Resolution limit of photorefractive spatial light modulators

P. Amrhein, P. Günter
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Abstract

The experimental set-up of our photorefractive incoherent to coherent converter 1 is shown in figure 1. With two interfering Ar-ion-laser beams (λ=514.5 nm) we write a phase hologram into a photorefractive KNbO3 crystal. Using anisotropic Bragg diffraction 2 we choose the direction of the diffracted beam (λ=632.8 nm) perpendicular to the crystal surface. The input image is projected into the crystal plate anti-parallel to the diffracted beam. A short wavelength transmitting dichroitic beam splitter is used to separate the incoherent light from the diffracted beam. This set-up shows highest resolution 3.
光折变空间光调制器的分辨率极限
我们的光折变非相干到相干转换器1的实验装置如图1所示。利用两个干涉氩离子激光束(λ=514.5 nm)将相位全息图写入光折变KNbO3晶体中。利用各向异性布拉格衍射,我们选择了垂直于晶体表面的衍射光束(λ=632.8 nm)的方向。输入图像被投射到与衍射光束反平行的晶体板中。采用短波长透射二色体分束器将非相干光与衍射光束分离。此设置显示最高分辨率3。
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