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Complete optical valley polarization in Weyl semimetals in strong magnetic fields

机译:Weyl半金属在强磁场中的完全光谷极化

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We present a theory of an optically induced valley polarization in an interacting, time-reversal-symmetric Weyl semimetal placed under strong magnetic fields. Because the application of a magnetic field reduces the symmetry of the crystal, the optical absorption intensity differs at Weyl nodes that were equivalent by symmetry at zero field. At strong magnetic field, the difference in the absorption intensity reaches 100% for a sizable frequency interval of the incident light. This complete valley polarization originates from interband transitions involving the chiral Landau level, and can be controlled by changing the directions of the magnetic field and the light propagation. We identify the splitting of 0 -> 1 or -1 -> 0 inter-Landau-level transitions as an observable signature of the complete valley polarization, and discuss its manifestation in the TaAs family of materials.
机译:我们提出了一种在强磁场下相互作用的,时间反转对称的魏尔半金属中的光诱导谷极化的理论。由于施加磁场会降低晶体的对称性,因此在Weyl节点处的光吸收强度会有所不同,而Weyl节点的对称性在零场处是等效的。在强磁场下,在相当大的入射光频率间隔内,吸收强度的差异达到100%。这种完全的谷底极化来自涉及手性朗道能级的带间跃迁,可以通过改变磁场方向和光传播方向来控制。我们将0-> 1或-1-> 0的Landau级跃迁的分裂识别为完整谷极化的可观察标志,并讨论了它在TaAs材料家族中的表现。

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