在具有不均磁性结构的基无形丝带中磁阻效应
Dmitry A Bukreev1, Michael S Derevyanko1, Alexander V Semirov1
1Department of Physics, Pedagogical Institute, Irkutsk State University, 664003 Irkutsk, Russia.
Sensors (Basel, Switzerland)
|October 14, 2023
概括
无形带中的磁阻抗 (MI) 效应显示超过200%的MI,对磁场传感器来说是有前途的. 频率依赖性显示出不均的磁性,通过磁电阻断层扫描进行研究.
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
- 电磁主义 电磁主义
背景情况:
- 磁阻抗 (MI) 效应是一种现象,其中磁性材料的阻抗在应对外部磁场时发生变化.
- 无形磁带,特别是基于铁合金的磁带,以显著的MI性能而闻名.
- 了解MI的频率依赖性和空间分布对于传感器应用至关重要.
研究的目的:
- 通过广泛的交流频率范围 (0.01100 MHz) 调查无形CoFeSiB和CoFeMoSiB带中的磁阻效应.
- 分析交流频率对MI响应特征的影响.
- 为了研究磁带截面内磁性质的不均分布,使用磁电阻断层扫描.
主要方法:
- 计算机模拟和实验测量MI效应.
- 从0.01到100MHz的交流频率依赖阻抗分析.
- 磁阻断断层扫描绘制磁性属性分布的地图.
主要成果:
- 观察到超过200%的最大MI值.
- 发现关键MI响应特征强烈依赖交流频率.
- 在带的截面上不均的磁性特性分布被确定为频率依赖的原因.
结论:
- 无形CoFeSiB和CoFeMoSiB带具有高MI值,因此适合用于磁场传感器开发.
- 磁性冲击的频率依赖性归因于磁性质的空间变化.
- 磁阻抗断层扫描为这些属性分布提供了宝贵的见解,有助于传感器设计.
更多相关视频
07:42Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
Published on: July 20, 2022
2.8K
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
相关概念视频
Magnetic Field Due To A Thin Straight Wire
4.9K
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.
4.9K
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
Colors and Magnetism
11.8K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
11.8K
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
Magnetic Field Due to Two Straight Wires
2.6K
Consider two parallel straight wires carrying a current of 10 A and 20 A in the same direction and separated by a distance of 20 cm. Calculate the magnetic field at a point "P2", midway between the wires. Also, evaluate the magnetic field when the direction of the current is reversed in the second wire.
2.6K
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
