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Point-diffraction interferometer by electro-optic effect in lithium niobate crystals

机译:铌酸锂晶体中电光效应的点衍射干涉仪

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We propose a new point-diffraction interferometer (PDI) based on a pinhole filter made by a z-cut lithium niobate (LN) crystal. A thin aluminium layer with a circular opening is fabricated on the surface of the crystal by conventional photolithography and subsequent aluminium deposition and lift-off. This aluminium layer acts both as electrode and as pinhole filter on the exit face of the crystal, while a uniform planar aluminium layer is deposited on the opposite face. When a voltage is applied across the z-axis of the crystal, the refractive index changes everywhere in the crystal except in a small portion underneath the area of the pinhole. Therefore, the applied voltage causes an uniform phase shift over the aberrated wavefront while leaving unaffected the diffracted reference beam passing through the pinhole. The interference taking place behind the sample produces an interference fringe pattern containing the information on the aberrated wavefront. Four phase shifted images of the fringe pattern are acquired and processed by means of the Carre algorithm to retrieve the aberrated wavefront. The proposed PDI arrangement has several important advantages over the other PDI configurations. The technological processes are very simple, and the phase-shift operation can be applied at very high speed limited only by the minimum acquisition time of the camera device. In fact, the electro-optic effect can be induced onto LN with bandwidths up to several GHz. Moreover, LN is transparent in very wide spectral range from 400 nm to 5500 nm, thus being useful in numerous applications.
机译:我们提出了一种新的点衍射干涉仪(PDI),它基于由z切割铌酸锂(LN)晶体制成的针孔滤光片。通过常规的光刻以及随后的铝沉积和剥离,在晶体表面上制造出具有圆形开口的薄铝层。该铝层既充当电极,又充当晶体出射面的针孔滤光片,而均匀的平面铝层则沉积在相对的面上。当在晶体的z轴上施加电压时,除了在针孔区域下方的一小部分之外,晶体中的各处折射率都会发生变化。因此,所施加的电压在畸变的波前上引起均匀的相移,同时不影响穿过针孔的衍射参考光束。样品后面发生的干涉会产生干涉条纹图案,其中包含有关畸变波阵面的信息。条纹图像的四个相移图像通过Carre算法获取和处理,以获取畸变的波前。与其他PDI配置相比,建议的PDI布置具有几个重要优点。工艺过程非常简单,并且相移操作可以以非常高的速度应用,仅受摄像设备的最小采集时间限制。实际上,可以在带宽高达几GHz的LN上感应电光效应。此外,LN在400 nm至5500 nm的非常宽的光谱范围内都是透明的,因此可用于众多应用。

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