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

机译:Savart偏光镜中O射线和E射线之间的离散

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摘要

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 through polarizer,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 the analyzer,the two rays get linearly polarized in the polarized orientation of the analyzer and are focused by the imaging lens 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 extension of Snell's law in the Savart polariscope. According to the relation between the wave vector of e-ray and e-ray,the direction of e-ray is solved. After the directions of o-ray and e-ray are given, the formula of the discrete between o-ray and e-ray can be got by calculating.
机译:空间调制偏振干涉成像光谱(SMPIIS)基于偏振干涉仪,偏振干涉仪的核心是Savart偏振镜。当光通过偏振片时,自然光在线性偏振片的偏振取向方向上变为线性偏振。 Savart偏振镜将线偏振射线分为两个偏振分量。经过分析仪后,两条光线在分析仪的偏振方向上呈线性偏振,并被成像透镜聚焦,形成干涉图和目标图像。通过分析干涉图和目标图像的形成机理,我们发现普通射线(o射线)和非常规射线(e射线)之间的离散极大地影响了干涉图和目标图像的强度和结果。 e射线的波矢是通过在Savart偏光镜中斯涅尔定律的扩展获得的。根据电子射线的波矢与电子射线之间的关系,求出电子射线的方向。给出o射线和e射线的方向后,可以通过计算得到o射线与e射线之间的离散关系式。

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