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Multi- Q hexagonal spin density waves and dynamically generated spin-orbit coupling: Time-reversal invariant analog of the chiral spin density wave

机译:多Q六角形自旋密度波和动态生成的自旋-轨道耦合:手性自旋密度波的时间反转不变模拟

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We study hexagonal spin-channel ("triplet") density waves with commensurate M-point propagation vectors. We first show that the three Q = M components of the singlet charge density and charge-current density waves can be mapped to multicomponent Q = 0 nonzero angular momentum order in three dimensions (3D) with cubic crystal symmetry. This one-to-one correspondence is exploited to define a symmetry classification for triplet M-point density waves using the standard classification of spin-orbit coupled electronic liquid crystal phases of a cubic crystal. Through this classification we naturally identify a set of noncoplanar spin density and spin-current density waves: the chiral spin density wave and its time-reversal invariant analog. These can be thought of as 3D L = 2 and 4 spin-orbit coupled isotropic β-phase orders. In contrast, uniaxial spin density waves are shown to correspond to α phases. The noncoplanar triple-M spin-current density wave realizes a novel 2D semimetal state with three flavors of four-component spin-momentum locked Dirac cones, protected by a crystal symmetry akin to nonsymmorphic symmetry, and sits at the boundary between a trivial and topological insulator. In addition, we point out that a special class of classical spin states, defined as classical spin states respecting all lattice symmetries up to global spin rotation, are naturally obtained from the symmetry classification of electronic triplet density waves. These symmetric classical spin states are the classical long-range ordered limits of chiral spin liquids.
机译:我们研究了具有相应M点传播矢量的六角形自旋通道(“三胞胎”)密度波。我们首先显示,单线态电荷密度和电荷电流密度波的三个Q = M分量可以立方晶体对称的三个维度(3D)映射到多分量Q = 0非零角动量阶。利用这种一对一的对应关系,使用立方晶体的自旋轨道耦合电子液晶相的标准分类来定义三重态M点密度波的对称分类。通过这种分类,我们自然地可以识别出一组非共面的自旋密度波和自旋电流密度波:手性自旋密度波及其随时间变化的不变类比。这些可以认为是3D L = 2和4个自旋轨道耦合的各向同性β相序。相反,示出了单轴自旋密度波对应于α相。非共面三重M自旋电流密度波实现了新型的二维半金属态,具有三种口味的四组分自旋动量锁紧的Dirac锥,受到类似于非对称对称的晶体对称性的保护,并位于平凡和拓扑之间的边界绝缘子。此外,我们指出一类特殊的经典自旋态,定义为尊重所有晶格对称性直至整体自旋旋转的经典自旋态,自然是从电子三重态密度波的对称性分类中获得的。这些对称的经典自旋态是手性自旋液体的经典远程有序极限。

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