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相关概念视频

Standing Waves in a Cavity01:28

Standing Waves in a Cavity

886
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:
886
Plane Electromagnetic Waves I01:30

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...
3.6K
Traveling Waves: Lossless Lines01:27

Traveling Waves: Lossless Lines

128
The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx  and a shunt capacitance CΔx.
128
Modes of Standing Waves: II01:04

Modes of Standing Waves: II

841
The starting point for expressing the modes of standing waves is understanding the boundary conditions that the waves must follow. The boundary conditions are derived from the physical understanding of how the standing waves are sustained, that is, how the vibrating particles of the medium behave at the boundaries imposed on them.
For a tube open at one end and closed at the other filled with air, the modes are such that there is always an antinode at the open end and a node at the closed end....
841
Transfer function and Bode Plots-II01:23

Transfer function and Bode Plots-II

307
In the standard form, the transfer function is shown in constant gain, poles/zeros at origin, simple poles/zeros, and quadratic poles/zeros; each contributing uniquely to the system's overall response. The term represents the magnitude of the simple zero:
307
Transfer function and Bode Plots-I01:19

Transfer function and Bode Plots-I

314
A transfer function presented in its standard form integrates elements' constant gain, the zeros, and poles at the origin, simple zeros and poles, and quadratic poles and zeros. The transfer function can be written as H(ω):
314

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相关实验视频

Updated: Jun 14, 2025

Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities
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普塞尔增益等于零模式波导的波导.

Tang-Chun Liu1, Wen-Hsiang Yu1, Chung-Kai Tseng1

  • 1Department of Optics and Photonics, National Central University, No. 300, Zhongda Rd., Zhongli, Taoyuan, 320317, Taiwan.

Scientific reports
|September 6, 2024
PubMed
概括
此摘要是机器生成的。

我们用元材料增强了零模式波导 (ZMWs),以实现均的分子激发和改进的光. 这使得高度生物化学反应的实时单分子感应成为可能.

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Last Updated: Jun 14, 2025

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Published on: November 30, 2012

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科学领域:

  • 纳米光子学 纳米光子学
  • 生物物理学的生物物理.
  • 分子传感传感器是一种分子传感器.

背景情况:

  • 零模式波导 (ZMWs) 对于单分子检测至关重要.
  • 现有的ZMW设计在均激发和光增强方面存在局限性.

研究的目的:

  • 为了提高性能,使用元材料重新设计ZMW.
  • 为了在ZMWs中实现均的电磁场分布.
  • 为了实现灵敏的,实时的单分子分析.

主要方法:

  • 在ZMW设计中引入元材料.
  • 导出用于波 impedance 的闭式表达式.
  • 有限差异时间域模拟用于验证.
  • 与超快激光器进行集成,以激发激发.

主要成果:

  • 超材料集成可以实现零级共振模式.
  • 实现了几乎恒定的电磁场分布,使分子激发率均等.
  • 孔腔细胞效应增强光,缩短寿命.
  • 激发体积降低到子zeptoliter.
  • 光寿命缩短到皮秒级.

结论:

  • 增强元材料的ZMW比现有设计提供了更高的性能.
  • 增强的ZMW可以促进单分子实时 (SMRT) 传感.
  • 在微分子度下,生物化学反应可以实时分析.