-
摘要:
冷反射现象是指在红外热成像系统中制冷探测器通过前面光学表面的反射而探测到的自身的像，冷反射的控制是红外成像系统的重要任务。本文设计了一款采用Cassegrain(卡塞格林)反射结构的制冷型中波红外成像系统，分析了该系统的冷反射现象，得到了冷反射现象严重的表面。接着，通过Zemax软件降低这些严重面的冷发射，在控制冷反射的同时兼顾系统传递函数MTF的优化。通过NARCISSUS宏命令（冷反射分析宏命令）、Tracepro建模软件和实际成像图将优化后的中波红外成像系统与冷反射抑制前的系统进行比对。结果显示：探测器像面冷反射引入的等效温差( NITD)由1.0484 K下降到了0.1576 K，同时系统在调焦过程中冷反射斑的能量和尺寸无明显变化，优化后的光学结构有效地控制了系统的冷反射。
-
关键词:
- 冷反射 /
- 制冷型中波红外成像系统 /
- 冷反射引入等效温差
Abstract:Narcissus refers to the phenomenon in an infrared system where a cooled imaging sensor can “see” its own reflected image by the reflection of the frontal optical surfaces. Control of narcissus is one of the important requirements in the design of the infrared imaging system. A cooled medium-wave infrared imaging system with Cassegrain reflection structure is designed and analyzed to obtain the optical surfaces with serious narcissus. In addition, the narcissus is reduced by Zemax, and the optimization of the system transfer function MTF is taken into account while the narcissus is controlled. The optimized medium-wave infrared imaging system is compared with the imaging system without narcissus suppression through NARCISSUS macro (narcissus analysis macro), Tracepro modeling software and actual imaging, and it was found that the narcissus induced equivalent temperature difference (NITD) of the detector image surface decrease from 1.0484 K to 0.1576 K. The energy and size of the narcissus spot did not show marked change during the focusing of the system. The optimized optical structure can effectively control the narcissus of the system.
-
图 1 冷反射抑制前折反式中波红外成像系统结构图
Figure 1. Structural diagram of a catadioptric medium-wave infrared imaging system without narcissus suppression
图 2 冷反射抑制前折反式中波红外成像系统的传递函数
Figure 2. MTF of a catadioptric medium-wave infrared imaging system without narcissus suppression
图 3 冷反射抑制前折反式中波红外成像系统倒置结构图
Figure 3. Inverted structure diagram of a catadioptric medium-wave infrared imaging system without narcissus suppression
图 5 探测器像面冷斑在调焦前后的变化
Figure 5. Changes of the narcissus spot in the detector image surface before and after focusing
图 6 中红外成像系统各透镜表面的NITD贡献
Figure 6. NITD of each lens surface of the medium-wave infrared imaging system
图 8 优化后的中波红外系统光学透射结构图
Figure 8. Transmission structure diagram of the optimized medium-wave infrared imaging system
图 9 优化后的折反式中波红外成像系统的传递函数
Figure 9. MTF of the optimized catadioptric medium-wave infrared imaging system
图 10 成像系统优化前后的主要差异
Figure 10. Main differences of the imaging system before and after optimization
图 11 优化后的中波红外成像系统各透镜表面的NITD
Figure 11. NITD of each lens surface of the optimized medium-wave infrared imaging system
图 12 冷反射抑制后探测器像面冷反射斑在调焦前后的变化
Figure 12. Changes of the narcissus spot in the detector image surface of the optimized system before and after focusing
图 13 Tracepro仿真探测器靶面的冷反射能量模拟结果
Figure 13. Simulation results of narcissus on the image surface through Tracepro modeling software
图 14 红外系统优化前后成像图
Figure 14. Images of the infrared system before and after optimization
表 1 不同靶标对应的MRTD值
Table 1. MRTD values for different targets
Target frequency (cy/mrad) MRTD (K) 2.5 0.035 4.01 0.055 10.77 0.103 
下载: 导出CSV
