Phase feedback fringe projection profilometry for shiny objects
Contiene ilustraciones
- Autores:
-
Juarez-Salazar, Rigoberto
Vega, Fabio
Esquivel-Hernandez, Sofia
Diaz-Ramirez, Victor H.
Marrugo Hernández, Andrés Guillermo
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2025
- Institución:
- Universidad Tecnológica de Bolívar
- Repositorio:
- Repositorio Institucional UTB
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.utb.edu.co:20.500.12585/13307
- Acceso en línea:
- https://hdl.handle.net/20.500.12585/13307
- Palabra clave:
- Shiny objects
Saturation
Phase feedback
High dynamic range
Multi-frequency fringe projection
- Rights
- closedAccess
- License
- https://creativecommons.org/licenses/by-nc-sa/4.0/
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Phase feedback fringe projection profilometry for shiny objects |
| title |
Phase feedback fringe projection profilometry for shiny objects |
| spellingShingle |
Phase feedback fringe projection profilometry for shiny objects Shiny objects Saturation Phase feedback High dynamic range Multi-frequency fringe projection |
| title_short |
Phase feedback fringe projection profilometry for shiny objects |
| title_full |
Phase feedback fringe projection profilometry for shiny objects |
| title_fullStr |
Phase feedback fringe projection profilometry for shiny objects |
| title_full_unstemmed |
Phase feedback fringe projection profilometry for shiny objects |
| title_sort |
Phase feedback fringe projection profilometry for shiny objects |
| dc.creator.fl_str_mv |
Juarez-Salazar, Rigoberto Vega, Fabio Esquivel-Hernandez, Sofia Diaz-Ramirez, Victor H. Marrugo Hernández, Andrés Guillermo |
| dc.contributor.author.none.fl_str_mv |
Juarez-Salazar, Rigoberto Vega, Fabio Esquivel-Hernandez, Sofia Diaz-Ramirez, Victor H. Marrugo Hernández, Andrés Guillermo |
| dc.subject.proposal.none.fl_str_mv |
Shiny objects Saturation Phase feedback High dynamic range Multi-frequency fringe projection |
| topic |
Shiny objects Saturation Phase feedback High dynamic range Multi-frequency fringe projection |
| description |
Contiene ilustraciones |
| publishDate |
2025 |
| dc.date.accessioned.none.fl_str_mv |
2025-04-28T16:33:56Z |
| dc.date.issued.none.fl_str_mv |
2025-04-22 |
| dc.date.available.none.fl_str_mv |
2027 |
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Artículo de revista |
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info:eu-repo/semantics/article |
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Juarez-Salazar, R., Vega, F., Esquivel-Hernandez, S., Diaz-Ramirez, V. H., & Marrugo, A. G. (2025). Phase feedback fringe projection profilometry for shiny objects. Optics and Lasers in Engineering, 15 páginas. |
| dc.identifier.issn.none.fl_str_mv |
01438166 |
| dc.identifier.uri.none.fl_str_mv |
https://hdl.handle.net/20.500.12585/13307 |
| dc.identifier.doi.none.fl_str_mv |
10.1016/j.optlaseng.2025.109013 |
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Repositorio UTB |
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Repositorio UTB |
| dc.identifier.repourl.none.fl_str_mv |
Repositorio UTB |
| identifier_str_mv |
Juarez-Salazar, R., Vega, F., Esquivel-Hernandez, S., Diaz-Ramirez, V. H., & Marrugo, A. G. (2025). Phase feedback fringe projection profilometry for shiny objects. Optics and Lasers in Engineering, 15 páginas. 01438166 10.1016/j.optlaseng.2025.109013 Repositorio UTB |
| url |
https://hdl.handle.net/20.500.12585/13307 |
| dc.language.iso.none.fl_str_mv |
eng |
| language |
eng |
| dc.relation.references.none.fl_str_mv |
