchange striction induces changes in the electric polarization up to 3 μC/m~2, and single-ion magnetic anisotropy effects induce a much larger electric polarization change of 300 μC/m~2.
机译:我们研究CoCl_2-2SC(NH_2)_2中的部分无序反铁磁性,其中ab平面六边形层沿c轴错开而不是堆叠。在所施加的磁场中,自旋被锁定,形成稳健的1β状态,并且既不随温度变化也不随磁场变化。相反,在较高温度下的零磁场和外加磁场中,会出现部分反铁磁序,其中自由自旋可用于产生居里样的磁化率。我们报告了晶体结构和比热,磁化强度和低至T = 50 mK且至μ_0H= 60 T的电极化的测量结果。Co〜(2+)S = 3/2自旋呈伊辛型并形成六角形扭曲的层。伊辛能级与磁交换良好地分开,并且两个能级均可用于测量,从而使我们能够对它们进行干净的参数化。在横向场中,可以在2 T处观察到量子Ising相变。最后,我们发现,磁交换收缩引起的极化变化高达3μC/ m〜2,而单离子磁各向异性效应引起的极化更大。极化变化为300μC/ m〜2。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2016年第10期|104407.1-104407.8|共8页
  • 作者单位

    National High Magnetic Field Laboratory, Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA ,Simon Frazer University, Burnaby, British Columbia, Canada V5A 1S6;

    Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    National High Magnetic Field Laboratory, Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA ,Rutgers Center for Emergent Materials, Piscataway, NJ 08854, USA;

    Materials Physics and Applications 11, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA ,National Institute of Materials Physics, 077125 Bucharest-Magurele, Romania;

    Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Department of Chemistry and Biochemistry, Eastern Washington University, Cheney, Washington 99004, USA;

    Department of Chemistry and Biochemistry, Eastern Washington University, Cheney, Washington 99004, USA;

    National High Magnetic Field Laboratory, Materials Physics and Applications-Condensed Matter and Magnetic Science, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

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