多层介质中隐含层的太赫兹无损检测

在工业应用中,大多数情况下的复合结构介质仅有一面可以被检测,因此需要研究反射模式下检测介质内部参数的太赫兹无损检测方法.推导了反射模式下太赫兹波在三层结构介质中的传输模型,通过遗传算法共同反演估计得到中间分层的厚度,以及它的折射率,从而获得中间隐藏层的具体信息.制备了具有200μm的隐藏分层的三层结构样品,利用太赫兹时域光谱系统对其进行了测量,将理论模型与实测数据进行对比,利用遗传算法估计得到隐藏层的厚度和折射率,将厚度估计值与测厚仪测量结果对比,误差保持在4%以内,折射率估计值与实际值相比,误差范围波动较大,平均误差为6%左右,最后对误差来源进行了分析,为多层复合材料内部缺陷、中间层材料的介电参数估计提供了理论和实验依据.研究表明该系统作为一种无损评价方法可以广泛应用于层状结构的可靠性评价.     

红外低发射率隐身涂层对太赫兹波的反射光谱研究

为研究红外低发射率隐身涂层对太赫兹波的反射特性,制备了红外低发射率隐身涂料,测试了其可见光效果、红外热像图及红外发射率等特性参数。以土黄色红外低发射率涂料为测试样品,利用透射式太赫兹时域光谱系统获得了样品在太赫兹波段的复折射率。分析了特征矩阵理论,并利用特征矩阵理论计算了涂层厚度(0.3~0.5 mm）与入射角度(0°~60°)的变化对入射太赫兹波反射特性的影响。结果表明,在相应厚度及入射角度范围内,太赫兹波在0.8 THz频率下具有多个反射峰值,最高值可达90%以上,有利于实现太赫兹波对红外低发射率隐身涂层下金属目标的探测。此外,涂层厚度变化对入射太赫兹波反射率具有较大影响,涂层越厚,太赫兹波的反射振荡越多,反射峰值越大。入射角度对太赫兹波的反射特性具有一定的影响,但整体影响不大,有利于太赫兹波实现多角度目标的探测。最后,以表面均匀涂覆0.42 mm厚涂料的金属板为测试样品,实验测量了样品在0.1~1.5 THz频率范围内的反射特性,并与部分理论计算结果进行对比。结果表明：实验测量结果与理论计算结果在数值和趋势上较为吻合,但也存在一定的偏差。究其原因,主要由样品厚度和样品参数误差导致,但依然可利用特征矩阵理论研究红外低发射率涂层对太赫兹波的反射光谱特性。     

多层介质中隐含层的太赫兹无损检测（英文）

在工业应用中,大多数情况下的复合结构介质仅有一面可以被检测,因此需要研究反射模式下检测介质内部参数的太赫兹无损检测方法 .推导了反射模式下太赫兹波在三层结构介质中的传输模型,通过遗传算法共同反演估计得到中间分层的厚度,以及它的折射率,从而获得中间隐藏层的具体信息.制备了具有200μm的隐藏分层的三层结构样品,利用太赫兹时域光谱系统对其进行了测量,将理论模型与实测数据进行对比,利用遗传算法估计得到隐藏层的厚度和折射率,将厚度估计值与测厚仪测量结果对比,误差保持在4%以内,折射率估计值与实际值相比,误差范围波动较大,平均误差为6%左右,最后对误差来源进行了分析,为多层复合材料内部缺陷、中间层材料的介电参数估计提供了理论和实验依据.研究表明该系统作为一种无损评价方法可以广泛应用于层状结构的可靠性评价.     

