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克服双层CrI中电子和空穴掺杂在磁跃迁方面的不对称性。

Overcoming the asymmetry of the electron and hole doping for magnetic transitions in bilayer CrI.

作者信息

Ghosh Sukanya, Stojić Nataša, Binggeli Nadia

机构信息

Abdus Salam International Centre for Theoretical Physics, Strada Costiera, Trieste, Italy.

出版信息

Nanoscale. 2021 May 27;13(20):9391-9401. doi: 10.1039/d1nr00262g.

Abstract

Electrical control of magnetism has great potential for low-power spintronics applications and the newly discovered two-dimensional van der Waals magnetic materials are promising systems for this type of applications. In fact, it has been recently shown experimentally (Jiang et al., Nat. Nanotechnol., 2018, 13, 549-553) that upon electrostatic doping by electrons bilayer CrI3 undergoes an antiferromagnetic-ferromagnetic (AFM-FM) phase transition, even in the absence of magnetic field. Doping by holes, on the other hand, does not induce the same transition in the experiment, which points to an intrinsic asymmetry in the hole and electron doping that limits the control of the transition by doping. We here show, based on first-principles calculations, that the asymmetry originates in the relativistic nature of the valence-band-edge states of the pristine bilayer, which inhibits the magnetic transition upon hole doping. Based on this finding, we propose an approach to overcome the asymmetry and predict the existence of the AFM-FM transition for both hole and electron doping upon moderate uniaxial compression along the soft direction of the bilayer.

摘要

磁的电控制在低功耗自旋电子学应用中具有巨大潜力,新发现的二维范德华磁性材料是这类应用的有前景的体系。事实上,最近的实验表明(Jiang等人,《自然·纳米技术》,2018年,第13卷,第549 - 553页),即使在没有磁场的情况下,通过电子进行静电掺杂时,双层CrI₃会发生反铁磁 - 铁磁(AFM - FM)相变。另一方面,在实验中通过空穴掺杂不会引发相同的转变,这表明空穴和电子掺杂存在内在不对称性,限制了通过掺杂对转变的控制。我们在此基于第一性原理计算表明,这种不对称性源于原始双层价带边缘态的相对论性质,它抑制了空穴掺杂时的磁转变。基于这一发现,我们提出一种克服不对称性的方法,并预测在沿双层软方向进行适度单轴压缩时,空穴和电子掺杂都会出现AFM - FM转变。

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