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首页> 外文期刊>Nature Materials >Room-temperature antiskyrmions and sawtooth surface textures in a non-centrosymmetric magnet with S_4 symmetry
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Room-temperature antiskyrmions and sawtooth surface textures in a non-centrosymmetric magnet with S_4 symmetry

机译:使用S_4对称性的非Centroosmmetric磁体中的房间温度的防误和锯齿纹理

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摘要

Topological spin textures have attracted much attention both for fundamental physics and spintronics applications. Among them, antiskyrmions possess a unique spin configuration with Bloch-type and Neel-type domain walls owing to anisotropic Dzyaloshinskii-Moriya interaction in the non-centrosymmetric crystal structure. However, antiskyrmions have thus far only been observed in a few Heusler compounds with D_(2d) symmetry. Here we report a new material, Fe_(1.9)Ni_(0.9)Pd_(0.2)P, in a different symmetry class (S_4), in which antiskyrmions exist over a wide temperature range that includes room temperature, and transform into skyrmions on changing magnetic field and lamella thickness. The periodicity of magnetic textures greatly depends on the crystal thickness, and domains with anisotropic sawtooth fractals were observed at the surface of thick crystals and attributed to the interplay between the dipolar interaction and the Dzyaloshinskii-Moriya interaction as governed by crystal symmetry. Our findings provide an arena in which to study antiskyrmions, and should stimulate further research on topological spin textures and their applications.
机译:拓扑旋转纹理吸引了很多关注的基本物理和闪闪发光的应用。其中,由于非中心对称晶体结构的各向异性Dzyaloshinskii-Moriya相互作用,Antikermions拥有独特的旋转配置,并具有布隆型和尼尔型畴壁。然而,迄今为止,在少量Heusler化合物中仅观察到具有D_(2D)对称性的抗励草。在这里,我们报告了一个新的材料,FE_(1.9)NI_(0.9)PD_(0.2)PD_(0.2)P,在不同的对称类(S_4)中,其中ANTISKYRMIONS存在于包括室温的宽温度范围内,并转换为改变时的斯基变磁场和薄片厚度。磁性纹理的周期性大量取决于晶体厚度,并且在厚晶体表面观察到具有各向异性锯齿分切片的结构域,并且归因于晶体相互作用与Dzyaloshinskii-moriya相互作用,如晶体对称所控制的。我们的调查结果提供了一个学习Antiskyrions的竞技场,并应刺激拓扑旋转纹理及其应用的进一步研究。

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  • 来源
    《Nature Materials》 |2021年第3期|335-340|共6页
  • 作者单位

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan Department of Applied Physics University of Tokyo Bunkyo-ku Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan Department of Applied Physics University of Tokyo Bunkyo-ku Japan Tokyo College University of Tokyo Bunkyo-ku Japan;

    RIKEN Center for Emergent Matter Science (CEMS) Wako Japan;

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