接近有序温度的非中心对称磁体的非海森堡模型中的手性调制

Magnetism Pub Date : 2024-04-01 DOI:10.3390/magnetism4020007
Andrey O. Leonov
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引用次数: 0

摘要

在接近有序温度的手性磁体现象学 Dzyaloshinskii 模型中研究的天融石和螺旋溶液的结构特点是纵向有序参数和角有序参数之间的强烈相互作用,这可能是实验观察到的前驱体效应的原因。在前驱体区域内,压力、电场、化学掺杂、单轴应变和/或磁晶各向异性等附加效应会改变能量分布,甚至可能导致半空晶的方形交错晶格等奇异相位的稳定,这种晶格的内部结构采用了 "软 "模量的概念,包含模量值为零的点。在这里,我们还改变了磁化模量的刚度,以有利于具有大调制量级参数的一维和二维调制态。计算得出的相图(省略了任何附加效应)显示了方形半天元晶格、六边形天元晶格(磁化在与外加磁场平行的晶格中心)和螺旋体(传播方向横向于磁场)的稳定口袋,也就是说,在这些相中,局部缺陷的概念被平滑但更复杂的空间平铺图所取代。我们注意到,这些结果可适用于金属玻璃和手性液晶,在金属玻璃中,能量贡献是相同的,并且源于模型中固有的挫折感,而手性液晶则具有不同的弹性常数比率。
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Chiral Modulations in Non-Heisenberg Models of Non-Centrosymmetric Magnets Near the Ordering Temperatures
The structure of skyrmion and spiral solutions, investigated within the phenomenological Dzyaloshinskii model of chiral magnets near the ordering temperatures, is characterized by the strong interplay between longitudinal and angular order parameters, which may be responsible for experimentally observed precursor effects. Within the precursor regions, additional effects, such as pressure, electric fields, chemical doping, uniaxial strains and/or magnetocrystalline anisotropies, modify the energetic landscape and may even lead to the stability of such exotic phases as a square staggered lattice of half-skyrmions, the internal structure of which employs the concept of the “soft” modulus and contains points with zero modulus value. Here, we additionally alter the stiffness of the magnetization modulus to favor one- and two-dimensional modulated states with large modulations of the order parameter magnitude. The computed phase diagram, which omits any additional effects, exhibits stability pockets with a square half-skyrmion lattice, a hexagonal skyrmion lattice with the magnetization in the center of the cells parallel to the applied magnetic field, and helicoids with propagation transverse to the field, i.e., those phases in which the notion of localized defects is replaced by the picture of a smooth but more complex tiling of space. We note that the results can be adapted to metallic glasses, in which the energy contributions are the same and originate from the inherent frustration in the models, and chiral liquid crystals with a different ratio of elastic constants.
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