A Holographic Interferometer For The Study Of Transparent Media

E. Vanhoecke
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引用次数: 1

Abstract

Holographic optical elements (HOEs)are more and more commonly used in all kind of optical design. When used in interferometry, holographic optics not only make it possible to avoid the use of expensive optical precision components, but allow under certain conditions a "holographic null correction" for all optical aberrations. In OIP, a holographic interferometer was built with the aim of studying transparent media. Convection phenomena in transparent fluida can be observed in real time; when using a complementary pair of lenses, deviations of a copy lens from a master one can be visualized. The interferometer can have a rather large visualization area (almost 100mm x 100mm), and has the possibility to zoom in onto the object. The image may be visualized by means of a CCD-camera. The interferometer operates entirely with HOE-technology, no conventional lens or beamsplitter is used, with exception for the microscope objective to produce a diverging laser beam. Four HOEs in dichromated gelatine are used to realize interferograms in a Mach-Zehnder configuration. The first acts as a holographic beamsplitter to produce a reference and an object beam; the second and the third are diffraction elements which convert the diverging object beam into a collimated one and back into a converging beam. On the last HOE a rest pattern has been recorded. The interference of an "active" object beam with the holographic "reconstructed" one produces the real-time interferogram corrected for optical aberrations of the system. The interferometer operates with an Ar-laser (λ=514nm) at this moment but will be modified to operate with a small built-in HeNe-laser.
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研究透明介质的全息干涉仪
全息光学元件在各种光学设计中得到越来越广泛的应用。当用于干涉测量时,全息光学不仅可以避免使用昂贵的光学精密元件,而且允许在某些条件下对所有光学像差进行“全息零校正”。在OIP中,为了研究透明介质,建立了一个全息干涉仪。可实时观测透明流体中的对流现象;当使用一对互补透镜时,复制透镜与主透镜的偏差可以可视化。干涉仪可以有一个相当大的可视化区域(几乎100毫米× 100毫米),并有可能放大到对象。所述图像可通过ccd摄像机可视化。干涉仪完全使用hoe技术,不使用传统的透镜或分束器,除了显微镜物镜产生发散激光束。用重铬酸盐明胶中的4个hos实现了马赫-曾德结构的干涉图。第一种作为全息分束器产生参考光束和目标光束;第二个和第三个是衍射元件,它们将发散的物体光束转换成准直光束,然后再转换回会聚光束。在最后一次HOE中记录了休息模式。“有源”物体光束与全息“重构”光束的干涉产生了校正系统光学像差的实时干涉图。目前,干涉仪使用ar激光器(λ=514nm),但将被修改为使用小型内置氦氖激光器。
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