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Crystallographic anisotropy and distortions in helicoidal magnetic structure

机译:螺旋磁结构的晶体学各向异性和畸变

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摘要

The appearance and development of aperiodic distortions in a helicoidal, layered magnetic structure with increasing crystallographic magnetic anisotropy in the magnetization rotation plane have been theoretically studied. A simple phase diagram for this system is proposed. It is established that, at a weak anisotropy, the spiral splits into regions of various lengths with an approximately uniform rotation of the magnetization in each region and a deviation from uniformity at the boundaries; the stronger the anisotropy, the shorter the regions and the greater the deviations. In the limit of high anisotropy, the minimum energy of the system corresponds (depending on the ratio of interlayer exchange integrals J _1 and J _2) to either a spiral with constant angular pitch (a multiple of the angle between easy axes) or a double antiferromagnetic structure with a four-layer period. In the case of sixth-order anisotropy with |J _1| = -J _2, the energies of phases with different periods (four and six layers for J _1 > 0; four and three layers for J _1 < 0) coincide and the excess boundary energy vanishes. In the case of a fourth- and second-order anisotropy, the analogous anomalies appear at |J _1| = -2J _2. As a result, the magnetic structure at these points becomes unstable and the phase diagram exhibits the corresponding singularities.
机译:理论上研究了在磁化旋转平面中随着晶体学磁各向异性的增加而出现的螺旋状分层磁性结构中非周期性畸变的出现和发展。提出了该系统的简单相位图。可以确定的是,在各向异性较弱的情况下,螺旋线分裂成各种长度的区域,每个区域的磁化强度近似均匀地旋转,并且在边界处偏离均匀性。各向异性越强,区域越短,偏差越大。在高各向异性的极限下,系统的最小能量(取决于层间交换积分J _1和J _2的比率)对应于具有恒定角度间距(易轴之间的角度的倍数)的螺旋具有四层周期的反铁磁结构。对于具有| J _1 |的六阶各向异性= -J _2时,具有不同周期的相的能量(对于J _1> 0为四层和六层;对于J _1 <0为四层和三层)重合,并且多余的边界能量消失了。在四阶和二阶各向异性的情况下,类似的异常出现在| J _1 |处。 = -2J _2。结果,这些点的磁性结构变得不稳定,并且相图呈现出相应的奇点。

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