C. Jiang, Y. Li, S. Feng, Y. Hu, W. Yin, J. Qian, C. Zuo, J. Liang, Fringe Projection Profilometry, Springer International Publish ing, Cham, 2024, Ch. 14, pp. 241–286. A. G. Marrugo, F. Gao, S. Zhang, State-of-the-art active optical techniques for three-dimensional surface metrology: a review [Invited], J. Opt. Soc. Am. A 37 (9) (2020) B60–B77 J. Geng, Structured-light 3d surface imaging: a tutorial, Adv. Opt. Photon. 3 (2) (2011) 128–160. S. S. Gorthi, P. Rastogi, Fringe projection techniques: Whither we are?, Optics and Lasers in Engineering 48 (2) (2010) 133– 140. E. B. Li, X. Peng, J. Xi, J. F. Chicharo, J. Q. Yao, D. W. Zhang, Multi-frequency and multiple phase-shift sinusoidal fringe projection for 3d profilometry, Opt. Express 13 (5) (2005) 1561– 1569 K. Creath, J. Schmit, J. C. Wyant, Optical shop testing, 3rd Edition, John Wiley & Sons, Inc., 2007, Ch. Optical metrology of diffuse surfaces, pp. 756–807. S. Lei, S. Zhang, Flexible 3-d shape measurement using projec tor defocusing, Opt. Lett. 34 (20) (2009) 3080–3082 S. Heist, P. Lutzke, I. Schmidt, P. Dietrich, P. Kuhmstedt, ¨ A. Tunnermann, G. Notni, High-speed three-dimensional shape ¨ measurement using gobo projection, Optics and Lasers in Engineering 87 (2016) 90–96. S. Zhang, Recent progresses on real-time 3D shape measurement using digital fringe projection techniques, Optics and Lasers in Engineering 48 (2) (2010) 149–158 Z. J. Geng, Rainbow three-dimensional camera: new concept of high-speed three-dimensional vision systems, Optical Engineering 35 (2) (1996) 376–383. G. Xiang, H. Zhu, H. Guo, Spatial phase-shifting profilometry by use of polarization for measuring 3d shapes of metal objects, Opt. Express 29 (13) (2021) 20981–20994 X. Su, W. Chen, Fourier transform profilometry: a review, Optics and Lasers in Engineering 35 (5) (2001) 263–284. C. Zuo, S. Feng, L. Huang, T. Tao, W. Yin, Q. 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Unsalan, Single stripe projection based range scanning of shiny objects under ambient light, in: 24th International Symposium on Computer and Information Sciences, 2009, pp. 1–6. S. Chen, Intraoral 3-d measurement by means of group coding combined with consistent enhancement for fringe projection pattern, IEEE Transactions on Instrumentation and Mea surement 71 (2022) 1–12. H. Lin, J. Gao, G. Zhang, X. Chen, Y. He, Y. Liu, Review and comparison of high-dynamic range three-dimensional shape measurement techniques, Journal of Sensors 2017 (1) (2017) 9576850. G. hua Liu, X.-Y. Liu, Q.-Y. Feng, 3d shape measurement of objects with high dynamic range of surface reflectivity, Appl. Opt. 50 (23) (2011) 4557–4565 H. Zhu, H. Guo, Surface profile measurement of metal objects by use of a fringe projection system with polarized dual projectors, Appl. Opt. 63 (30) (2024) 7883–7892 S. Zhang, S.-T. Yau, High dynamic range scanning technique, Optical Engineering 48 (3) (2009) 033604. H. Jiang, H. Zhao, X. Li, High dynamic range fringe acquisition: A novel 3-d scanning technique for high-reflective surfaces, Optics and Lasers in Engineering 50 (10) (2012) 1484–1493. S. Feng, Y. Zhang, Q. Chen, C. Zuo, R. Li, G. Shen, General solution for high dynamic range three-dimensional shape measurement using the fringe projection technique, Optics and Lasers in Engineering 59 (2014) 56–71. J. Jeong, M. Y. Kim, Adaptive imaging system with spatial light modulator for robust shape measurement of partially specular objects, Opt. Express 18 (26) (2010) 27787–27801. S. Ri, M. Fujigaki, Y. Morimoto, Intensity range extension method for three-dimensional shape measurement in phasemeasuring profilometry using a digital micromirror device camera, Appl. Opt. 47 (29) (2008) 5400–5407 B. Salahieh, Z. Chen, J. J. Rodriguez, R. Liang, Multipolarization fringe projection imaging for high dynamic range objects, Opt. Express 22 (8) (2014) 10064–10071. X. Huang, J. Bai, K. Wang, Q. Liu, Y. Luo, K. Yang, X. Zhang, Target enhanced 3d reconstruction based on polarization-coded structured light, Opt. Express 25 (2) (2017) 1173–1184. Z. Zhu, Y. Dong, D. You, X. Sun, Accurate three-dimensional measurement based on polarization-defocused encoded structured light, Measurement 205 (2022) 112128. S. Zhang, Rapid and automatic optimal exposure control for digital fringe projection technique, Optics and Lasers in Engineering 128 (2020) 106029. Z. Song, H. Jiang, H. Lin, S. Tang, A high dynamic range structured light means for the 3d measurement of specular surface, Optics and Lasers in Engineering 95 (2017) 8–16. S. Feng, L. Zhang, C. Zuo, T. Tao, Q. Chen, G. Gu, High dynamic