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Surface characterization techniques for determining the root-mean-square roughness and power spectral densities of optical components

机译:用于确定光学组件的均方根粗糙度和功率谱密度的表面表征技术

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摘要

Surface topography and light scattering were measured on 15 samples ranging from those having smooth surfaces to others with ground surfaces. The measurement techniques included an atomic force microscope, mechanical and optical profilers, confocal laser scanning microscope, angle-resolved scattering, and total scattering. The samples included polished and ground fused silica, silicon carbide, sapphire, electroplated gold, and diamond-turned brass. The measurement instruments and techniques had different surface spatial wavelength band limits, so the measured roughnesses were not directly comparable. Two-dimensional power spectral density (PSD) functions were calculated from the digitized measurement data, and we obtained rms roughnesses by integrating areas under the PSD curves between fixed upper and lower band limits. In this way, roughnesses measured with different instruments and techniques could be directly compared. Although smaller differences between measurement.. techniques remained in the calculated roughnesses, these could be explained mostly by surface topographical features such as isolated particles that affected the instruments in different ways. (C) 2002 Optical Society of America. [References: 56]
机译:测量了15个样品的表面形貌和光散射,样品范围从具有光滑表面的样品到具有地面表面的样品。测量技术包括原子力显微镜,机械和光学轮廓仪,共聚焦激光扫描显微镜,角度分辨散射和总散射。样品包括抛光和研磨后的熔融石英,碳化硅,蓝宝石,电镀金和金刚石车削的黄铜。测量仪器和技术具有不同的表面空间波长带限值,因此所测量的粗糙度不能直接比较。从数字化的测量数据中计算出二维功率谱密度(PSD)函数,并且通过对固定的上下限之间的PSD曲线下的面积进行积分,我们获得了均方根粗糙度。这样,可以直接比较使用不同仪器和技术测得的粗糙度。尽管测量技术之间的较小差异仍保留在计算出的粗糙度中,但这些可以主要通过表面形貌特征来解释,例如以不同方式影响仪器的孤立颗粒。 (C)2002年美国眼镜学会。 [参考:56]

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