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Unravelling Incommensurate Magnetism and Its Emergence in Iron-Based Superconductors

机译:解开不加许的磁力及其在铁基超导体中的出现

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We focus on a broad class of tetragonal itinerant systems sharing a tendency towards the spontaneous formation of incommensurate magnetism with ordering wave vectors Q 1 , 2 = ( π ? δ , 0 ) / ( 0 , π ? δ ) or Q 1 , 2 = ( π , δ ) / ( ? δ , π ) . Employing a Landau approach, we obtain the generic magnetic phase diagram and identify the leading instabilities near the paramagnetic-magnetic transition. Nine distinct magnetic phases exist that either preserve or violate the assumed C 4 symmetry of the paramagnetic phase. These are single- and double- Q phases consisting of magnetic stripes, helices, and whirls, either in an individual or coexisting manner. These nine phases can be experimentally distinguished by polarized neutron scattering, or, e.g., by combining measurements of the induced charge order and magnetoelectric coupling. Within two representative five-orbital models, suitable for BaFe 2 As 2 and LaFeAsO, we find that the incommensurate magnetic phases we discuss here are accessible in iron-based superconductors. Our investigation unveils a set of potential candidates for the unidentified C 2 -symmetric magnetic phase that was recently observed in Ba 1 ? x Na x Fe 2 As 2 . Among the phases stabilized we find a spin-whirl crystal, which is a textured magnetic C 4 -symmetric phase. The possible experimental observation of textured magnetic orders in iron-based superconductors opens new directions for realizing intrinsic topological superconductors.
机译:我们专注于广泛的四方巡回系统,与订购波矢量Q 1,2 =(παδ,0)/(0,π≤δ)或Q 1,2 = (π,δ)/(Δ,π)。采用Landau方法,我们获得了通用磁相图,并确定了近磁磁转换附近的领先不稳定性。存在九个不同的磁相,保持或违反副孔阶段的假定的C 4对称性。这些是由磁条,螺旋和旋转组成的单一和双Q阶段,无论是个人还是共存的方式。可以通过偏振中子散射实验地区分这些九个相,或者例如,通过组合诱导的电荷级和磁电联接器的测量来实现。在两个代表性的五轨道模型中,适用于Bafe 2和Lafeaso,我们发现我们在此讨论的不计磁阶段可用于基于铁基超导体。我们的调查推出了一组潜在的候选人,用于最近在BA 1中观察到的未识别的C 2 - 对称磁阶段? x na x fe 2为2。在阶段中,稳定我们发现旋转旋转晶体,其是纹理磁性C 4-对称相。在铁基超导体中纹理磁性订单的可能实验观察开辟了实现内在拓扑超导体的新方向。

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