概括
我们使用级联元表面和电子束引入极化 Smith-Purcell 辐射. 这种方法可以控制新型自由电子驱动装置的旋转和轨道角动量.
科学领域:
- 光学和光子学 在光学和光子学.
- 凝聚物质物理学 凝聚物质物理学
- 自由电子物理学 自由电子物理学
背景情况:
- 史密斯-普塞尔辐射是当一个带电粒子,如电子束,通过周期结构时产生的.
- 超表面可以对光极化和波面成形提供先进的控制.
- 产生结构光,如束,具有特定的极化特性是一个关键的研究领域.
研究的目的:
- 介绍和研究极化旋史密斯-普尔塞尔辐射的产生.
- 探索级联元表面在控制辐射的自旋和轨道角动量的作用.
- 证明实现各种极化状态和拓电荷的可行性.
主要方法:
- 使用由格子和相梯度元面组成的级联元面.
- 电子束与级联元表面相互作用,产生辐射.
- 分析发射的 Smith-Purcell 辐射的极化状态 (线性和圆形) 和拓电荷.
主要成果:
- 成功生成了极化 Smith-Purcell 辐射.
- 证明了级联的超表面决定了旋转和轨道角动量.
- 实现对线性和圆形极化进行控制,并观察到带有拓电荷变化的奇拉性转换.
结论:
- 拟议的方法可以产生极化 Smith-Purcell 辐射.
- 级联元表面对于调整电子束辐射的角动量特性是有效的.
- 这项研究推动了自由电子驱动光学设备和结构光源的开发.
相关概念视频
Potential Due to a Polarized Object
398
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
398
Plane Electromagnetic Waves II
3.1K
Consider a plane wavefront traveling in position x-direction with a constant speed. This wavefront can be utilized to obtain the relationship between electric and magnetic fields with the help of Faraday's law.
3.1K
Standing Waves in a Cavity
918
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
918
Plane Electromagnetic Waves I
3.6K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed...
The EM field is assumed...
3.6K
Equipotential Surfaces and Conductors
3.4K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
3.4K
Generating Electromagnetic Radiations
2.9K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
2.9K


