Physical spherical phase compensation in reflection digital holographic microscopy

Reflection configured digital holographic microscopy (DHM) can perform accurate optical topography measurements of reflecting objects, such as MEMs, MOEMs, and semiconductor wafer. It can provide non-destructive quantitative measurements of surface roughness and geometric pattern characterization wi...

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Main Authors: Qu, Weijuan, Chee, Oi Choo, Tan, Lewis Rongwei, Xu, Qiangsheng, Wang, Zhaomin, Xiao, Zhenzhong, Anand, Asundi
Other Authors: School of Mechanical and Aerospace Engineering
Format: Article
Language:English
Published: 2013
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Online Access:https://hdl.handle.net/10356/99611
http://hdl.handle.net/10220/13639
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-996112020-03-07T13:22:19Z Physical spherical phase compensation in reflection digital holographic microscopy Qu, Weijuan Chee, Oi Choo Tan, Lewis Rongwei Xu, Qiangsheng Wang, Zhaomin Xiao, Zhenzhong Anand, Asundi School of Mechanical and Aerospace Engineering DRNTU::Engineering::Mechanical engineering Reflection configured digital holographic microscopy (DHM) can perform accurate optical topography measurements of reflecting objects, such as MEMs, MOEMs, and semiconductor wafer. It can provide non-destructive quantitative measurements of surface roughness and geometric pattern characterization with nanometric axial resolution in real-time. However, the measurement results may be affected by an additional phase curvature introduced by the microscope objective (MO) used in DHM. It needs to be removed either by numerical compensation or by physical compensation. We present a method of physical spherical phase compensation for reflection DHM in the Michelson configuration. In the object arm, collimated light is used for illumination. Due to the use of the MO, the object wavefront may have a spherical phase curvature. In the reference arm, a lens and mirror combination is used to generate a spherical recording reference wave in order to physically compensate the spherical phase curvature of the object wavefront. By controlling the position of the mirror and the sample stage, the compensation process has been demonstrated. The relative positions of the test specimen and the reference mirror must be fixed for the physical spherical phase to be totally compensated. A numerical plane reference wave is preferred for the numerical reconstruction of the phase introduced by the test specimen. Experimental results on wafer pattern recognition are also given. 2013-09-24T06:38:50Z 2019-12-06T20:09:30Z 2013-09-24T06:38:50Z 2019-12-06T20:09:30Z 2011 2011 Journal Article Qu, W., Chee, O. C., Tan, L. R., Xu, Q., Wang, Z., Xiao, Z., & Anand, A. (2011). Physical spherical phase compensation in reflection digital holographic microscopy. Optics and lasers in engineering, 50(4), 563-567. https://hdl.handle.net/10356/99611 http://hdl.handle.net/10220/13639 10.1016/j.optlaseng.2011.06.010 en Optics and lasers in engineering
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic DRNTU::Engineering::Mechanical engineering
spellingShingle DRNTU::Engineering::Mechanical engineering
Qu, Weijuan
Chee, Oi Choo
Tan, Lewis Rongwei
Xu, Qiangsheng
Wang, Zhaomin
Xiao, Zhenzhong
Anand, Asundi
Physical spherical phase compensation in reflection digital holographic microscopy
description Reflection configured digital holographic microscopy (DHM) can perform accurate optical topography measurements of reflecting objects, such as MEMs, MOEMs, and semiconductor wafer. It can provide non-destructive quantitative measurements of surface roughness and geometric pattern characterization with nanometric axial resolution in real-time. However, the measurement results may be affected by an additional phase curvature introduced by the microscope objective (MO) used in DHM. It needs to be removed either by numerical compensation or by physical compensation. We present a method of physical spherical phase compensation for reflection DHM in the Michelson configuration. In the object arm, collimated light is used for illumination. Due to the use of the MO, the object wavefront may have a spherical phase curvature. In the reference arm, a lens and mirror combination is used to generate a spherical recording reference wave in order to physically compensate the spherical phase curvature of the object wavefront. By controlling the position of the mirror and the sample stage, the compensation process has been demonstrated. The relative positions of the test specimen and the reference mirror must be fixed for the physical spherical phase to be totally compensated. A numerical plane reference wave is preferred for the numerical reconstruction of the phase introduced by the test specimen. Experimental results on wafer pattern recognition are also given.
author2 School of Mechanical and Aerospace Engineering
author_facet School of Mechanical and Aerospace Engineering
Qu, Weijuan
Chee, Oi Choo
Tan, Lewis Rongwei
Xu, Qiangsheng
Wang, Zhaomin
Xiao, Zhenzhong
Anand, Asundi
format Article
author Qu, Weijuan
Chee, Oi Choo
Tan, Lewis Rongwei
Xu, Qiangsheng
Wang, Zhaomin
Xiao, Zhenzhong
Anand, Asundi
author_sort Qu, Weijuan
title Physical spherical phase compensation in reflection digital holographic microscopy
title_short Physical spherical phase compensation in reflection digital holographic microscopy
title_full Physical spherical phase compensation in reflection digital holographic microscopy
title_fullStr Physical spherical phase compensation in reflection digital holographic microscopy
title_full_unstemmed Physical spherical phase compensation in reflection digital holographic microscopy
title_sort physical spherical phase compensation in reflection digital holographic microscopy
publishDate 2013
url https://hdl.handle.net/10356/99611
http://hdl.handle.net/10220/13639
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