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The first-order quantity of the optical structure can be obtained using the ybar-y diagram and this diagram has a control point quantity. Based on the concept and quantity of the ybar-y diagram, this paper establishes a mathematical model to calculate an optical system’s first-order structure. The aberration is induced by the deflection of the transmission rays. If a first-order structure has a minimal total deflection angle of the first paraxial ray and the second paraxial ray, the higher order aberration will have a small value and the calculated first-order optical structure will be the best. According to the mathematical model, the issue of optical structure calculation is converted to a numerical optimization problem. And the objective function, i.e. the sum of the first and second paraxial ray’s deflection angles, is constructed. After comparison among etween many kinds of numerical optimization algorithms, the particle swarm optimization algorithm is used to solve the problem. Then a calculation program containing graphical user interface (GUI) is developed to calculate the first-order structure quickly and efficiently. The basic design parameters of the optical system are imported into the GUI after some treatments, then the resulting first-order structure is obtained after some clicks of the mouse. The resulting structure is thereafter converted to a practical lens system by the use of commercially available optical design software such as ZEMAX. After a lens optimization process, an actual optical system is accomplished. According to the method proposed in this paper and by the use of the calculation program, a 13 megapixel mobile phone camera lens is designed first. The F# of this lens system is 2.3 and the full field of viewing angle is 70 degree. The system has a total length of 4.5 mm and a distortion of 1.2%. Only four aspheric lenses are used and the other optical performance meets the design requirements as well. In addition, an eyepiece of helmet-mounted display system is designed, in which only two lenses are used and a visual field angle of 90 degree is achieved. The entrance pupil is 5 mm width and the image diagonal length is 65 mm. This system has a total length less than 45 mm and eye relief greater than 12 mm. Other performance of the eyepiece can also meet the requirements. These designs of the two optical systems demonstrate that the proposed method is reliable in calculating the optical structure of the optical system.
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Keywords:
- optical design /
- first-order optical structure /
- mobile phone lens design /
- helmet-mounted display
[1] Zeng F, Zhang X, Zhang J P, Shi G W, Qu H M, Zhang J Z 2013 Acta Optica Sinica 33 0909001 (in Chinese) [曾飞, 张新, 张建萍, 史广维, 曲贺盟, 张继真 2013光学学报 33 0909001]
[2] Zhang H J 2005 Chinese Journal of Lasers 32 856 (in Chinese) [张慧娟 2005中国激光 32 856]
[3] Li G, Wang J Y, Zhang Y 2011 Appl. Opt. 32 420 (in Chinese) [李广, 汪建业, 张燕 2011 应用光学 32 420]
[4] Zhang Y M 2008 Applied optics 3rd ed (Beijing:Publishing House of Electronics Industry) pp602-658 (in Chinese) [张以谟 2008 应用光学第3版 (北京:电子工业出版社) 第602-658页]
[5] Delano E 1963 Appl. Opt. 2 1251
[6] Pegis R J, Vogl T P, Rigler A K, Walters R 1967 Appl. Opt. 6 969
[7] López-López F J 1970 Appl. Opt. 9 2485
[8] Zhuang S L, Zheng Q, Yu F T S 1982 Opt. Lett. 7 581
[9] Harrigan M E, Loce R P, Rogers J 1988 Appl. Opt. 27 459
[10] Kessler D, Shack R V 1992 Appl. Opt. 31 2692
[11] Wang Z J 2006 Handbook of practical optical technology (Beijing:China Machine Press) pp278-317 (in Chinese) [王之江 2006 实用光学技术手册 (北京:机械工业出版社) 第278-317页]
[12] Nocedal J, Wright S J 2000 Numerical optimization (New York:Springer) pp1-10
[13] Li S Y, Du Z H, Wu M Y, Zhu J, Li S L 2001 Acta Phys. Sin. 50 1260 (in Chinese) [李树有, 都志辉, 吴梦月, 朱静, 李三立 2001 50 1260]
[14] Zhang J J, Ji Y, Yao D C, Chen J B 1996 Acta Phys. Sin. 45 789 (in Chinese) [张静娟, 姬扬, 姚德成, 陈俊本 1996 45 789]
[15] Eberhart R C, Shi Y 2001 Proceedings of Evolutionary Computation Seoul May 27-30, 2001 p81
[16] Meiron J 1965 J. Opt. Soc. Am. 55 1105
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[1] Zeng F, Zhang X, Zhang J P, Shi G W, Qu H M, Zhang J Z 2013 Acta Optica Sinica 33 0909001 (in Chinese) [曾飞, 张新, 张建萍, 史广维, 曲贺盟, 张继真 2013光学学报 33 0909001]
[2] Zhang H J 2005 Chinese Journal of Lasers 32 856 (in Chinese) [张慧娟 2005中国激光 32 856]
[3] Li G, Wang J Y, Zhang Y 2011 Appl. Opt. 32 420 (in Chinese) [李广, 汪建业, 张燕 2011 应用光学 32 420]
[4] Zhang Y M 2008 Applied optics 3rd ed (Beijing:Publishing House of Electronics Industry) pp602-658 (in Chinese) [张以谟 2008 应用光学第3版 (北京:电子工业出版社) 第602-658页]
[5] Delano E 1963 Appl. Opt. 2 1251
[6] Pegis R J, Vogl T P, Rigler A K, Walters R 1967 Appl. Opt. 6 969
[7] López-López F J 1970 Appl. Opt. 9 2485
[8] Zhuang S L, Zheng Q, Yu F T S 1982 Opt. Lett. 7 581
[9] Harrigan M E, Loce R P, Rogers J 1988 Appl. Opt. 27 459
[10] Kessler D, Shack R V 1992 Appl. Opt. 31 2692
[11] Wang Z J 2006 Handbook of practical optical technology (Beijing:China Machine Press) pp278-317 (in Chinese) [王之江 2006 实用光学技术手册 (北京:机械工业出版社) 第278-317页]
[12] Nocedal J, Wright S J 2000 Numerical optimization (New York:Springer) pp1-10
[13] Li S Y, Du Z H, Wu M Y, Zhu J, Li S L 2001 Acta Phys. Sin. 50 1260 (in Chinese) [李树有, 都志辉, 吴梦月, 朱静, 李三立 2001 50 1260]
[14] Zhang J J, Ji Y, Yao D C, Chen J B 1996 Acta Phys. Sin. 45 789 (in Chinese) [张静娟, 姬扬, 姚德成, 陈俊本 1996 45 789]
[15] Eberhart R C, Shi Y 2001 Proceedings of Evolutionary Computation Seoul May 27-30, 2001 p81
[16] Meiron J 1965 J. Opt. Soc. Am. 55 1105
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