厚度误差对THz-TDS的测量不确定度分析

阐述了基于菲涅尔公式的透射式太赫兹时域光谱系统提取样品光学常数的方法和原理,分析了样品厚度误差对THz-TDS测量不确定度的影响,并建立了相应的不确定度模型。进行太赫兹时域光谱测量实验,提取硅片在太赫兹波段的折射率,并计算了误差对提取样品折射率的影响。结果表明,随着厚度误差的增大,系统测量偏差也随之增大。对于较厚样品,相同厚度误差对其测量结果影响较小。样品厚度为994μm时,在厚度存在1μm的测量误差情况下,系统测量折射率的偏差为0.001 2,接近模型的仿真值。实验结果验证了厚度误差对测量不确定度模型的有效性,了解了厚度误差对系统测量结果的影响情况,对测量过程及结果分析具有一定的指导意义。     

基于太赫兹时域光谱技术的多层涂层高效可靠测厚方法

为实现基于太赫兹技术的多层涂层的快速与可靠测厚,提出了一种自适应教与学优化算法,改进了标准Kent混沌映射,提高了初始种群多样性;并基于步长调节优化和次优个体优化,改进了教阶段与学阶段,提高算法寻优精度和效率。将该算法与太赫兹波测量多层涂层厚度的理论模型结合,建立了涂层厚度求解方法。最后,制备了多层涂层样件,开展了太赫兹无损检测实验。实验结果表明:建立的涂层厚度求解方法相比于全局最优算法的效率提高了1倍,单次实验仅需50 s左右便可快速得到多层涂层的厚度、折射率和消光系数,测量所得的多层涂层厚度的相对误差在1.5%以内,且标准差最大不超过1.7μm。基于太赫兹测量信号,所提方法可以高效、准确及可靠地计算多层涂层的厚度。     

单发太赫兹时域光谱技术

太赫兹时域光谱技术(THz-TDS)广泛应用于材料、生物医学、化学、药学、安检等诸多领域。传统扫描式THz-TDS技术需要通过改变探测光延时逐点扫描并重构时域信号,仅适合于具有较高重复频率且稳定的太赫兹辐射源情形下的样品探测。在低重复频率或涨落较大的太赫兹辐射源情形下和不可逆过程中样品的探测,扫描式THz-TDS不再适用,需要使用单发THz-TDS技术,单发THz-TDS技术原则上仅需要一个激光脉冲就可以获取一个完整的太赫兹时域脉冲波形。介绍几种主要的单发THz-TDS探测技术,这些技术都利用了电光晶体的泡克尔斯效应,通过测量探测光的某个物理量的变化来提取太赫兹信号。根据探测方法不同可分为光谱编码、空间编码和互相关等技术。在光谱编码技术中,探测光不同频率成分在时间上发生分离,不同时间成分分别被太赫兹脉冲不同时刻电场调制,通过测量探测光各个频率被太赫兹脉冲调制前后的光谱的变化提取太赫兹脉冲波形。该方法光路简单,测量结果直观,有较高的信噪比,但其时间分辨率较低,且被测太赫兹信号容易产生失真。为提高被测信号的时间分辨率,有人提出了空间编码技术,即不同位置探测光分别被太赫兹脉冲不同时刻电场调制,通过测量探测光各个位置太赫兹脉冲调制前后的光强变化提取太赫兹脉冲波形。根据不同空间展开方法可分为一维空间编码技术和二维空间编码技术。空间编码技术中虽然有较高的时间分辨率,但由于探测光在空间展开能量分散使得其信噪比相对较低。此外,还有一种较高时间分辨率的技术即互相关技术,可分为共线互相关和非共线互相关技术。在非共线互相关技术中,被太赫兹脉冲调制的激光啁啾脉冲与短脉冲互相关作用产生二次谐波,通过太赫兹脉冲调制前后二次谐波空间分布变化来提取太赫兹信号;在共线互相关技术中被太赫兹脉冲调制的啁啾脉冲与短脉冲共线入射到光谱仪,通过干涉条纹提取太赫兹信号,该技术提高了时间分辨率和信噪比,但光路布置复杂,不能进行实时监测。回顾了这几种单发THz-TDS探测技术的发展历程,综述探测技术的原理、实验方案和测量结果,并讨论了这些探测技术的优势和不足。     

