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The Discrete Between O-Ray and E-Ray in Savart Polariscope

机译:在Savart偏光镜中的O射线和电子射线之间的离散

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The spatially modulated polarization interference imaging spectroscopy ( SMPIIS ) is based on the polarization interferometer.The core of the polarization interferometer is the Savart polariscope. When light passing throughpolarizer,the natural light becomes linearly polarized in the direction of the polarization orientation of a linear polarizer.The linearly polarized ray is split into two polarized components by a Savart polariscope. After going through theanalyzer,the two rays get linearly polarized in the polarized orientation of the analyzer and are focused by the imaginglens to form the interferogram and target image. From analyzing the mechanism of formation the interferogram and target image,we find the discrete between ordinary ray ( o-ray ) and extraordinary ray ( e-ray ) greatly influence the intensities and the results of the interferogram and target image. The wave vector of e-ray is obtained by the extensionof Snell's law in the Savart polariscope. According to the relation between the wave vector of e-ray and e-ray,thedirection of e-ray is solved. After the directions of o-ray and e-ray are given, the formula of the discrete between o-rayand e-ray can be got by calculating.
机译:空间调制偏振干扰成像光谱(SMPIIS)基于偏振干涉仪。偏振干涉仪的核心是Savart偏振镜。当光通过通向器时,自然光在线性偏振器的偏振取向方向上变得线性偏振。通过Savart偏振镜,线性偏振光被分成两个偏振分量。经过Theanalyzer之后,两条光线以分析仪的偏振取向线性偏振,并由其聚焦,以形成干扰图和目标图像。通过分析形成干涉图和目标图像的机制,我们发现普通射线(O射线)和非凡(E-RAY)之间的离散地影响了干涉图和目标图像的强度和结果。 E-ray的波矢量是通过Snell在Savart偏光镜中的延伸法的延伸。根据电子射线和电子射线的波向量之间的关系,解决了电子射线的指标。在给出O射线和电子射线的方向之后,通过计算可以通过计算O-Rayand电子射线之间的离散的公式。

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