表 2 冷反射严重面的YNI和I/IBAR值
Table 2. YNI and I/IBAR values for the optical surfaces with serious narcissus
Surface S2 S3 S5 S14 S15 S18 YNI 0.367 0.371 0.454 −0.091 −0.091 −0.298 I/IBAR 0.420 0.424 0.378 0.106 0.106 0.512
下载: 导出CSV
表 3 面S5的I/IBAR值的优化函数
Table 3. Merit function of I/IBAR values with surface S5
OPER# type surf wave Hx Hy Px Py Target Weight Value 1 RAED 5 2 0 0 0 1 0 0 1.08 2 RAED 5 2 0 1 0 0 0 0 2.86 3 DIVI 1 2 0 — — — 0 0 0.378 4 ABSO 3 — — — — — 0 0 0.378 5 OPGT 4 — — — — — 1 1 0.378
下载: 导出CSV
表 4 冷反射严重面在优化后系统中的YNI和I/IBAR值
Table 4. YNI and I/IBAR values of the surfaces with serious narcissus in optimized system
Surface S5 S18 YNI −0.52 0.74 I/IBAR 1.46 1.93
下载: 导出CSV
表 5 优化前后的NITD值
Table 5. NITD values before and after optimization
(K) Structural state Max Min ΔNITD Non-optimization 1.0484 0.8634 0.1850 Optimization 0.1576 0.1557 0.0019
下载: 导出CSV
表 6 调焦过程中探测器像面冷反射仿真结果
Table 6. Simulation results of narcissus on the detector’s image surface during focusing
Structural state Maximum-intensity（W/m2） Average-intensity（W/m2） Total-luminous-flux（W） Theoretical design location 6.95×10−4 4.48×10−4 2.96×10−6 The focus group moves by +2 mm 6.97×10−4 4.49×10−4 2.97×10−6 The focus group moves by -2 mm 6.97×10−4 4.48×10−4 2.96×10−6
下载: 导出CSV
-
[1] 杨正, 屈恩世, 曹剑中, 等. 对凝视红外热成像冷反射现象的研究[J]. 与红外,2008,38(1):35-38.YANG ZH, QU E SH, CAO J ZH, et al. The narcissus study in the optical system for the infrared staring arrays[J]. Laser &Infrared, 2008, 38(1): 35-38. (in Chinese) [2] 任国栋, 张良, 兰卫华, 等. 红外成像系统冷反射的定量分析[J]. 红外技术,2016,38(4):290-295.REN G D, ZHANG L, LAN W H, et al. Quantitative analysis of the narcissus of infrared imaging system[J]. Infrared Technology, 2016, 38(4): 290-295. (in Chinese) [3] 王文芳, 杨晓许, 姜凯, 等. 大视场红外折反光学系统杂散光分析[J]. 红外与 工程,2013,42(1):138-142.WANG W F, YANG X X, JIANG K, et al. Stray light analysis of catadioptric infrared optical system with large field[J]. Infrared and Laser Engineering, 2013, 42(1): 138-142. (in Chinese) [4] 刘鑫, 黄一帆, 李林, 等. 多谱段相机红外光学系统杂散辐射分析[J]. 红外与 工程,2013,42(12):3201-3206.LIU X, HUANG Y F, LI L, et al. Stray radiation analysis of infrared optical system in multispectral camera[J]. Infrared and Laser Engineering, 2013, 42(12): 3201-3206. (in Chinese) [5] 张葆, 洪永丰, 史光辉. 非均匀性校正在红外杂散辐射抑制中的应用[J]. 光学 精密工程,2008,16(12):2421-2428.ZHANG B, HONG Y F, SHI G H. Application of non-uniformity correction to stray radiation suppression of infrared optical system[J]. Optics and Precision Engineering, 2008, 16(12): 2421-2428. (in Chinese) [6] 陈锐, 谈新权. 红外图像非均匀性校正方法综述[J]. 红外技术,2002,24(1):1-3.CHEN R, TAN X Q. Study on non-uniformity correction of infrared image[J]. Infrared Technology, 2002, 24(1): 1-3. (in Chinese) [7] 代少升, 袁祥辉. 红外图像非均匀性实时校正的新技术[J]. 光学 精密工程,2004,12(2):201-204.DAI SH SH, YUAN X H. Real-time correction of infrared image nonuniformity[J]. Optics and Precision Engineering, 2004, 12(2): 201-204. (in Chinese) [8] 陈迎娟, 张之江, 张智强. CCD像素响应不均匀性的校正方法[J]. 光学 精密工程,2004,12(2):216-220.CHEN Y J, ZHANG ZH J, ZHANG ZH Q. Correction of CCD pixel nonuniformity[J]. Optics and Precision Engineering, 2004, 12(2): 216-220. (in Chinese) [9] 刘欣, 潘枝峰. 红外光学系统冷反射分析和定量计算方法[J]. 