太赫兹片上系统中低温砷化镓薄膜光电导天线的研究

太赫兹时域光谱技术是一种在太赫兹频段内,广泛应用的光谱测量技术。这种技术可以用于许多物质的频谱分析,对于研究化学、半导体与生物分子等领域有着无可比拟的作用。然而用该系统进行样品探测时,受回波的影响频谱分辨率较低;受太赫兹波光斑大小以及待测样品与电磁波相互作用距离长短的影响,样品消耗量较多,并且整个系统的占用空间较大,这些局限性都限制了太赫兹时域光谱系统的进一步发展。为了突破太赫兹时域光谱系统的局限性,设计了一种将太赫兹泵浦区、探测区和传输波导集成到一个硅片上的太赫兹片上系统,该系统不仅能够解决上述系统的局限性,还能够省去样品测量前的光路准直环节,使样品的测量过程更加简便,同时集成化的系统也很大程度上提高了太赫兹波传输的稳定性。在太赫兹片上系统中,泵浦区和探测区的光电导天线是由低温砷化镓和金属电极制成,由于受到太赫兹片上系统的高度集成化和低温砷化镓晶体生长条件的限制,如何制备出低温砷化镓半导体薄膜衬底,并将其转移与键合,是太赫兹片上系统研制过程中的关键环节。首先利用分子束外延（MBE）技术制备出由半绝缘砷化镓、砷化镓缓冲层、砷化铝牺牲层和低温砷化镓层构成的外延片,然后利用盐酸溶液与砷化铝和低温砷化镓反应速度差别较大的原理,将200 nm厚的AlAs牺牲层腐蚀掉,从而得到2 μm厚的低温砷化镓薄膜。为了更加高效并且完整地得到低温砷化镓薄膜,研究了盐酸溶液在不同温度和不同浓度下与AlAs牺牲层的选择性腐蚀速率的关系。给出了低温砷化镓薄膜制备过程中盐酸的最佳体积比浓度和最佳温度,即在73 ℃下13.57%的盐酸溶液中进行砷化铝牺牲层的腐蚀。相比于已有工艺,这种腐蚀方法对实验设备的要求较低并且具有较高的安全性。最后,将单层低温砷化镓薄膜转移键合至硅片上,并制成光电导天线的结构。利用飞秒激光脉冲进行激发探测到太赫兹信号。由此说明,低温砷化镓薄膜的获取、转移与键合工艺能够满足芯片级太赫兹系统的制作要求,这为太赫兹片上系统的进一步研制打下了坚实的基础。     

基于太赫兹光谱的固体片剂孔隙率研究

内部孔隙影响着药片的崩解特性,进而影响药效的发挥,但目前鲜有关于药片孔隙率有效检测手段的报道。基于太赫兹脉冲的飞行时间测量原理,利用太赫兹时域光谱技术研究了微晶纤维素和吲哚美辛混合片剂的孔隙率与折射率、吲哚美辛质量分数之间的定量关系;建立了三者关系的数学计算模型,通过实际测试固体样品片剂的太赫兹时域光谱,计算了片剂的孔隙率、折射率。结果表明:片剂的孔隙率与折射率、不同成分质量分数间存在线性关系,与建立的数学计算模型相符。利用太赫兹光谱法测得的孔隙率与采用气体置换法测量的孔隙率的平均相对误差为6.0%,与采用密度法计算的孔隙率的平均相对误差为8.9%,表明利用太赫兹光谱法测量片剂孔隙率具有可行性,能够成为药物片剂质量监测的补充手段。     

基于液晶空间光调制器的太赫兹波频谱调制

频谱可调制的太赫兹波具有广泛的应用价值。利用一台纯相位式的液晶空间光调制器对飞秒激光脉冲进行空间整形,通过改变飞秒激光脉冲的横向空间分布,实现太赫兹波频谱的调制。在实验中,利用光泵浦整流方式产生太赫兹波,并利用太赫兹时域光谱系统对太赫兹信号进行探测。通过GS算法在液晶空间光调制器上加载不同的相位图,获得了不同的飞秒激光脉冲横向空间分布。通过改变探测距离和飞秒脉冲的空间分布参数,实现了太赫兹波频谱的调制。还利用菲涅尔衍射算法对这一过程进行了理论模拟,理论模拟结果与实验结果吻合的较好,这充分说明了基于飞秒脉冲空间整形的太赫兹光谱调制技术的可行性。     

