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基于CrI₃的范德华异质结构的衬底诱导电子相变

Substrate induced electronic phase transitions of CrI[Formula: see text] based van der Waals heterostructures.

作者信息

Chakraborty Shamik, Ravikumar Abhilash

机构信息

Nanoelectronics Research Laboratory, Department of Electronics and Communication Engineering, Amrita School of Engineering, Amrita Vishwa Vidyapeetham, Bengaluru, 560035 India.

出版信息

Sci Rep. 2021 Jan 8;11(1):198. doi: 10.1038/s41598-020-80290-5.

Abstract

We perform first principle density functional theory calculations to predict the substrate induced electronic phase transitions of CrI[Formula: see text] based 2-D heterostructures. We adsorb graphene and MoS[Formula: see text] on novel 2-D ferromagnetic semiconductor-CrI[Formula: see text] and investigate the electronic and magnetic properties of these heterostructures with and without spin orbit coupling (SOC). We find that when strained MoS[Formula: see text] is adsorbed on CrI[Formula: see text], the spin dependent band gap which is a characteristic of CrI[Formula: see text], ceases to remain. The bandgap of the heterostructure reduces drastically ([Formula: see text] 70%) and the heterostructure shows an indirect, spin-independent bandgap of [Formula: see text] 0.5 eV. The heterostructure remains magnetic (with and without SOC) with the magnetic moment localized primarily on CrI[Formula: see text]. Adsorption of graphene on CrI[Formula: see text] induces an electronic phase transition of the subsequent heterostructure to a ferromagnetic metal in both the spin configurations with magnetic moment localized on CrI[Formula: see text]. The SOC induced interaction opens a bandgap of [Formula: see text] 30 meV in the Dirac cone of graphene, which allows us to visualize Chern insulating states without reducing van der Waals gap.

摘要

我们进行第一性原理密度泛函理论计算,以预测基于CrI₃的二维异质结构的衬底诱导电子相变。我们将石墨烯和MoS₂吸附在新型二维铁磁半导体CrI₃上,并研究这些有自旋轨道耦合(SOC)和没有自旋轨道耦合的异质结构的电子和磁性特性。我们发现,当应变的MoS₂吸附在CrI₃上时,作为CrI₃特征的自旋相关带隙不再存在。异质结构的带隙急剧减小(约70%),并且异质结构显示出约0.5 eV的间接、自旋无关带隙。该异质结构在有和没有SOC的情况下都保持磁性,磁矩主要定域在CrI₃上。在两种自旋构型中,石墨烯吸附在CrI₃上都会使随后的异质结构发生电子相变,成为铁磁金属,磁矩定域在CrI₃上。SOC诱导的相互作用在石墨烯的狄拉克锥中打开了约30 meV的带隙,这使我们能够在不减小范德华间隙的情况下可视化陈绝缘态。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b7f3/7794430/efd1e15277f5/41598_2020_80290_Fig1_HTML.jpg

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