在反铁磁的迪拉克半金属的多波向量电荷密度波形状态中的巨大磁阻
Ratnadwip Singha1, Kirstine J Dalgaard1, Dmitry Marchenko2
1Department of Chemistry, Princeton University, Princeton, NJ 08544, USA.
Science advances
|October 13, 2023
概括
研究人员在迪拉克半金属CeSbTe中发现了巨大的负磁阻,这种现象通常在矿中见到. 在被电子杂材料中的这一发现为了解和利用这种效应在先进的电子设备中开辟了新的途径.
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
- 量子材料是一种量子材料.
背景情况:
- 巨大的负磁阻 (CNMR) 是铁磁矿中观察到的显著现象,推动了技术应用的研究.
- 拓性半金属通常由于具有高流动性的电荷载体而表现出很大的正磁阻.
- 了解不同材料类中CNMR的新型机制对于推进自旋电子和磁传感技术至关重要.
研究的目的:
- 为了研究电子合的迪拉克半金属CeSbTe.Te的磁阻特性.
- 探索电荷密度波,磁性排序和CeSbTe中的电子传输之间的关系.
- 确定CeSbTe是否表现出巨大的负磁电阻,并了解潜在的物理机制.
主要方法:
- 电子合的迪拉克半金属CeSb0.11Te1.90的合成和表征.
- 测量电子传输特性,包括在不同磁场下的电阻.
- 分析磁相图和电荷密度波 (CDW) 调制向量.
- 对异常的霍尔效应进行调查,以探测探针旋转调制.
主要成果:
- CeSb0.11Te1.90被证实是一种具有多个CDW调制向量的反铁磁迪拉克半金属.
- 尽管具有金属费米表面,但该材料表现出半导体类型的电子传输特性.
- 观察到一个巨大的负磁电阻,由磁场驱动的过渡诱导,从半导体类的金属类行为.
- 检测到CDW和旋转调制之间的合信号,导致巨大的异常霍尔反应.
结论:
- 电子合的迪拉克半金属CeSbTe通过独特的磁场诱导过渡表现出巨大的负磁电阻,类似于铁磁矿.
- 在CeSbTe中,电荷密度波和旋转调制之间的相互作用是导致观察到的磁阻和巨大的异常霍尔效应的原因.
- 这一发现扩大了展示CNMR的材料类别,并突出了拓半金属在自旋电子应用中的潜力.
更多相关视频
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.1K
05:39Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
9.7K
相关概念视频
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
Magnetic Field due to Moving Charges
8.8K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
8.8K
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
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
Potential Due to a Magnetized Object
297
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
297
Magnetic Susceptibility and Permeability
1.1K
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...
1.1K
