杨练根, 刘丙康, 王选择, 翟中生. 一种提高干涉相位识别精度的方法[J]. 应用光学, 2015, 36(4): 590-595. DOI: 10.5768/JAO201536.0403006
引用本文: 杨练根, 刘丙康, 王选择, 翟中生. 一种提高干涉相位识别精度的方法[J]. 应用光学, 2015, 36(4): 590-595. DOI: 10.5768/JAO201536.0403006
Yang Lian-gen, Liu Bing-kang, Wang Xuan-ze, Zhai Zhong-sheng. Method for improving precision of interferometric phase-recognization[J]. Journal of Applied Optics, 2015, 36(4): 590-595. DOI: 10.5768/JAO201536.0403006
Citation: Yang Lian-gen, Liu Bing-kang, Wang Xuan-ze, Zhai Zhong-sheng. Method for improving precision of interferometric phase-recognization[J]. Journal of Applied Optics, 2015, 36(4): 590-595. DOI: 10.5768/JAO201536.0403006

一种提高干涉相位识别精度的方法

Method for improving precision of interferometric phase-recognization

  • 摘要: 针对开环相移驱动下的单色光干涉测量,提出一种满足四步法的高精度相位识别的方法。首先选取干涉场中存在适当相位差的两像素点,建立相移驱动单周期内两像素点灰度序列值之间的干涉方程组。运用椭圆拟合获取相应干涉方程组参数,然后通过反算序列相位确定逐点驱动步长或序列相位信息。结合序列相位信息,运用Lagrange抛物插值算法,设计计算满足四步法的4幅干涉图,并计算各像素点的初相位。最后,运用多波长算法计算表面形貌并进行误差分析。实验表明:计算得到的方波多刻线样板的Ra值为0.439 0 m,测量误差为0.23%,此方法降低了对测量条件的硬件与环境要求,满足表面形貌高精度测量的要求。

     

    Abstract: For monochromatic light interferometry under open-loop phase shifter, a high precision method for phase recognization was developed to satisfy four-step phase-shift algorithm. Firstly two pixels with suitable phase-difference were selected from the interference field, and the interference equations of the two pixels gray values were established in one phase-shifting cycle. Secondly, the interference equations parameters could be obtained by using ellipse fitting algorithm, and the point-to-point driven step length and sequence phases could be determined through back calculation of sequence phases. Then four interference gray scales meeting the four-step phase-shift algorithm were designed and calculated through Lagrange parabolic interpolation, which were used to calculate the initial phase of every pixel. Finally, the surface topography was calculated through multi-wavelength algorithm and the measurement errors were analyzed. Experimental results show that the Ra value of square wave specimen with multiple grooves is 0.4390m, and the measurement error is 0.23%. This method decreases the requirement for hardware and environment. It can meet the high precision demands of surface topography measurement.

     

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