狭窄线宽全光学微波振荡器基于单模光纤的扭转辐射声学模式
Wen Wang1,2, Wenjun He1,2,3, Xinyue Fang1,2
1Key Laboratory of Instrumentation Science and Dynamic Measurement Ministry of Education, North University of China, Taiyuan 030051, China.
Micromachines
|January 25, 2025
概括
一个全新的全光微波振荡器利用单模光纤声学模式来产生狭窄的线宽. 这种稳定,低相位噪声的设备为先进的雷达,通信和传感应用提供了潜力.
科学领域:
- 光子学是指光子学的使用方法.
- 光学工程是指光学工程.
- 声学 声学 在声学方面
背景情况:
- 全光微波振荡器对于高性能系统至关重要.
- 在这些振荡器中实现狭窄的线宽和高稳定性仍然是一个挑战.
研究的目的:
- 提出和验证一个Hz级窄线宽全光微波振荡器.
- 在单模光纤 (SMF) 系统中利用扭转辐射声学模式 (TR2,m).
主要方法:
- 使用双腔设计 (20公里主,5公里小SMF) 与刺激的布里卢恩散射增益.
- 实现TR2.7模式锁定的非线性偏振旋转和单纵模式 (SLM) 输出的维尼尔效应.
- 减少被动共振腔的线宽,以实现TR2.7模式的6.281Hz的线宽.
主要成果:
- 在TR2.7模式下显示了6.281Hz的窄线宽.
- 实现了高压抑比:43dB (音响模式) 和54dB (侧面模式).
- 在40分钟的功率波动±0.49dB和频率波动±0.187kHz的情况下,表现出极好的稳定性.
- 在10kHz偏移时报告了低相噪声-110dBc/Hz.
结论:
- 拟议的基于SMF声模式的全光微波振荡器表现出了卓越的性能.
- 该设备提供高稳定性,窄线宽和低相位噪声.
- 潜在的应用包括高精度雷达,远距离光通信和先进的光纤传感.
相关概念视频
Oscillations In An LC Circuit
2.2K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
2.2K
Modes of Standing Waves: II
828
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....
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....
828
Standing Waves in a Cavity
855
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:
855