基于衰减全反射式太赫兹时域光谱技术的食用油光谱特性研究

食用油是人类营养和能量的重要来源,为人体提供必需的脂肪酸,研究食用油在太赫兹波段光学特性,对食用油成分分析及品质评价具有重要价值。衰减全反射式太赫兹时域光谱技术是一种新型的太赫兹时域光谱技术,通过样品与倏逝波的相互作用,获取样品的太赫兹光谱。与透射式或反射式太赫兹时域光谱技术相比,该技术能有效地避免测量食用油等液体样品时样品池对光学参数的影响,并能获得样品的精确光学参数。分别利用透射式太赫兹时域光谱技术和衰减全反射式太赫兹时域光谱技术测量了大豆油的吸收光谱。结果表明,与透射式太赫兹时域光谱技术相比,衰减全反射式太赫兹时域光谱技术能更有效地提取大豆油的吸收系数、吸收峰分布等光学特性。进一步利用衰减全反射式太赫兹时域光谱技术研究了大豆油、核桃油、葡萄籽油在太赫兹波段的光学特性,获得了三种食用油在1~1.8 THz范围内的折射率谱和吸收光谱。利用密度泛函理论计算了食用油中四种主要成分(软脂酸、硬脂酸、油酸和亚油酸)在太赫兹波段的振动、转动模式,理论计算结果同实验测量结果吻合较好。研究表明,在太赫兹波段食用油的吸收峰与所含脂肪酸分子种类与含量有关,其主要来源为脂肪酸分子的低频振动和转动。研究成果对食用油成分定性定量分析及品质检测等具有指导意义。     

Evaluation of paint coating thickness variations based on pulsed Infrared thermography laser technique

In this paper, a pulsed Infrared thermography technique using a homogeneous heat provided by a laser source is used for the non-destructive evaluation of paint coating thickness variations. Firstly, numerical simulations of the thermal response of a paint coated sample are performed. By analyzing the thermal responses as a function of thermal properties and thickness of both coating and substrate layers, optimal excitation parameters of the heating source are determined. Two characteristic parameters were studied with respect to the paint coating layer thickness variations. Results obtained using an experimental test bench based on the pulsed Infrared thermography laser technique are compared with those given by a classical Eddy current technique for paint coating variations from 5 to 130 μm. These results demonstrate the efficiency of this approach and suggest that the pulsed Infrared thermography technique presents good perspectives to characterize the heterogeneity of paint coating on large scale samples with other heating sources.     

激光辐射致热单层薄膜温度响应

用热传导方程计算了在脉宽10ns、波长1.06μm的激光辐射下,TiO_2单层膜的温度场分布.结果表明:膜层的热参数增大,其峰值温度明显降低,而基板热参数变化对膜层温度响应影响很小,温度场分布由电场分布决定,1/4波长薄膜的峰值温度低于半波长薄膜的峰值温度.     

Simple fabrication of an antireflective hemispherical surface structure using a self-assembly method for the terahertz frequency range

A hemispherical surface structure was fabricated on a sapphire substrate by utilizing a self-assembly and spin-coating process for a terahertz (THz) antireflection coating. The self-assembled glass spheres and spin-coated material led to a gradual change in the effective refractive index. The aspect ratio of the hemispherical surface structure was controlled easily by adjusting the thickness of the B-staged bisbenzocyclobutene used as a coating. The reflectance of the fabricated hemispherical surface structure, having a period of 140 μm, exhibited low reflectance and low Fabry-Perot resonance in a THz spectral range from 0.1 to 1.9 THz.     

白光LED光斑均匀性的改进

用于照明领域的白光LED,其出射光斑的色度均匀性对于产品性能有着更加重要的意义.介绍了目前工业上制作白光LED主要采用的荧光粉灌封点胶工艺.并在目前主流灌封点胶工艺的基础上通过改善荧光粉层结构形状,以提高白光LED器件的出射光斑均匀性.并通过九点法对不同工艺结构下LED出射光斑的空间色度分布进行了测量和分析.通过分析,虽然采用不同的粉层结构,能够一定程度上改善白光光斑的色度均匀性.但总体上,采用这种传统的点胶工艺制作的器件的白光光斑性能不好,现有的荧光粉层灌封点胶工艺存在很大的弊端.荧光粉层的可控性是影响色度均匀性(即光斑均匀性)的主要因素,包括单个器件内的光斑和器件之间的颜色一致性都不理想.     

