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Glan-Foucault Prism

Glan-Foucault棱镜

The Glan-Foucault prism achieves polarization by removing one plane of polarization by total internal reflection. It is made of two prisms of calcite with no other intervening material, i.e., with air between them. The O-ray is removed and the E-ray continues straight through the device as shown.

Glan-Foucault棱镜通过全内反射去除一个偏振面来实现偏振。它由两个无其他介质的方解石棱镜组成,即两者之间是空气。O光被去除,而E光则直接通过该装置,如图所示。

One of the advantages of the Glan-Foucault prism is that it can handle the high power densities (about 100 watts/cm2) characteristic of laser work. One disadvantage is a narrow field of view, about 10°. That field of view is widened in the Glan-Thompson prism, which has similar geometry but is cemented together. This extends the angle of view to about 30°, but cuts the maximum continuous power density by a factor of 100 to about 1 watt/cm2.

Glan-Foucault棱镜的一个优点是它可以处理激光工作(约100瓦/平方厘米)所特有的高功率密度。一个缺点是视场狭窄,约为10°。Glan-Thompson棱镜的视场更宽,其几何结构相似,但被粘合在一起。这将视场角度扩展到约30°,但最大连续功率密度降低到约1瓦/平方厘米,即减少了100倍。

The presence of the cement in the Glan-Thompson prism means that the angles must be different, since the critical angle for total internal reflection depends upon the indices of refraction of both materials at an interface.

由于格兰-汤普森棱镜中存在水泥,角度必须不同,因为全内反射的临界角取决于两种材料在界面处的折射率。
Polarizing prisms
偏振棱镜
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Polarization concepts
索引偏振概念
 
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