调整相对论反铁磁域墙壁的弹性和非弹性碰撞
Rubén M Otxoa1,2, Gen Tatara3, Pierre E Roy4
1Hitachi Cambridge Laboratory, J. J. Thomson Avenue, Cambridge, CB3 OHE, UK. ro274@cam.ac.uk.
Scientific reports
|November 30, 2023
概括
研究人员在反铁磁材料中探索了磁域壁碰撞,发现了弹性和不弹性散射的条件. 这项研究是开发基于新型单子计算技术的关键.
科学领域:
- 这就是Spintronics.
- 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
背景情况:
- 基于Soliton的计算利用在碰撞后保持完整性的粒子进行信息处理.
- 抗铁磁材料中的磁域壁是单子的潜在候选者,但它们的散射特性需要研究.
- 旋转轨道扭矩是操纵磁域壁的关键机制.
研究的目的:
- 为了研究Mn中相对论域壁的散射动力[公式:见文本]Au反铁磁材料的散射动力学.
- 为了确定磁域壁之间的弹性和非弹性碰撞的条件.
- 探索这些动态对抗铁磁螺旋电子和逻辑门开发的潜力.
主要方法:
- 实验演示旋转轨道扭矩诱导的域壁动态.
- 在不同的旋转轨道场强度和持续时间下对域壁散射的分析.
- 阶段图构造用于映射碰撞结果 (弹性与非弹性).
主要成果:
- 在特定条件下,在域壁之间展示了弹性散射,即使是具有相反绕数的域壁,在特定条件下.
- 确定了对弹性碰撞的最小域壁速度值,归因于具有吸引力的潜力.
- 在较低的速度下观察到不弹性散射,导致散射呼吸器的形成.
结论:
- 在 Mn Au 中域壁的散射行为是可控制的,取决于速度和旋转轨道扭矩参数.
- 这些发现为计算应用提供了对磁域墙壁的"孤独"性质的关键见解.
- 这项研究强调了使用反铁磁自旋电子技术实现 NOT 和 XOR 逻辑门的前景.
相关概念视频
Elastic Collisions: Introduction
12.9K
An elastic collision is one that conserves both internal kinetic energy and momentum. Internal kinetic energy is the sum of the kinetic energies of the objects in a system. Truly elastic collisions can only be achieved with subatomic particles, such as electrons striking nuclei. Macroscopic collisions can be very nearly, but not quite, elastic, as some kinetic energy is always converted into other forms of energy such as heat transfer due to friction and sound. An example of a nearly...
12.9K
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
Magnetic Field due to Moving Charges
8.7K
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...
8.7K
Electrostatic Boundary Conditions in Dielectrics
1.2K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
1.2K
Atomic Nuclei: Nuclear Relaxation Processes
657
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
657
Elastic Strain Energy for Shearing Stresses
195
As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
195