range 3d measurements with fringe projection profilometry: a review, Measurement Science and Technology 29 (12) (2018) 122001. M. Wang, G. Du, C. Zhou, C. Zhang, S. Si, H. Li, Z. Lei, Y. Li, Enhanced high dynamic range 3d shape measurement based on generalized phase-shifting algorithm, Optics Communications 385 (2017) 43–53. C. Waddington, J. Kofman, Analysis of measurement sensitivity to illuminance and fringe-pattern gray levels for fringe-pattern projection adaptive to ambient lighting, Optics and Lasers in Engineering 48 (2) (2010) 251–256 D. Li, J. Kofman, Adaptive fringe-pattern projection for image saturation avoidance in 3d surface-shape measurement, Opt. Express 22 (8) (2014) 9887–9901. F. Vega, A. G. Marrugo, Intelligent exposure time determination with structured light for accurate 3d object reconstruction, in: IEEE Colombian Caribbean Conference, 2023, pp. 1–5. E. Hu, Y. He, Y. Chen, Study on a novel phase-recovering algorithm for partial intensity saturation in digital projection grating phase-shifting profilometry, Optik 121 (1) (2010) 23–28 B. Chen, S. Zhang, High-quality 3d shape measurement using saturated fringe patterns, Optics and Lasers in Engineering 87 (2016) 83–89 H. Li, H. Wei, J. Liu, G. Deng, S. Zhou, W. Wang, L. He, P. 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Zuo, Robust and efficient multi-frequency temporal phase unwrapping: optimal fringe frequency and pattern sequence selection, Opt. Express 25 (17) (2017) 20381–20400. Y. Hu, Q. Chen, Y. Liang, S. Feng, T. Tao, C. Zuo, Microscopic 3d measurement of shiny surfaces based on a multi-frequency phase-shifting scheme, Optics and Lasers in Engineering 122 (2019) 1–7. J. H. Bruning, D. R. Herriott, J. E. Gallagher, D. P. Rosenfeld, A. D. White, D. J. Brangaccio, Digital wavefront measuring interferometer for testing optical surfaces and lenses, Appl. Opt. 13 (11) (1974) 2693–2703 R. Juarez-Salazar, C. Mendoza-Rodriguez, J. E. Hernandez Beltran, C. Robledo-Sanchez, How do phase-shifting algorithms work?, European Journal of Physics 39 (6) (2018) 065302. R. Vargas, L. A. Romero, S. Zhang, A. G. Marrugo, Calibration method based on virtual phase-to-coordinate mapping with linear correction function for structured light system, Optics and Lasers in Engineering 183 (2024) 108496. R. Juarez-Salazar, S. Esquivel-Hernandez, V. H. Diaz-Ramirez, Are camera, projector, and camera–projector calibrations different?, Applied Optics 62 (22) (2023) 5999–6006 S. Feng, C. Zuo, L. Zhang, T. Tao, Y. Hu, W. Yin, J. Qian, Q. Chen, Calibration of fringe projection profilometry: A comparative review, Optics and Lasers in Engineering 143 (2021) 106622 R. Juarez-Salazar, J. Zheng, V. H. Diaz-Ramirez, Distorted pinhole camera modeling and calibration, Applied Optics 59 (36) (2020) 11310–11318. R. Juarez-Salazar, V. H. Diaz-Ramirez, Operator-based homo geneous coordinates: application in camera document scanning, Optical Engineering 56 (7) (2017) 070801. R. Juarez-Salazar, G. A. Rodriguez-Reveles, S. Esquivel Hernandez, V. H. Diaz-Ramirez, Three-dimensional spatial point computation in fringe projection profilometry, Optics and Lasers in Engineering 164 (2023) 107482. Y. Long, S. Wang, W. Wu, K. Liu, Accurate identification of saturated pixels for high dynamic range measurement, Optical Engineering 54 (4) (2015) 043106. K. Zhong, Z. Li, X. Zhou, Y. Li, Y. Shi, C. Wang, Enhanced phase measurement profilometry for industrial 3d inspection automation, The International Journal of Advanced Manufacturing Technology 76 (9) (2015) 1563–1574. I. Amidror, Scattered data interpolation methods for electronic imaging systems: a survey, Journal of Electronic Imaging 11 (2) (2002) 157 – 176 K. S. Surana, Numerical methods and methods of approximation in sciencie and engineering, CRC Press Taylor & Francis Group, Boca Raton, 2019. R. Juarez-Salazar, V. H. Diaz-Ramirez, Flexible camera projector calibration using superposed color checkerboards, Optics and Lasers in Engineering 120 (2019) 59–65 P. Xu, J. Liu, J. Wang, High dynamic range 3d measurement technique based on adaptive fringe projection and curve fitting, Appl. Opt. 62 (13) (2023) 3265–3274. |
