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能带弯曲和单轴应变诱导的反铁磁锡烯纳米带中的高光自旋过滤

High optical spin-filtering in antiferromagnetic stanene nanoribbons induced by band bending and uniaxial strain.

作者信息

Rahimi F, Phirouznia A

机构信息

Department of Physics, Azarbaijan Shahid Madani University, Tabriz, 53714-161, Iran.

Condensed Matter Computational Research Lab, Azarbaijan Shahid Madani University, Tabriz, 53714-161, Iran.

出版信息

Sci Rep. 2023 Aug 8;13(1):12874. doi: 10.1038/s41598-023-39593-6.

DOI:10.1038/s41598-023-39593-6
PMID:37553395
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10409786/
Abstract

Non-equilibrium spin-polarized transport properties of antiferromagnetic stanene nanoribbons are theoretically studied under the combining effect of a normal electric field and linearly polarized irradiation based on the tight-binding model at room temperature. Due to the existence of spin-orbit coupling in stanene lattice, applying normal electric field leads to splitting of band degeneracy of spin-resolved energy levels in conduction and valence bands. Furthermore, unequivalent absorption of the polarized photons at two valleys which is attributed to an antiferromagnetic exchange field results in unequal spin-polarized photocurrent for spin-up and spin-down components. Interestingly, in the presence of band bending which has been induced by edge potentials, an allowable quantum efficiency occurs over a wider wavelength region of the incident light. It is especially important that the variation of an exchange magnetic field generates spin semi-conducting behavior in the bended band structure. Moreover, it is shown that optical spin-filtering effect is obtained under the simultaneous effect of uniaxial strain and narrow edge potential.

摘要

基于紧束缚模型,在室温下,研究了在正常电场和线偏振光辐照的联合作用下,反铁磁锡烯纳米带的非平衡自旋极化输运特性。由于锡烯晶格中存在自旋轨道耦合,施加正常电场会导致导带和价带中自旋分辨能级的能带简并分裂。此外,由于反铁磁交换场导致的两个谷对偏振光子的不等效吸收,使得自旋向上和自旋向下分量的自旋极化光电流不相等。有趣的是,在由边缘势引起的能带弯曲存在的情况下,在更宽的入射光波长区域会出现允许的量子效率。特别重要的是,交换磁场的变化会在弯曲的能带结构中产生自旋半导体行为。此外,结果表明,在单轴应变和窄边缘势的同时作用下可获得光学自旋滤波效应。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/794669aa3514/41598_2023_39593_Fig10_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/c790da91453b/41598_2023_39593_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/67404db0f65b/41598_2023_39593_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/794669aa3514/41598_2023_39593_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/bf6abe4ed48a/41598_2023_39593_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/abe3706ff9b9/41598_2023_39593_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/1778d838dfe4/41598_2023_39593_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/d299c1ca757e/41598_2023_39593_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/3540c967bdf4/41598_2023_39593_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/09628101695a/41598_2023_39593_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/86818b6b435b/41598_2023_39593_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/c790da91453b/41598_2023_39593_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/67404db0f65b/41598_2023_39593_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1cf4/10409786/794669aa3514/41598_2023_39593_Fig10_HTML.jpg

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