Self-Calibrated Absolute Thickness Measurement of Opaque Specimen Based on Differential White Light Interferometry

被引:13
|
作者
Lu, Xu [1 ,2 ]
Yuan, Yonggui [1 ,3 ]
Ma, Chi [1 ,2 ]
Zhu, Haibo [1 ,2 ]
Zhu, Yunlong [1 ,2 ]
Yu, Zhangjun [1 ,2 ]
Zhang, Xiaojun [1 ,2 ]
Jiang, Fuqiang [1 ,2 ]
Zhang, Jianzhong [1 ,2 ]
Li, Hanyang [1 ,2 ]
Yang, Jun [1 ,4 ]
Yuan, Libo [1 ,5 ]
机构
[1] Harbin Engn Univ, Key Lab In Fiber Integrated Opt, Minist Educ China, Harbin 150001, Peoples R China
[2] Harbin Engn Univ, Coll Phys & Optoelect Engn, Harbin 150001, Peoples R China
[3] Harbin Engn Univ, Coll Informat & Commun Engn, Harbin 150001, Peoples R China
[4] Guangdong Univ Technol, Sch Informat Engn, Guangzhou 510008, Peoples R China
[5] Guilin Univ Elect Technol, Photon Res Ctr, Guilin 541004, Peoples R China
基金
中国国家自然科学基金;
关键词
Measurement uncertainty analysis; opaque specimens; self-calibration; thickness measurement; white light interferometry; ZNO THIN-FILMS;
D O I
10.1109/TIM.2020.2966315
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
In this article, we present a self-calibrated absolute thickness measurement method for opaque specimens based on fiber-optic white light interferometry. A new type of self-reference probe, which is composed of a fiber ferrule, an integrated beam splitter, and a gradient index lens, is presented. In our setup, two probes of this kind are fixed facing each other, and the distance between them can be measured. Then we insert a specimen between the probes and measure the distance between the specimen surfaces and probes on both sides. Thisway, a self-calibrated measurement of specimen thickness can be realized without the traditional calibration process using a standard thickness sample. Thus, the uncertainty component introduced by the standard thickness sample can be eliminated. The performance of the proposed method is evaluated by measuring standard thickness samples calibrated by the National Institute of Metrology of China, and the results show a good agreement with the nominal values. Also, we analyzed several key uncertainty components, as well as the reliability of our method. The calculated extended measurement uncertainty (k = 2) is 0.06 mu m for Cr specimen with a nominal thickness of 10.56, and 0.08 mu m for Ni specimen with a nominal thickness of 31.46 mu m.
引用
收藏
页码:2507 / 2514
页数:8
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