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Optical fiber Fabry-Perot cavity applied to an optical microphone

机译:光纤法布里-珀罗腔应用于光学麦克风

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A new installation structure of optical fiber Fabry-Perot (F-P) cavity is proposed to function in an optical microphone. The F-P cavity consists of an optical fiber end with self-focused lens and a sound-sensitive membrane. Distance between the two parts is the F-P cavity length. The sound membrane is produced by semiconductor sculpture, which guarantees its tiny size, uniform thickness and high sensitivity to sound. The membrane responds to the sound vibration and vibrates in concavo-convex shape, which results in the change of cavity length, so the F-P cavity performs as an optical microphone. A mathematical model for this kind of arc F-P cavity is also proposed to study the optical microphone. The arc end is assimilated to a step-like model, so the arc F-P cavity equals an assembly of annular plane-end F-P cavities. The mathematical model is educed by simple integral of the annular plane-end F-P cavities and multi-beam interference theory. Relevant simulation and experiments are executed, which confirm the accuracy of the mathematical model and feasibility of the installation structure.
机译:提出了一种新的光纤法布里-珀罗(F-P)腔的安装结构,该结构可在光学麦克风中发挥作用。 F-P腔由一个带有自聚焦透镜的光纤端和一个声敏膜组成。两部分之间的距离是F-P腔的长度。音膜是由半导体雕塑制成的,从而保证了其微小的尺寸,均匀的厚度和对声音的高灵敏度。膜片响应声音振动并以凹凸形状振动,这导致腔体长度发生变化,因此F-P腔体起到了光学麦克风的作用。还提出了一种用于此类弧形F-P腔的数学模型,以研究光学麦克风。弧形端被同化为阶梯状模型,因此弧形F-P腔等于环形平面端F-P腔的组合。通过对环形平面端部F-P腔的简单积分和多光束干涉理论建立了数学模型。进行了相关的仿真和实验,证实了数学模型的准确性和安装结构的可行性。

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