Forensic examination of multilayer white paint by lateral scanning Raman spectroscopy

Multilayer samples of white architectural paint potentially have very high evidential value in forensic casework, because the probability that two unrelated samples will have the same sequence of layers is extremely low. However, discrimination between the different layers using optical microscopy is often difficult or impossible. Here, lateral scanning Raman spectroscopy has been used to chemically map the cross‐sections of multilayer white paint chips. It was found that the spectra did allow the different layers to be delineated on the basis of their spectral features. The boundaries between different layers were not as sharp as expected, with transitions occurring over length scales of > 20 µm, even with laser spot diameters < 4 µm. However, the blurring of the boundaries was not so large as to prevent recording and identification of spectra from each of the layers in the samples. This method clearly provides excellent discrimination between different multilayer white paint samples and can readily be incorporated into existing procedures for examination of paint transfer evidence. © 2011 Crown copyright.     

High-dispersive mirror for pulse stretcher in femtosecond fiber laser amplification system

We present a high-dispersive multilayer mirror for pulse stretching in a femtosecond fiber laser amplification system. The designed mirror contains 54 layers with a total physical thickness of 7.3 μm, which can provide a positive group delay dispersion (GDD) of 600 fs² and a high reflectance over 99.9% from 1010 to 1070 nm. The samples were prepared by dual ion beam sputtering. The measured transmittance matches well with the theoretical result. The GDD characteristics of samples were tested by home-made white light interferometer. The measured GDD is higher than the design results, an average GDD of +722 fs² from 1010 nm to 1070 nm. The mirrors were employed in a Yb-doped large-mode-area photonic crystal fiber amplification system. An input pulse compressed by the gratings with autocorrelation function of 83 fs is obtained with a stretched FWHM of 1.29 ps after 28 bounces between the dispersive mirrors. The results show that the multilayer dispersive mirror could be an effective and promising technique for pulse stretching in femtosecond amplification systems.     

Microstructure and properties of plastic deformed martensite induced by laser shock processing

Firstly, 45# steel was quenched by the NEL-2500A rapidly axial flow CO2 laser. The experimental parameters were the laser power of 750 W, the laser beam diameter of 4 mm, the scanning velocity of 7 mm/s.The thickness of coating layer was 0.1 mm and the width was 8 mm. Secondly, the martensite induced by laser quench was shocked by Nd:YAG laser. The parameters of laser shock processing were the wavelength of 1.06 μm, the pulse duration of 23 ns, and the output energy of 16-20 J. The laser was focused on a spot of φ7 mm. K9 optical glass was used as confinement. The sample was coated with black paint 86-1 (the thickness is about 0.025 mm). By testing and analysis of samples which were treated by laser quench and laser quench+shock with transmission electron microscope (TEM), it was discovered that the surface layer of martensite was deformed plastically by laser shock processing. In the secondary hardened zones,there were a lot of slender secondary twin crystal martensites, dislocation tangles, and cellular dislocations.Compared with that of the hardened zones through laser quench only, the residual stress and mechanical properties of the secondary hardened zones were improved and increased through laser compound method.     

Experimental study on laser cleaning of paint layer on white marble surface北大核心CSCD

In order to effectively remove the surface paint of the cultural relic of white marble, the area extrapolation method and laser-induced plasma spectroscopy (LIPS) method were used to obtain the ablation threshold power of the gold, silver paint layer and white marble surface. On the basis of this, the optimal laser power for removing paint without damaging the white marble substrate was determined. The image processing method was used to study the cleaning degree and variation trend of cleaning rate of the gold and silver paint on the surface of 10 mm×10 mm white marble by laser cleaning, and the optimal laser spot overlap rate and the optimal cleaning times were obtained. Finally, the image processing method was used to evaluate the cleaning effect of laser cleaning of paint layer on the white marble surface. More than 93% of the cleaning degree shows that the synergistic use of the area extrapolation method, LIPS method and image processing method can effectively improve the laser cleaning efficiency of the paint layer on white marble surface. Copyright ©2022 Journal of Applied Optics. All rights reserved.