用尾纤光学探头对电场矢量进行单次测量

L. Duvillaret, P. Jarrige, F. Lecoche, G. Gaborit
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引用次数: 0

摘要

只提供摘要形式。在各种可用的专用于电(E)场表征的传感器中,天线的使用构成了最广泛的技术。虽然这种探针很方便,而且灵敏度很高,但它们仍然是侵入性的,而且带宽有限。相反,光纤电光换能器1是完全介电的,毫米大小,允许使用等效时间采样对从直流电到几千赫兹,甚至到太赫兹的频率的电场矢量进行测量。此外,最近的发展导致用单个EO探针同时表征2个横向电场矢量分量2。基于偏振状态调制,EO换能器连接到远程(高达30米)光电装置,包括超低噪声激光器馈送探头和实时光学装置来管理调制处理。自动化和伺服控制的测量台是无温度依赖的。可用的测量动态超过100db,范围从小于1v - m-1。Hz-1/2到空气中的击穿电场。在会议期间,将首先对BO传感器和其他技术进行详尽的比较。这种分析将基于传感器的固有特性,如灵敏度、频率带宽、矢量选择性、空间分辨率和待测场的诱导扰动。在回顾了BO效应的原理之后,将描述光探针的光学排列。将介绍BO系统的特性以及说明BO传感器潜力的实验结果。在这些例子中,测量空气中的脉冲b场(脉冲功率),水(脉冲状态下的特定吸收率评估)或等离子体(放电相关的b场的实时演变)将被显示。
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Single shot measurements of the E-field vector with pigtailed optical probes
Summary form only given. Over the variety of available sensors dedicated to electric (E)-field characterization, the use of antennas constitutes the most widespread technique. While such probes are convenient and provide a good sensitivity, they remain invasive and bandwidth limited. At the opposite, fibered electro-optic transducers1 are fully dielectric, millimeter sized and allow to perform measurements of the E-field vector from DC to several gigahertz and even up to terahertz frequencies using equivalent-time sampling. Furthermore, recent developments lead to a simultaneous characterization of 2 transverse E-field vector components with a single EO probe2. Based on polarization state modulation, the EO transducer is linked to a remote (up to 30 meters) optoelectronic set-up including a ultra low noise laser feeding the probe and a real time optical set-up to manage the modulation treatment. The automated and servo controlled measurement bench is temperature dependent free. The available measurement dynamics exceeds 100 dB, ranging from less than 1 V. m-1. Hz-1/2 up to the breakdown electric field in air.An exhaustive comparison between BO sensors and other technologies will be firstly given during the conference. This analysis will be based on intrinsic sensor properties, such as sensitivity, frequency bandwidth, vectorial selectivity, spatial resolution and induced perturbation on the field to be measured. After recalling the principles of the BO effect, the optical arrangement of the optical probes will be described. The characterization of the BO system will be presented together with experimental results illustrating the potentialities of BO sensors. Among these examples, measurements of pulsed B-field in air (pulsed power), water (specific absorption rate evaluation in pulsed regime) or in plasma (real time evolution of the electrical discharge associated B-field) will be shown.
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