来自复杂电场的通道波导中的模式强度的确定
Isaac Doughan1, Atri Halder2, Igor Reduto2
1Center for Photonics Sciences, University of Eastern Finland, P.O. Box 111, 80101, Joensuu, Finland. isaac.doughan@uef.fi.
Scientific reports
|November 20, 2024
概括
研究人员开发了一种新的方法来测量非对称波导中的引导场的模式强度和相位信息. 该技术使用干扰度测量进行精确的光学分析.
科学领域:
- 光子学和波导光学 波导光学
- 电磁学和光学 电磁学和光学
- 材料科学 材料科学 材料科学
背景情况:
- 在不对称的波导中描述导向场对于光学设备的性能至关重要.
- 准确确定模式强度和相位对于理解光传播至关重要.
- 现有的阶段检索方法可能是复杂的和非碎的.
研究的目的:
- 开发一种创新的技术,以独特地确定非对称通道波导中的模式强度.
- 为了检索复杂的电场分布的振幅和相位信息.
- 提供一种直接的方法来测量多式联调分散.
主要方法:
- 在波导出口平面上利用自我引用的干扰度测量.
- 使用定制的波面折叠干扰仪来测量复杂的跨光谱密度 (CSD) 函数.
- 从测量的CSD数据构建总复杂的电场.
主要成果:
- 成功确定了非对称条形波导中的允许模式的独特模式强度.
- 直接从电场分布中获取相位信息,包括模式间分散.
- 在各种内条件下实验证明了该方案,显示了不同的模式强度分布.
结论:
- 开发的技术为全面的光场表征提供了一个有前途和替代的方法.
- 这种方法可以精确测量模式强度和相位,这对于波导设计和分析至关重要.
- 实验验证证证实了该技术对不同波导输入的稳定性和适用性.
相关概念视频
Intensity Of Electromagnetic Waves
4.4K
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:
4.4K
Propagation Speed of Electromagnetic Waves
3.3K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
3.3K
Electromagnetic Waves in Matter
2.9K
Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the...
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the...
2.9K
Standing Waves in a Cavity
869
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:
869
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
Standing Electromagnetic Waves
1.5K
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...
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
1.5K


