面接磁旋霍尔效应在范德瓦尔斯Fe3GeTe2/MoTe2异构结构中的作用
Yudi Dai1, Junlin Xiong1, Yanfeng Ge2
1National Laboratory of Solid State Microstructures, Institute of Brain-Inspired Intelligence, School of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China.
Nature communications
|February 6, 2024
概括
研究人员在Fe3GeTe2/MoTe2异构结构中发现了一个巨大的时间逆转奇偶旋转霍尔效应 (T-奇偶SHE). 这种接口磁自旋霍尔效应 (接口-MSHE) 能够为自旋电子和内存计算提供新的功能.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 纳米技术纳米技术
背景情况:
- 旋转霍尔效应 (SHE) 对旋转电子非常重要,它将电荷电流转换为旋转电流.
- 在非磁性材料中,反转时间均的SHE是常见的.
- 时间反转奇偶 (T-odd) SHE,加上磁化,提供了新的电荷-自旋转换.
研究的目的:
- 报道了在范德瓦尔斯异构结构中观察到一个巨大的T-odd SHE.
- 为了识别和描述一个新的界面磁自旋霍尔效应 (界面-MSHE).
- 探索这种效应在计算中的潜在应用.
主要方法:
- 德瓦尔斯 Fe3GeTe2/MoTe2 异构结构的制造.
- 对T-odd SHE的实验观测.
- 对称性分析和理论计算.
- 用于演示计算操作的设备制造.
主要成果:
- 在Fe3GeTe2/MoTe2中观察到一个巨大的T-odd SHE,称为界面-MSHE.
- 将这种效应归因于在接口上引发的突破对称性的旋转电流双极.
- 在实施多重积累运算和卷积神经网络中证明效果的实用性.
结论:
- 发现了一个新的T-odd接口电荷-自旋转换机制.
- 接口-MSHE为旋转电子提供了新的功能.
- 开发节能内存计算设备的潜力.
相关概念视频
The Hall Effect
2.4K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
2.4K
Valence Bond Theory
8.6K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
8.6K
Ferromagnetism
2.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.4K
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Magnetostatic Boundary Conditions
934
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
934
MOSFET: Enhancement Mode
336
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
336


