巨型道磁电阻基于自旋谷不匹配的铁磁金属
Kun Yan1, Li Cheng2, Yizhi Hu1
1Harbin Institute of Technology, School of Science, State Key Laboratory on Tunable Laser Technology and Ministry of Industry and Information Technology Key Lab of Micro-Nano Optoelectronic Information System, Shenzhen, Shenzhen 518055, China.
Physical review letters
|February 10, 2025
概括
具有自旋谷不匹配状态的材料像半金属一样起作用,使巨型磁阻成为可能. 这一发现扩大了高磁阻装置的可能性,超出了有限的半金属选项.
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
- 这就是Spintronics.
背景情况:
- 由于完美的旋转过,半金属对于高磁阻装置至关重要.
- 已知半金属的稀缺性限制了先进的自旋电子装置的开发.
- 旋转谷不匹配 (SVM) 状态为旋转过提供了一个潜在的替代机制.
研究的目的:
- 为了证明具有内在自旋谷不匹配状态的材料可以模仿半金属.
- 探索SVM材料的潜力,以实现巨型道磁阻.
- 为了确定适合高性能自旋电子应用的特定SVM材料.
主要方法:
- 使用第一原则运输计算.
- 研究铁磁过渡金属二甲基化物 (TMD) 的电子和自旋特性.
- 模拟使用SVM材料的范德瓦尔斯 (vdW) 连接的性能.
主要成果:
- 铁磁1T-VSe2,1T-VS2和2H-VS2表现出内在的自旋谷不匹配状态.
- 这些SVM材料有效地阻断了充电传输,类似于半金属.
- 在使用这些电极的VDW旋接口中,预计超出99%的巨型磁阻.
- 由于内在的自旋状态不匹配,VDW连接处的中心非磁性层可能是任意的.
结论:
- 内在的旋转谷不匹配状态为高磁阻提供了可行的途径.
- 像1T-VSe2,1T-VS2和2H-VS2这样的材料是下一代自旋电子设备的有希望的候选者.
- 这项研究提供了对高磁阻机制的基本见解,并指导了新型设备的设计.
相关概念视频
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
Paramagnetism
2.5K
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...
2.5K
Magnetic Susceptibility and Permeability
934
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...
934
Diamagnetism
2.4K
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....
2.4K
Biasing of Metal-Semiconductor Junctions
201
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
201
Magnetic Field Due To A Thin Straight Wire
4.7K
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
4.7K


