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相关概念视频

Electromagnetic Waves01:30

Electromagnetic Waves

James Clerk Maxwell formulated a single theory combining all the electric and magnetic effects scientists knew during that time, calling the phenomena his theory predicted “Electromagnetic waves”. He brought together all the work that had been done by brilliant physicists such as Oersted, Coulomb, Gauss, and Faraday and added his own insights to develop the overarching theory of electromagnetism. Maxwell’s equations, combined with the Lorentz force law, encompass all the laws of electricity and...
Generating Electromagnetic Radiations01:10

Generating Electromagnetic Radiations

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 the...
Intensity Of Electromagnetic Waves01:22

Intensity Of Electromagnetic Waves

The energy transport per unit area per unit time, or the Poynting vector, gives the energy flux of an electromagnetic wave at any specific time. For a plane electromagnetic wave with E0 and B0 as the peak electric and magnetic fields and traveling along the x-axis, the time-varying energy flux can be given by the following equation:
Standing Electromagnetic Waves01:15

Standing Electromagnetic Waves

Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Electromagnetic Wave Equation01:24

Electromagnetic Wave Equation

Maxwell's equations for electromagnetic fields are related to source charges, either static or moving. These fields act on a test charge, whose trajectory can thus be determined using suitable boundary conditions. The objective of electromagnetism is thus theoretically complete.
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations: What...
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

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:

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相关实验视频

Updated: May 11, 2026

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
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从可电调的互子波段极声元表面产生局部到非局部的二次波.

Jaesung Kim1, Hyeongju Chung1, Seongjin Lee1

  • 1Department of Electrical Engineering, Ulsan National Institute of Science and Technology (UNIST), Ulsan, 44919, Republic of Korea.

Advanced science (Weinheim, Baden-Wurttemberg, Germany)
|November 29, 2025
PubMed
概括

这项研究引入了一种新的可调节的超表面,用于独立控制第二波 (SH) 信号强度和波长. 这一突破为先进的光子应用增强了非线性光学功能.

关键词:
角度多重复合光学 角度多重复合光学双重制能力的双重制能力电气调节电气调节本地到非本地过程过程.非线性元面是指非线性元面.非局部共振的共振.第二个和的第二代.

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科学领域:

  • 光子学和光学 在光子学和光学.
  • 材料科学 材料科学 材料科学
  • 量子光学是一种量子光学.

背景情况:

  • 非线性光学元表面提供波长下的光控制.
  • 同时调整波信号强度和光谱响应是一个关键的挑战.

研究的目的:

  • 呈现一个电调 polaritonic metasurface 独立控制第二波 (SH) 生成强度和光谱峰值波长.
  • 展示一种混合方法,将局部和非局部光学模式结合起来.

主要方法:

  • 在多个量子井层内工程模态重叠.
  • 使用局部表面等离子体共振 (基本频率) 和横向磁导模式共振 (SH频率) 的组合.
  • 采用电压控制调制和角度控制的光谱调.

主要成果:

  • 通过电压实现了SH强度的独立控制,通过角度实现了光谱调整.
  • 证明与局部和非局部光学模式相关的分离的自由度.
  • 通过角度解析的非线性反射测量验证了独立的可调性.

结论:

  • 混合超表面为非线性光学中增强灵活性和功能控制提供了总体框架.
  • 这种方法使SH光谱峰值和强度的独立调整成为可能,克服了一个基本的挑战.
  • 为非线性信号处理,角度复合光子学和量子光学的应用铺平了道路.