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Optimum lens aperture in phase-shifting speckle interferometric setups for maximum accuracy of phase measurement

机译:相移斑点干涉仪设置中的最佳镜头光圈可最大程度地提高相位测量的准确性

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Negative exponentially distributed intensities of speckle fields seem unfavorable in terms of precision metrology, if interferometric setups are involved with a saturable photodetector and an analog-to-digital converter that imposes a finite resolution. By spatial integration, extended detector apertures modify the intensity distribution toward a less awkward function. However, because the detector aperture also integrates over points of rapidly changing speckle phases, this is done at the expense of a lower modulation of measured intensity during phase shire. An optimum set of parameters is calculated here, consisting of values for the lens aperture, the mean speckle intensity, and the beam ratio. The remaining phase-measurement error assumes its minimum of 10.6 mrad when the space-bandwidth product of the lens-detector system (thus concerning the lens aperture) is 0.31, the mean speckle intensity is 1/11 of the saturation intensity, and the reference intensity is four times higher than the mean speckle intensity. The 90 degrees phase-shift algorithms with either three, four, or five frames turned out to be quite powerful, even with interference signals of rather poor modulation. Not needing a very small lens aperture is interesting, because stopping down, the lens is a trade-off with the limited power of the laser. (C) 1997 Optical Society of America.
机译:如果干涉测量装置与可饱和的光电探测器和施加有限分辨率的模数转换器有关,则散斑场的负指数分布强度就精密计量而言似乎是不利的。通过空间整合,扩展的检测器孔径可以使强度分布朝着不太尴尬的功能方向变化。但是,由于检测器孔径也集成了快速变化的斑点相位点,因此这样做的代价是在相位偏移期间降低了对测量强度的调制。此处计算出一组最佳参数,包括透镜光圈,平均散斑强度和光束比的值。当镜头检测器系统的空间带宽乘积(因此与镜头光圈有关)为0.31,平均斑点强度为饱和强度的1/11时,剩余的相位测量误差假定为最小值10.6 mrad。强度是平均散斑强度的四倍。即使具有调制效果较差的干扰信号,具有三帧,四帧或五帧的90度相移算法也非常强大。不需要非常小的透镜孔径是很有趣的,因为停下来,透镜是在激光功率有限的情况下进行权衡的。 (C)1997年美国眼镜学会。

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