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Quasi 2D electronic states with high spin-polarization in centrosymmetric MoS2 bulk crystals

机译:中心对称MoS2块状晶体中具有高自旋极化的准二维电子态

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摘要

Time reversal dictates that nonmagnetic, centrosymmetric crystals cannot be spin-polarized as a whole. However, it has been recently shown that the electronic structure in these crystals can in fact show regions of high spin-polarization, as long as it is probed locally in real and in reciprocal space. In this article we present the first observation of this type of compensated polarization in MoS2 bulk crystals. Using spin- and angle-resolved photoemission spectroscopy (ARPES), we directly observed a spin-polarization of more than 65% for distinct valleys in the electronic band structure. By additionally evaluating the probing depth of our method, we find that these valence band states at the point in the Brillouin zone are close to fully polarized for the individual atomic trilayers of MoS2, which is confirmed by our density functional theory calculations. Furthermore, we show that this spin-layer locking leads to the observation of highly spin-polarized bands in ARPES since these states are almost completely confined within two dimensions. Our findings prove that these highly desired properties of MoS2 can be accessed without thinning it down to the monolayer limit.
机译:时间反转表明,非磁性,中心对称晶体不能整体上自旋极化。但是,最近显示,这些晶体中的电子结构实际上可以显示高自旋极化的区域,只要它在实空间和倒数空间中被局部探测即可。在本文中,我们提出了在MoS2块状晶体中这种类型的补偿极化的第一个观察结果。使用自旋和角度分辨光发射光谱(ARPES),我们直接观察到电子能带结构中不同波谷的自旋极化率超过65%。通过进一步评估我们方法的探测深度,我们发现在布里渊区中的这些价带态对于MoS2的单个原子三层接近于完全极化,这由我们的密度泛函理论计算所证实。此外,我们表明,这种自旋层锁定导致观察到ARPES中的高度自旋极化带,因为这些状态几乎完全限制在二维范围内。我们的发现证明,在不将MoS2减薄到单层限制的情况下,可以访问这些高度期望的MoS2属性。

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