金属铁磁铁磁铁的超低磁性阻尼
Martin A W Schoen1,2, Danny Thonig3, Michael L Schneider1
1Quantum Electromagnetics Division, National Institute of Standards and Technology, Boulder, Colorado 80305, USA.
Nature physics
|October 30, 2024
概括
研究人员发现了一种具有超低磁阻尼的铁合金,这对于自旋电子设备至关重要. 这一突破挑战了以前的理论,为高速,低能耗电子应用提供了新的可能性.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 这就是Spintronics.
背景情况:
- 磁性缓冲对于旋转电子和旋转轨道电子设备至关重要.
- 预测铁磁材料的阻尼仍然是一个理论上的挑战.
- 金属中的超低减通常受到电子-马格农散射的限制.
研究的目的:
- 研究一种用于超低磁阻尼的新型二元合金.
- 了解负责降低阻尼的潜在物理机制.
- 为了测试现有的磁阻尼理论预测.
主要方法:
- 铁二元合金的制造和表征.
- 测量磁阻尼参数的测量.
- 分析材料的电子带结构,特别是状态密度.
主要成果:
- 实现了接近10−4的磁性阻尼参数,与铁磁绝缘体可比.
- 在最佳合金度下,在费米水平的状态密度中确定了尖的最小值.
- 证明了这种带结构特征可以克服电子-马格农散射的限制.
结论:
- 铁合金表现出前所未有的低磁阻尼.
- 观察到的现象归因于一个独特的带结构特征.
- 这一发现为缓冲机制提供了基本的见解,并验证了理论模型.
相关概念视频
Magnetic Damping
431
Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
431
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
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 Susceptibility and Permeability
983
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...
983
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
Magnetostatic Boundary Conditions
879
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...
879


