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Initial structure of dispersion objective for chromatic confocal sensor based on doublet lens

机译:基于双重透镜的色耦合传感器分散目标的初始结构

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摘要

Dispersion objective is the crucial device of chromatic confocal sensor (CCS). The dispersion range and numerical aperture (NA) determine the measurement range and the maximum measurement slope of CCS, respectively. In this paper, we present two kinds of initial structures of dispersion objective for CCS based on doublet lens, which are suitable for the design of dispersion objectives with large dispersion range and high NA, respectively. We categorized the doublet lens by the distribution of optical power into three kinds of surface structures, divided the distribution area of the glass material into four quadrants according to the refractive index and Abbe number, and then combined to obtain 36 kinds of doublet lens structures. We analyzed the characteristics of the dispersion produced by each structure, and proposed L-type, S-type, and two types of dispersion. The influence of dispersion type on the dispersion range and NA of CCS was deduced, and two kinds of dispersion objective initial structures were constructed based on the doublet lenses with different dispersions. Taking the single wavelength spherical aberration of starting wavelength (400nm) less than 1 mu m as the optimization goal, the 10 sets of initial structures were optimized and the dispersion range and NA variation direction before and after optimization were compared and evaluated. The design results shown that the initial structure based on the doublet lens that produces L-type dispersion is suitable to design sensors with larger dispersion range, while the initial structure using the doublet lens which produces S-type dispersion is more conducive to designing the sensors with higher NA.
机译:色散物镜是彩色共焦传感器(CCS)的关键装置。分散范围和数值孔径(NA)分别确定CCS的测量范围和最大测量斜率。在本文中,我们为基于双重透镜的CCS的两种初始分散目标结构,其适用于具有大分散范围和高Na的色散物镜的设计。通过将光功率分配到三种表面结构中,将双层透镜分类为三种表面结构,将玻璃材料的分布区域分成四个象限,然后组合以获得36种双重透镜结构。我们分析了每个结构产生的分散体的特性,以及提出的L型,S型和两种分散体。推导出分散型对分散范围和CCS的Na的影响,并且基于具有不同分散体的双重透镜构建两种分散物镜初始结构。以优化目标采用小于1μm的起始波长(400nm)的单波长球形像差,优化10组初始结构,并进行比较和评估前后的分散范围和Na变化方向。设计结果表明,基于双重透镜的初始结构,该初始结构产生L型分散体,适用于具有较大色散范围的传感器,而使用双峰透镜的初始结构更有利于设计传感器na较高。

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