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Juarez-Salazar, RigobertoVega, FabioEsquivel-Hernandez, SofiaDiaz-Ramirez, Victor H.Marrugo Hernández, Andrés Guillermovirtual::812-12025-04-28T16:33:56Z20272025-04-22Juarez-Salazar, R., Vega, F., Esquivel-Hernandez, S., Diaz-Ramirez, V. H., & Marrugo, A. G. (2025). Phase feedback fringe projection profilometry for shiny objects. Optics and Lasers in Engineering, 15 páginas.01438166https://hdl.handle.net/20.500.12585/1330710.1016/j.optlaseng.2025.109013Repositorio UTBRepositorio UTBRepositorio UTBContiene ilustracionesDiffuse objects have suitable optical properties for accurate three-dimensional reconstruction by fringe projection profilometry. In contrast, shiny objects, such as glossy plastic items and metallic workpieces, are difficult to reconstruct due to image saturation. In this paper, the recursive structure of the hierarchical multi-frequency fringe projection profilometry is exploited to prevent saturation by a feedback loop. Novel functions for saturation, low-modulation, and grating intensity correction, suited to adjust the projector pixels inducing saturation, are proposed. The usefulness of the proposal is verified experimentally, confirming the high performance of the proposed phase feedback approach for the reconstruction of shiny objects.15 páginasapplication/pdfengUniversidad Tecnológica de Bolívarhttps://creativecommons.org/licenses/by-nc-sa/4.0/info:eu-repo/semantics/closedAccessAtribución-NoComercial-CompartirIgual 4.0 Internacional (CC BY-NC-SA 4.0)http://purl.org/coar/access_right/c_14cbOptics and Lasers in EngineeringPhase feedback fringe projection profilometry for shiny objectsArtículo de revistainfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1http://purl.org/redcol/resource_type/ARTTextinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85C. Jiang, Y. Li, S. Feng, Y. Hu, W. Yin, J. Qian, C. Zuo, J. Liang, Fringe Projection Profilometry, Springer International Publish ing, Cham, 2024, Ch. 14, pp. 241–286.A. G. Marrugo, F. Gao, S. Zhang, State-of-the-art active optical techniques for three-dimensional surface metrology: a review [Invited], J. Opt. Soc. Am. A 37 (9) (2020) B60–B77J. Geng, Structured-light 3d surface imaging: a tutorial, Adv. Opt. Photon. 3 (2) (2011) 128–160.S. S. Gorthi, P. Rastogi, Fringe projection techniques: Whither we are?, Optics and Lasers in Engineering 48 (2) (2010) 133– 140.E. B. Li, X. Peng, J. Xi, J. F. Chicharo, J. Q. Yao, D. W. Zhang, Multi-frequency and multiple phase-shift sinusoidal fringe projection for 3d profilometry, Opt. Express 13 (5) (2005) 1561– 1569K. Creath, J. Schmit, J. C. Wyant, Optical shop testing, 3rd Edition, John Wiley & Sons, Inc., 2007, Ch. Optical metrology of diffuse surfaces, pp. 756–807.S. Lei, S. Zhang, Flexible 3-d shape measurement using projec tor defocusing, Opt. Lett. 34 (20) (2009) 3080–3082S. Heist, P. Lutzke, I. 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Opt. 62 (13) (2023) 3265–3274.Optics and Lasers in Engineering191115109013Shiny objectsSaturationPhase feedbackHigh dynamic rangeMulti-frequency fringe projectionPublication651b0410-2e8f-4894-87bc-d3d803c92eabvirtual::812-1651b0410-2e8f-4894-87bc-d3d803c92eabvirtual::812-1LICENSElicense.txtlicense.txttext/plain; charset=utf-814837https://repositorio.utb.edu.co/bitstreams/a7c94963-09c5-4b0f-b866-f8a9776c3968/downloadb76e7a76e24cf2f94b3ce0ae5ed275d0MD51falseAnonymousREADORIGINALRJuarez_manuscript.pdfRJuarez_manuscript.pdfapplication/pdf3629253https://repositorio.utb.edu.co/bitstreams/4dd7958c-6f6c-450d-b8a8-e68ae018f1f6/download2786c4cbe368d8f6b466fdc4552294abMD52trueAnonymousREADTEXTRJuarez_manuscript.pdf.txtRJuarez_manuscript.pdf.txtExtracted texttext/plain55486https://repositorio.utb.edu.co/bitstreams/3c2f6ada-6de4-485f-a473-1e5d1a8921fa/download56d7cacbadc04d3456066c804262be3dMD53falseAnonymousREADTHUMBNAILRJuarez_manuscript.pdf.jpgRJuarez_manuscript.pdf.jpgGenerated 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