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激光诱导表面周期性结构对铜薄膜红外发射特性的改变
引用本文:王田宇,卞进田,李欣,孔辉,孙晓泉.激光诱导表面周期性结构对铜薄膜红外发射特性的改变[J].中国激光,2021(4):264-271.
作者姓名:王田宇  卞进田  李欣  孔辉  孙晓泉
作者单位:国防科技大学脉冲功率激光技术国家重点实验室;国防科技大学先进激光技术安徽省重点实验室
基金项目:安徽省自然科学基金青年基金(2008085QF314);先进激光技术安徽省实验室青年基金(ky19c604);国防科技大学自主科研项目(zk19-15)。
摘    要:金属铜在中红外波段的发射率极低,所以铜薄膜是一种性能优异且对抗被动式中红外热探测器隐身的材料,而在铜薄膜表面使用激光诱导表面周期性结构(LIPSS)可以显著提高其在中红外波段的发射率。首先使用双温方程模型模拟LIPSS形成过程中材料软化的过程,然后使用波长为1064nm的偏振脉冲激光在融石英基底上的铜薄膜表面诱导产生周期为波长量级的LIPSS,最后基于实验产生的铜薄膜LIPSS搭建仿真模型并对其在近红外和中红外波段的发射率进行分析。模拟结果表明,铜薄膜LIPSS的产生可以显著提高其在中红外波段的发射率,该方法可以实现铜薄膜对被动式中红外热探测器的隐身。

关 键 词:激光光学  激光损伤  激光诱导表面周期性结构  中红外激光  发射率  反隐身

Effect of Laser Induced Periodic Surface Structures on Infrared Emission Characteristics of Copper Films
Wang Tianyu,Bian Jintian,Li Xin,Kong Hui,Sun Xiaoquan.Effect of Laser Induced Periodic Surface Structures on Infrared Emission Characteristics of Copper Films[J].Chinese Journal of Lasers,2021(4):264-271.
Authors:Wang Tianyu  Bian Jintian  Li Xin  Kong Hui  Sun Xiaoquan
Affiliation:(State Key Laboratory of Pulsed Power Laser Technology,National University of Defense Technology,Hefei Anhui 230037 China;Anhui Key Laboratory of Advanced Laser Technology,National University of Defense Technology,Hefei Anhui 230037 China)
Abstract:Objective Metal films have lots of excellent characteristics such as higher mechanical strength and damage threshold,better toughness,and thermal conductivity.They are widely used in modern optical industry.Moreover,copper films are used as infrared stealth material because the emissivity of copper is very low in mid-infrared band.This property can reduce the detection efficiency of passive mid infrared detector.The characteristic has extensive applications in military and many groups have performed research about it.However,they only focused on production of high quality copper film.However,the methods to destroy this film are ignored,which is presented in this paper.Laser-induced periodic surface structure(LIPSS)is special surface grating structures which is induced by polarized pulses that appear on nearly all kinds of solid materials.The period and direction of the grating only depend on the wavelength and polarized direction of laser.The structures can change the surface properties of materials such as super hydrophilic/hydrophobic,suppress the growth of the miscellaneous bacteria,as well as high emissivity.LIPSS has drawn attentions of many researchers.Lots of new materials with special characters have been produced by inducing LIPSS on the surface of the materials.However,the study of changing emission characteristics within mid-infrared band of metal films is lacking.Some researches are performed about the effect of LIPSS on infrared emission characteristics of copper films in this paper.Methods First,the production of LIPSS on copper films is investigated using the surface interference between plasmons and incident laser model(Sipe model).The Sipe model involves two processing:softening and migration of materials.A two-temperature model is used to illustrate the copper-softening process.The theory of the twotemperature absorption of metals can be applied to all types of incident lasers because the processing is performed by the distribution of a large number of free electrons on the material surface,which is different from other types of materials.Therefore,a linear pulse at a center wavelength of 1064 nm with a pulse duration of 100 fs and energy density of 5 J/m2 is used in the simulation experiment.Then,LIPSS is induced on a copper film that covered a quartz substrate using nanosecond linear pulses at a center wavelength of 1064 nm.Additionally,a simulation model is established according to the surface topography of the sample induced in the experiment.The emissivity is within the 1--5μm band.Results and Discussions The results of the two-temperature model experiment show that the temperature of the copper free electrons reaches 7073 Kafter the pulse introduction is finished,which is very much higher than the melting point of copper(1375.8 K).The high temperature softens the target,which means that materials can be rearranged under a periodic space electromagnetic field according to the Sipe model.Then,the temperature of the electronic system quickly decreases,whereas that of the lattice system gradually increases.At 12 ps,the temperatures of the two systems are balanced at 1017 K,which is less than the melting point(Fig.2),indicating that classical heat damage does not occur.LIPSS is induced by linearly polarized nanosecond pulses(Fig.4).The direction of the gratings is perpendicular to the polarization direction of the laser.The results show that lowsurfacefrequency LIPSS(LSFL)is induced on the film.The electric field distribution of the reflected and transmitted fields of the simulation model show that the laser is modulated by the gratings(Fig.6).Therefore,the emissivity of the model can reach 0.365 and 0.119 when the laser wavelength is 3μm and 5μm,respectively(Fig.7),which is very much higher than that of smooth copper(Fig.1).The results show that LIPSS can improve the emissivity of copper films.Conclusions This paper has presented three main studies.The first one is a brief explanation of how LIPSS can be induced by pulses lower than the damage threshold of materials.The Sipe model is used to describe the process of inducing LIPSS on metals.The material-softening step due to the pulses,whose influence is lower than the damage threshold,is achieved using a two-temperature simulation model.The second study induces LIPSS on a copper film over a quartz basement.The LIPSS is of LSFL type.The results agree with those in the previous studies.The third one proves that LIPSS can improve the emissivity of copper films through a simulation experiment.The results show that a much higher emissivity of films is achieved with LIPSS because the space electromagnetic field is periodically modulated by the micro gratings.The effect on the improvement is significant.These results show that inducing LIPSS on the surface of copper films is a feasible technique to destroy the stealth characteristics of a material in the mid-infrared band.
Keywords:laser optics  laser damage  laser-induced periodic surface structures  mid-infrared laser  emissivity  anti-invisible
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