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Wave front and phase correction for double-ended gauge block interferometry

机译:波前和相位校正,用于双端量块干涉仪

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摘要

Double-ended interferometry has several benefits over single-ended gauge block interferometry: there is no need for wringing, which wears surfaces and requires expertise, and there is improved repeatability, since there is no variation due to inconsistent wringing conditions or form errors of the gauge block surfaces. Some disadvantages of double-ended interferometry are that absolute phase change correction is needed for the gauge block and its uncertainty has a double effect on total uncertainty. In addition, elimination of the wavefront error is more complicated than with single-ended interferometry. A simple optical modification that enables double-ended interferometer (DEI) measurements with the MIKES interferometer for long gauge blocks is presented. This modification is applicable to almost any single-ended interferometer (SEI). A procedure for evaluating the wave front correction for different parts of the interferogram of DEI is explained, and a modification and software with capability for nine-point phase stepping is presented. Three independent methods for evaluation of the phase correction were studied. One of them uses integrating sphere for the surface roughness correction and literature values for the phase change due to complex refractive index of material correction. The second evaluates the phase correction from the difference between DEI and SEI results obtained with a quartz platen. The third uses differences-from separate measurements-between the results obtained with quartz or steel auxiliary platens. Only a few gauge blocks per set need testing to obtain phase correction. SEI and DEI results with different phase correction determination methods are presented and evaluated. The uncertainty estimate for gauge block calibration with DEI gives a similar standard uncertainty to that with the best SEIs, u = root(10.0 nm)(2) + (118 x 10(-9)L)(2).
机译:与单端量块干涉仪相比,双端干涉仪具有以下几项优势:无需拧紧,不磨损表面且需要专业知识,并且可重复性得到改善,因为不存在因不一致的拧紧条件或形状误差而引起的变化。量块表面。双端干涉测量法的一些缺点是,量规模块需要绝对相位变化校正,并且其不确定度对总不确定度有双重影响。此外,消除波前误差比使用单端干涉仪更为复杂。提出了一种简单的光学修改方法,该方法可以使用MIKES干涉仪对长规格模块进行双端干涉仪(DEI)测量。此修改几乎适用于任何单端干涉仪(SEI)。说明了评估DEI干涉图不同部分的波前校正的过程,并提出了一种具有九点相位步进能力的修改和软件。研究了三种独立的相位校正评估方法。其中之一使用积分球进行表面粗糙度校正,并使用文献资料来校正由于材料校正的复数折射率引起的相变。第二种方法根据石英压板获得的DEI和SEI结果之间的差异评估相位校正。第三种方法是使用石英或钢制辅助压板获得的结果之间的差异(来自单独的测量值)。每套只有几个量块需要进行测试以获得相位校正。提出并评估了采用不同相位校正确定方法的SEI和DEI结果。使用DEI进行量规校准的不确定度估计值与最佳SEI的标准不确定度相似,u = root(10.0 nm)(2)+(118 x 10(-9)L)(2)。

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