红外与 工程,2012,41(7):1684-1688.LIU X, PAN ZH F. Analysis and quantitative calculating methods for narcissus of infrared optical system[J]. Infrared and Laser Engineering, 2012, 41(7): 1684-1688. (in Chinese) [10] 栾亚东. 红外扫描成像系统中冷反射的光学抑制[J]. 红外与 工程,2006,35(S2):26-30.LUAN Y D. Optical method of restraining narcissus in scanning infrared system[J]. Infrared and Laser Engineering, 2006, 35(S2): 26-30. (in Chinese) [11] 牛金星, 周仁魁, 刘朝晖, 等. 红外探测系统自身热辐射杂散光的分析[J]. 光学学报,2010,30(8):2267-2271. doi: 10.3788/AOS20103008.2267NIU J X, ZHOU R K, LIU ZH H, et al. Analysis of stray light caused by thermal radiation of infrared detection system[J]. Acta Optica Sinica, 2010, 30(8): 2267-2271. (in Chinese) doi: 10.3788/AOS20103008.2267 [12] 姚秀文, 肖静, 曾曙光, 等. 红外光学系统自身杂散辐射分析及抑制[J]. 与光电子学进展,2009,46(12):91-94.YAO X W, XIAO J, ZENG SH G, et al. Analysis and suppression of self-generated thermal emission in infrared optical systems[J]. Laser &Optoelectronics Progress, 2009, 46(12): 91-94. (in Chinese) [13] 孙文芳. 基于MRTD的红外成像系统性能评估和大气影响的研究[D]. 南京: 南京航空航天大学, 2015.SUN W F. Research of performance evaluation of infrared imaging system and atmospheric effects based on MRTD[D]. Nanjing: Nanjing University of Aeronautics and Astronautics, 2015. (in Chinese) [14] 梁子健, 杨甬英, 赵宏洋, 等. 非球面光学元件面型检测技术研究进展与最新应用[J]. 中国光学,2022,15(2):161-186. doi: 10.37188/CO.2021-0143LIANG Z J, YANG Y Y, ZHAO H Y, et al. Advances in research and applications of optical aspheric surface metrology[J]. Chinese Optics, 2022, 15(2): 161-186. (in Chinese) doi: 10.37188/CO.2021-0143 [15] 袁方, 谭庆贵, 王光耀, 等. 基于液晶偏振光栅的快速大角度光束偏转[J]. 液晶与显示,2022,37(11):1411-1419. doi: 10.37188/CJLCD.2022-0240YUAN F, TAN Q G, WANG G Y, et al. Fast and large-angle optical beam deflection based on liquid crystal polarization grating[J]. Chinese Journal of Liquid Crystals and Displays, 2022, 37(11): 1411-1419. (in Chinese) doi: 10.37188/CJLCD.2022-0240 [16] 路陆, 姜鑫, 杨锦程, 等. 基于自适应引导滤波的红外图像细节增强[J]. 液晶与显示,2022,37(9):1182-1189. doi: 10.37188/CJLCD.2022-0024LU L, JIANG X, YANG J CH, et al. Adaptive guided filtering based infrared image detail enhancement[J]. Chinese Journal of Liquid Crystals and Displays, 2022, 37(9): 1182-1189. (in Chinese) doi: 10.37188/CJLCD.2022-0024 [17] 黎四明, 李青, 董旭辉. 具有取向转换膜的偏振无关模式控制液晶透镜[J]. 液晶与显示,2022,37(10):1293-1301. doi: 10.37188/CJLCD.2022-0149LI S M, LI Q, DONG X H. Polarizer-free modal liquid crystal lenses with an alignment conversion layer[J]. Chinese Journal of Liquid Crystals and Displays, 2022, 37(10): 1293-1301. (in Chinese) doi: 10.37188/CJLCD.2022-0149 [18] 付强, 闫磊, 谭双龙, 等. 轻小型金属基增材制造光学系统[J]. 中国光学(中英文),2022,15(5):1019-1028. doi: 10.37188/CO.2022-0128FU Q, YAN L, TAN SH L, et al. Light-and-small optical systems by metal-based additive manufacturing[J]. Chinese Optics, 2022, 15(5): 1019-1028. (in Chinese) doi: 10.37188/CO.2022-0128 [19] 王成龙, 王春阳, 谷健, 等. 一种基于定标的非均匀性校正改进算法[J]. 中国光学,2022,15(3):498-507. doi: 10.37188/CO.2021-0231WANG CH L, WANG CH Y, GU J, et al. An improved non-uniformity correction algorithm based on calibration[J]. Chinese Optics, 2022, 15(3): 498-507. (in Chinese) doi: 10.37188/CO.2021-0231 -
下载:
计量
- 文章访问数: 545
- HTML全文浏览量: 231
- PDF下载量: 203
- 被引次数: 0
