论文标题

在中心对称晶格系统中,无垂直镜子对称的方形晶体的螺旋锁定

Helicity locking of square skyrmion crystal in a centrosymmetric lattice system without vertical mirror symmetry

论文作者

Hayami, Satoru, Yambe, Ryota

论文摘要

从理论上讲,我们研究了方形晶体晶体(SKX)在中心对称四方晶格结构中的稳定性,重点是由于缺乏垂直镜子对称性而引起的磁各向异性的作用。我们的分析基于动量空间中有效的双线性和生物二级模型,这是弱耦合方案中巡回磁铁的规范模型。通过在二维方形晶格上对模型进行模拟退火,我们发现相互作用中的非对角线旋转组件在破碎垂直镜对称性时变为非零,从而在外部磁场中具有明确的螺旋性引起正方形SKX。我们表明,中心对称SKX的螺旋度取决于异对角线和对角线各向异性相互作用之间的竞争,后者出现在离散的四重旋转晶格结构中。此外,我们通过引入奇数多物来讨论螺旋依赖性的物理现象,其中电(磁性)和电(磁性)环形多物是反对称自旋极化和Edelstein效应(磁电效应)的来源。我们还讨论了在磁场旋转中具有不同螺旋性的SKXS的稳定性。我们的结果提供了一种通过中心对称磁体中的对称各向异性相互作用来设计螺旋性锁定的SKX的方法,这与非中性磁体中的反对称dzyaloshinskii-Moriya相互作用不同。

We theoretically investigate the stability of a square skyrmion crystal (SkX) in a centrosymmetric tetragonal lattice structure with the emphasis on the role of the magnetic anisotropy arising from the absence of vertical mirror symmetry. Our analysis is based on an effective bilinear and biquadratic model in momentum space, which is a canonical model for itinerant magnets in a weak-coupling regime. By performing the simulated annealing for the model on the two-dimensional square lattice, we find that the off-diagonal spin component in the interaction, which becomes nonzero when the vertical mirror symmetry is broken, gives rise to the square SkX with a definite helicity in an external magnetic field. We show that the helicity of the centrosymmetric SkXs is determined by the competition between the off-diagonal and diagonal anisotropic interactions, the latter of which appears in the discrete fourfold-rotational lattice structure. Furthermore, we discuss helicity-dependent physical phenomena by introducing odd-parity multipoles, where electric (magnetic) and electric (magnetic) toroidal multipoles are sources of an antisymmetric spin polarization and an Edelstein effect (a magnetoelectric effect). We also discuss the stability of the SkXs with different helicities in a magnetic field rotation. Our results provide a way of engineering the helicity-locked SkXs by the symmetric anisotropic interaction in centrosymmetric magnets, which is distinct from that by the antisymmetric Dzyaloshinskii-Moriya interaction in noncentrosymmetric magnets.

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