基于谷电子性能的锡掺杂硫系镉单层材料的设计

Sutapa Chattopadhyay, Anjali Kshirsagar
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摘要

谷电子学是二维系统中一个有趣的研究领域,它使用谷指数或谷伪自旋来编码信息。自旋轨道耦合(SOC)和反转对称破缺导致了谷附近能带的自旋分裂。这一性质具有很好的器件应用前景。 为了找到一种新的用于谷电子的二维材料,我们从块状CdX锌闪锌矿结构的(111)表面设计了六方平面单层镉硫族化合物(CdX, X = S, Se, Te)。确定了这些结构的结构稳定性、动力稳定性、力学稳定性和热稳定性。带结构研究揭示了价带在K和K′对称点处的局部最大值(谷)。SOC的应用引发了谷中的自旋分裂,提高了能量简并性,表现出较强的谷-自旋耦合特性。为了引发更强的SOC,我们用Sn原子取代了几乎是平面的单层中的两个Cd原子,这大大增加了自旋分裂。掺杂锡的CdSe和CdTe单层在谷区观察到zeeman型自旋分裂,在Γ点观察到Rashba自旋分裂。所有掺杂锡的单分子膜的Berry曲率值都大于未掺杂锡的单分子膜。因此,这些新设计的单分子层被发现适用于谷电子应用。掺杂锡的单层膜在锡s、p态和p态之间的价带和导带深处显示出能带反转,但缺乏拓扑性质。
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Design of Sn-doped cadmium chalcogenide based monolayers for valleytronics properties
Abstract Valleytronics has emerged as an interesting field of research in two-dimensional (2D) systems and uses the valley index or valley pseudospin to encode information. Spin-orbit coupling (SOC) and inversion symmetry breaking leads to spin-splitting of bands near the valleys. This property has promising device applications.
In order to find a new 2D material useful for valleytronics, we have designed hexagonal planar monolayers of cadmium chalcogenides (CdX, X = S, Se, Te) from the (111) surface of bulk CdX zinc blende structure. The structural, dynamic, mechanical and thermal stability of these structures is confirmed. Band structure study reveals valence band local maxima (valleys) at K and K′ symmetry points. Application of SOC initiates spin-splitting in the valleys that lifts the energy degeneracy and shows strong valley-spin coupling character. To initiate stronger SOC, we have substituted two Cd atoms in the almost planar monolayers by Sn atoms which increases the spin-splitting significantly. Zeeman-type spin-splitting is observed in the valley region and Rashba spin-splitting is observed at the Γ point for Sn-doped CdSe and CdTe monolayers. Berry curvature values are more in all the Sn-doped monolayers than the pristine monolayers. These newly designed monolayers are thus found to be suitable for valleytronics applications. Sn-doped monolayers show band inversion deep in the valence and conduction bands between Sn s and p and X p states but lack topological properties.

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