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NVThermIP模型作为经典的性能模型，在指导红外系统参数的设计优化方面略有不足，因此需要构建更科学合理的综合评估模型.在经典模型基础上，结合人眼噪声的理论和实验研究，利用噪声等效温差修正了系统的对比度阈值函数.并利用现有的红外系统实验数据，对修正后的模型进行图像模糊和不同距离下辨识两方面验证，结果证明该模型具有很高的预测精确度，可为新型系统设计分析提供可靠的依据和理论指导.
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关键词:
- 系统设计 /
- NVThermIP模型 /
- 对比度阈值函数 /
- 噪声等效温差
With the innovation of infrared imaging technology, the performance evaluation of the infrared imaging system plays an indispensable role in the general technology. Therefore, the establishment of a comprehensive, scientific and reasonable performance evaluation model is a prerequisite for accurately predicting the performance of the imaging system, and is also an effective technology to design and develop the high performance imaging system. According to previous studies, in this paper we analyze the key problems that need to be solved urgently in the current research and the factors limiting the development of performance evaluation techniques. The main researches of this paper are as follows. 1) Through improving the deficiencies of the inherent physical effect evaluation methods, the accuracy and reliability of the performance evaluation model are enhanced. 2) In order to meet the needs of performance optimization design, the performance parameters provided by product design and production requirements must be selected correctly to achieve an organic combination of performance evaluation model and imaging system.The NVThermIP model, a widely used performance evaluation model, is slightly inadequate for guiding the optimization of the parameters of an infrared system. A more scientific and reasonable performance evaluation model is proposed in this paper, in which the contrast-threshold function of the system in the NVThermIP model is corrected by noise equivalent temperature difference based on the theory of the human-eye noise. By quantitatively analyzing the typical physical effects on infrared imaging system, the modeling theory and process of NVThermIP model are introduced in detail. The simulation results give a visual representation of evaluating the performance of an infrared imaging system. The limitations of the NVThermIP model used to guide the design and production of the system and the deficiencies of the early theoretical basis for system optimization design are analyzed. The noise equivalent temperature difference is introduced to revise and perfect the NVThermIP model combined with the theory of human eye noise. The accuracy of the newly proposed model is verified by two experiments. Experimental results show that the corrected model is more accurate in system prediction and can be used to guide the design of a new system.-
Keywords:
- system design /
- NVThermIP model /
- contrast threshold function /
- noise equivalent temperature difference
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[7] Teaney B P, Tomkinson D M 2015 Proc. SPIE 9452 94520P
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[10] Li Q, Yang C, Zhang J Q 2012 Appl. Opt. 51 7668
[11] Vaitekunas D A, Holst G C, Ramaswamy S 2015 Proc. SPIE 9452 94520G
[12] Hu M P 2009 Infrared Technol. 31 27 (in Chinese)[胡明鹏 2009 红外技术 31 27]
[13] Devitt N, Moyer S, Flug E 2005 Proc. SPIE 5784 48
[14] Teaney B P, Reynolds J P 2007 Proc. SPIE 6543 65430L
[15] Moyer S, Devitt N 2005 Proc. SPIE 5784 60
[16] Vollmerhausen R 2016 Opt. Express 24 23654
[17] Vollmerhausen R H, Driggers R G, Wilson D L 2008 J. Opt. Soc. Am. A 25 2055
[18] Dulski R, Barela J, Trzaskawka P 2013 Proc. SPIE 8896 889617
[19] Zuo F, Liu G R, Gao Z Y 2002 Opt. Technol. 28 63 (in Chinese)[左昉, 刘广荣, 高稚允 2002 光学技术 28 63]
[20] Tohyama S, Sasaki T, Endoh T, et al. 2015 Yun Guang Ji Shu 1 41
[21] Sui X B, Chen Q, Lu H H 2007 J. Infrared Millim. Waves 26 377 (in Chinese)[隋修宝, 陈钱, 陆红红 2007 红外与毫米波学报 26 377]
[22] Da Z S, Chen L Y 2003 Acta Photon. Sin. 32 669 (in Chinese)[达争尚, 陈良益 2003 光子学报 32 669]
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[1] Gerald C H (translated by Yan J X, Yu X) 2015 Electro-optical Imaging System Performance (4th Ed.) (Beijing: National Defence Industry Press) pp1-8 (in Chinese)[霍尔斯特 著 (阎吉祥, 俞信 译) 2015 光电成像系统性能 (第四版) (北京: 国防工业出版社) 第1–8页]
[2] Li X D, Ai K C, Wang W 2004 J. Appl. Opt. 25 37 (in Chinese)[李旭东, 艾克聪, 王伟 2004 应用光学 25 37]
[3] Tsujino Y 2010 Infrared Phys. Technol. 53 50
[4] Gravrand O, Baier N, Ferron A 2014 J. Electron. Mater. 43 3025
[5] Preece B L, Reynolds J P, Fanning J D 2011 Proc. SPIE 8014 801406
[6] Vollmerhausen R H 2009 Opt. Express 17 17253
[7] Teaney B P, Tomkinson D M 2015 Proc. SPIE 9452 94520P
[8] Holst G C 2007 Opt. Eng. 46 103204
[9] Preece B L, Reynolds J P, Fanning J D 2014 Opt. Eng. 53 061712
[10] Li Q, Yang C, Zhang J Q 2012 Appl. Opt. 51 7668
[11] Vaitekunas D A, Holst G C, Ramaswamy S 2015 Proc. SPIE 9452 94520G
[12] Hu M P 2009 Infrared Technol. 31 27 (in Chinese)[胡明鹏 2009 红外技术 31 27]
[13] Devitt N, Moyer S, Flug E 2005 Proc. SPIE 5784 48
[14] Teaney B P, Reynolds J P 2007 Proc. SPIE 6543 65430L
[15] Moyer S, Devitt N 2005 Proc. SPIE 5784 60
[16] Vollmerhausen R 2016 Opt. Express 24 23654
[17] Vollmerhausen R H, Driggers R G, Wilson D L 2008 J. Opt. Soc. Am. A 25 2055
[18] Dulski R, Barela J, Trzaskawka P 2013 Proc. SPIE 8896 889617
[19] Zuo F, Liu G R, Gao Z Y 2002 Opt. Technol. 28 63 (in Chinese)[左昉, 刘广荣, 高稚允 2002 光学技术 28 63]
[20] Tohyama S, Sasaki T, Endoh T, et al. 2015 Yun Guang Ji Shu 1 41
[21] Sui X B, Chen Q, Lu H H 2007 J. Infrared Millim. Waves 26 377 (in Chinese)[隋修宝, 陈钱, 陆红红 2007 红外与毫米波学报 26 377]
[22] Da Z S, Chen L Y 2003 Acta Photon. Sin. 32 669 (in Chinese)[达争尚, 陈良益 2003 光子学报 32 669]
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