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Existence of Dirac cones in the Brillouin zone of diperiodic atomic crystals according to group theory

机译:基于群论的二重原子晶体布里渊区中狄拉克锥的存在

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We have considered non-magnetic materials with weak spin-orbit coupling, that are periodic in two non-collinear directions, and finite in the third, orthogonal direction. In some cases, the combined time-reversal and crystal symmetry of such systems, allows the existence of Dirac cones at certain points in the reciprocal space. We have investigated in a systematic way, all points of the Brillouin zone of all 80 diperiodic groups and have found sufficient conditions for the existence of s = 1/2 Dirac fermions, with symmetry-provided band touching at the vertex of the Dirac cones. Conversely, complete linear dispersion is forbidden for orbital wave functions belonging to two-dimensional (2D) irreducible representations (irreps) of little groups that do not satisfy certain group theoretical conditions given in this paper. Our results are illustrated by a tight-binding example.
机译:我们考虑了具有弱自旋轨道耦合的非磁性材料,它们在两个非共线方向上是周期性的,而在第三个正交方向上是有限的。在某些情况下,此类系统的时间反转和晶体对称性相结合,使得在倒易空间中的某些点处存在狄拉克锥。我们以系统的方式研究了所有80个二元组的布里渊区的所有点,并找到了存在s = 1/2 Dirac费米子的充分条件,并且在Dirac锥的顶点处有对称提供的谱带。相反,对于不满足本文给出的某些组理论条件的小组的二维(2D)不可约表示(irreps),轨道波函数被禁止完全线性弥散。一个紧密绑定的例子说明了我们的结果。

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