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中国物理学会期刊

基于光学Parity-Time对称微腔结构的大范围电场传感器

CSTR: 32037.14.aps.68.20190784

Large-range electric field sensor based on parity-time symmetry cavity structure

CSTR: 32037.14.aps.68.20190784
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  • 为解决传统电场传感器测量范围受限的技术难题, 设计了一种基于光学Parity-Time(PT)对称掺杂电光介质的微腔结构, 提出新的电场传感机制. 利用传输矩阵方法计算结构的传输谱, 发现独特的放大的缺陷模式. 缺陷模式的峰值和波长位置均随外电场变化, 由此可以利用缺陷模峰值变化和波长位置变化两种机制测量同一电场. 测量范围仅受电光介质击穿电场的限制, 可以为0—0.06 V/nm, 几乎涵盖了可能的电场环境. 对峰值变化传感机制, 灵敏度范围38.042—47.558 nm/V; 对波长变化传感机制, 灵敏度范围18.357—18.642 nm2/V, 在测量范围内平均分辨率为0.00925 V/nm.

     

    In order to solve the technical problem of the traditional electric field sensor limited by its measurement range, a parity-time (PT) symmetric microcavity structure doped by electro-optical medium is designed, and a new electric field sensing mechanism is proposed. The transfer matrix method is used to calculate the transmission spectrum of the structure. A unique amplified defect mode is found. The peak value and wavelength position of the defect mode vary with the external electric field. The same electric field can be measured by using two mechanisms. One is to detect the change of the defect mode peak value, and the other is to measure the change of the defect mode wavelength position. The measurement range is limited only by the breakdown field value of the electro-optical medium, which can range from 0 to 0.06 V/nm, covering almost any possible electric field environment. For the peak-value sensing mechanism, the sensitivity range is 38.042—47.558 (nm/V); for the wavelength position sensing mechanism, the sensitivity range is 18.357—18.642 (nm2/V), and the average resolution in the measurement range is 0.00925 V/nm.

     

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