Spatial Selected Spin Filtering Effect in Z-Shaped MoS<sub>2</sub> Nanoribbon

Due to the gapless between any two successive subbands with the same spin, the spin polarization in uniform MoS<sub>2</sub> zigzag nanoribbon (MoS<sub>2</sub>-ZR) is weak. Here, through configuring Z-shaped structure, we realize 100&#x0025; spin polarization in MoS<sub...

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Bibliographic Details
Main Authors: Yi-Hao Ma, Liang-Hao Ruan, Jing Wang, Wen-Sheng Zhao, Yue Hu, Yuhua Cheng, Da-Wei Wang, Gaofeng Wang
Format: Article
Language:English
Published: IEEE 2021-01-01
Series:IEEE Access
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Online Access:https://ieeexplore.ieee.org/document/9497047/
Description
Summary:Due to the gapless between any two successive subbands with the same spin, the spin polarization in uniform MoS<sub>2</sub> zigzag nanoribbon (MoS<sub>2</sub>-ZR) is weak. Here, through configuring Z-shaped structure, we realize 100&#x0025; spin polarization in MoS<sub>2</sub>-ZR with only exchange field. The filtered spin electrons transmit along a specified edge of the device. This phenomenon is the result of the combined effect of the localized edge states and structure induced inversion of the Mo-edge and S-edge. In our calculation the fully spin polarization appears in several energy regions, so this Z-shaped MoS<sub>2</sub>-ZRs can be used in making spintronic devices.
ISSN:2169-3536