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Error Estimation due to approximations in Shack-Hartmann sensor based measurement of high slope freeform wavefront

机译:基于Shack-Hartmann传感器的高斜率自由形式波阵面测量中的近似误差估计

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This paper addresses the challenges and limitations involved in the measurement of steep freeform wavefront by usingShack-Hartmann Sensor (SHS). To estimate the slope errors, Zemax simulation tool is used to design a SHS setup includingarray of lenslets and detector plane with predefined specifications. In first step, error due to approximation of tilted planewavefront over curved wavefront is simulated. Plane, tilted, curved and tilted-curved wavefronts are defined usingappropriate ray source objects. The centroids of the focal spots of lenslets are calculated based on the detector data obtainedby using ray tracing method, which is done by an in-plane scanning aperture for segmented local wavefrontssequentially.The scanning aperture is used to block rays from more than one lenslet array. Centroids from the focus spotsare calculated and the slopes are estimated with respect to collimated reference wavefront for each ray trace process.Further, matrix of slope errors is used as an input for MATLAB routines for surface reconstruction and error estimation.Based on the simulation data, it is found that the assumption used in the Shack-Hartmann wavefront measurementintroduce residual errors. For example a 50 wave peak to valley input and 1.19 mm thick lenslet array can give up to 9waves of residual form error. However, very thin lenslets can have very less residual error.The effect of shift of focal plane,tilted plane wavefront and curve wavefront during the reconstruction using SHS is reported.
机译:本文通过使用以下方法解决了陡峭自由形式波前测量中的挑战和局限性 Shack-Hartmann传感器(SHS)。为了估算斜率误差,Zemax仿真工具用于设计SHS设置,包括 具有预定规格的小透镜和探测器平面的阵列。第一步,由于倾斜平面的近似而产生的误差 模拟了弯曲波前的波前。使用以下方法定义平面,倾斜,弯曲和倾斜弯曲的波前 适当的射线源对象。根据获得的检测器数据计算小透镜焦点的质心 通过使用射线追踪方法,该方法是通过平面内扫描孔径对分段的局部波前进行的 扫描孔径用于阻挡来自多个小透镜阵列的光线。来自焦点的质心 计算每个射线跟踪过程相对于准直参考波前的斜率,并估计斜率。 此外,将坡度误差矩阵用作MATLAB例程的输入,以进行曲面重建和误差估计。 根据仿真数据,发现在Shack-Hartmann波前测量中使用的假设 引入残留错误。例如,峰谷输入为50波,而厚度为1.19 mm的小透镜阵列则最多可产生9个 残留形式误差波。但是,非常细的小透镜的残留误差会很小。 报道了在利用SHS重建过程中倾斜的平面波前和曲线波前。

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