A Remote Sensor For Electro-optic And Magneto-optic Effects Using Fiber Optics And Heterodyne Phase Detection

S. P. Bush, D. Mazzoni, K. Cho, C. Davis
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Abstract

1. Birefringence Detector After the first beamsplitter we have orthogonal polarization states with differing frequency :E, = , / i jJ5eiwlt , E, = m e i W z t + * A X/2 plate precedes the second PBS and is aligned so that the input Polarization to the PBS is at 45 degrees to the PBS axes. This gives Assuming the fiber has negligible birefringence and the 0 and E of the sample are aligned along x,y then the output at the measuring the photocurrents in detectors and resp.port of the fiber is given by :I1 = ? ! ! ! (1 cos( Awt + 2D + $)) 8hv
基于光纤和外差相位检测的电光和磁光遥感器
1. 在第一个分束器之后,我们有不同频率的正交偏振态:E, =, / i jJ5eiwlt, E, = m E i W z t + * A X/2板在第二个PBS之前,并对齐,使PBS的输入偏振与PBS轴呈45度。假设光纤具有可忽略不计的双折射,并且样品的0和E沿x,y对齐,那么在测量检测器和resp中的光电流时的输出。端口表示:I1 = ?! ! ! (1cos (Awt + 2D + $)) 8hv
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