相关实验视频
Updated: Jun 12, 2025

06:53
Scanning SQUID Study of Vortex Manipulation by Local Contact
Published on: February 1, 2017
6.8K
在磁对中可引导电流驱动的自旋波的发射
Sabri Koraltan1,2,3, Katrin Schultheiss4, Florian Bruckner1
1Faculty of Physics, University of Vienna, Kolingasse 14-16, A-1090 Vienna, Austria.
Science advances
|September 25, 2024
概括
研究人员使用电流驱动的欧斯特德场在磁中实现了高效的自旋波生成. 这种方法为先进的磁设备提供了更高的激发效率和可调节的磁传播.
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
- 纳米技术纳米技术
背景情况:
- 有效的自旋波激发对于开发功能性的磁器件至关重要.
- 现有的方法往往缺乏必要的效率或可调性.
研究的目的:
- 展示一种新的方法,用于在反铁磁合的磁中产生电流驱动的自旋波.
- 为了研究激发机制,并探索磁传播的可调性.
主要方法:
- 利用时间分辨率的X射线显微镜直接成像自旋波辐射.
- 采用微磁模拟来确定激发源.
- 研究了磁束性材料,以研究马格农方向盘.
主要成果:
- 在磁中成功演示了电流驱动的自旋波生成.
- 确定了欧斯特德场,而不是旋转转移扭矩,作为主要的激发机制.
- 与条形天线相比,实现了显著更高的旋波激发效率.
- 展示了可调节的马格农传播方向,通过控制磁强化材料中的激发幅度.
结论:
- 展示的方法为旋波激发提供了一种高效和可调的方法.
- 这项工作代表了巨大的进步,在设计和实现magnonic设备.
相关概念视频
Torque On A Current Loop In A Magnetic Field
3.9K
The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
3.9K
Magnetic Field Of A Current Loop
4.4K
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.
4.4K
Force On A Current Loop In A Magnetic Field
3.2K
Magnetic forces on wires carrying current are most frequently applied in motors. A DC motor is a device that converts electrical energy into mechanical work. In motors, wire loops are enclosed in a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate. The direction of the current is reversed once the loop's surface area is lined up with the magnetic field, causing a constant torque on the loop. During the process,...
3.2K
Atomic Nuclei: Nuclear Relaxation Processes
632
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.
632
Magnetic Field due to Moving Charges
8.5K
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...
8.5K
Magnetic Force Between Two Parallel Currents
3.5K
Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
3.5K

