在石墨烯盘中的THz驱动等离子体诱导的强过渡性磁场
Jeong Woo Han1, Pavlo Sai2, Dmytro B But2
1Universität Duisburg-Essen, Fakultät für Physik, 47057, Duisburg, Germany.
Nature communications
|November 19, 2023
概括
工程设计的石墨烯磁盘使用等离子体共振产生强烈的,短暂的磁场. 这种通过超快法拉第旋转观察到的高效方法,为元材料中的光诱导磁性提供了新的控制.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 塑制剂是一种塑制剂.
- 超材料是什么?超材料是什么?
背景情况:
- 循环极化光可以通过相反的法拉第效应在固体中诱导有效的磁场.
- 等离子共振可以对光-物质相互作用提供可调节的控制,与固定的物质特性不同.
- 工程化超材料可以增强光诱导的磁场.
研究的目的:
- 通过在石墨烯盘中使用等离子体循环电流来证明光诱导的短暂磁场的高效生成.
- 探索等离子体共振的可调性,用于控制磁场生成.
- 量化诱导磁场的强度和动态.
主要方法:
- 制造石墨烯盘以支持等离子体共振.
- 在太赫兹频率的循环极化光激发.
- 测量超快法拉第旋转以检测诱导的磁场.
- 与模拟和参考测量进行比较.
主要成果:
- 石墨烯磁盘表现出3.5 THz的等离子体共振.
- 观察到强烈的超快法拉第旋转 (~1°),表明诱导磁场.
- 诱导的磁场估计在流动度为440nJ cm-2.2时为~0.7 T.
- 在产生光诱导磁场方面实现了高效率.
结论:
- 工程石墨烯结构中的等离子共振提供了一个高效的途径,可以产生可调节的,短暂的磁场.
- 这种方法比传统方法具有显著的优势,仅限于材料特性.
- 这些发现为利用光来控制超材料中的磁性开辟了新的途径.
相关概念视频
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Potential Due to a Magnetized Object
296
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...
296
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
8.7K
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
Induced Electric Fields: Applications
1.6K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.6K
Electric Field of a Charged Disk
2.2K
The simplest case of a surface charge distribution is the uniformly charged disk. Calculating its electric field also helps us calculate the electric field of a large plane of charge.
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
2.2K


