铁磁节点线半导体中的巨大角磁阻
Junho Seo1,2, Chandan De1,3, Hyunsoo Ha4
1Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science (IBS), Pohang, Korea.
Nature
|November 25, 2021
概括
研究人员在磁结线半导体中发现了巨大的角磁阻力. 通过对电子导电与磁场进行调整, 使得极其灵敏的自旋电子器件成为可能.
科学领域:
- 凝聚物质物理学
- 材料科学
- 机器人
背景情况:
- 电子传导的高效磁性控制对于记忆和逻辑等旋转应用至关重要.
- 磁铁中的拓带交叉为通过旋转配置调节电子传导提供了一个可调节的平台.
研究的目的:
- 调查磁性半导体在大型磁传输反应中的拓结线退化潜力.
- 在模型系统中展示巨大的角磁阻力,并探索其对自旋电子学的影响.
主要方法:
- 磁节线半导体中的巨大角磁阻的理论建议.
- 使用分层铁磁体Mn3Si2Te6及其衍生化合物的实验研究作为模型系统.
- 分析旋转方向的拓带退化及其对磁传输的影响.
主要成果:
- 证明磁性半导体的拓结线退化会导致磁传输的极大角响应.
- 在相同的铁磁阶段内观察到金属绝缘器过渡,这是由于带退化升级.
- 在模型系统中量化了巨大的角磁阻,
结论:
- 磁结线半导体是实现前所未有的自旋和轨道依赖功能的有希望的平台.
- 巨大的角磁阻效应为先进的旋转器件设计和应用开辟了新的途径.
相关概念视频
Ferromagnetism
2.5K
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...
2.5K
Diamagnetism
2.5K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.5K
Paramagnetism
2.6K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
2.6K
Magnetic Moment of an Electron
1.9K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
1.9K
Magnetic Susceptibility and Permeability
1.5K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.5K
Magnetic Field Of A Current Loop
5.1K
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
5.1K


