平面反射镜反射率检测系统研究

为实现在高功率激光装置中对平面反射镜反射率的高精度测量,提出了将双光束分光光度法与VW测量法相结合,利用扩束后的测量光束测量被测元件的反射率.推导了计算公式,搭建了测量光束口径为50mm的检测系统,通过对标准吸收玻璃吸收值的测试验证了系统对光束能量测试的准确性.利用该系统对高功率激光装置使用的反射镜的反射率进行了测量,...     

高折射玻璃微珠粒径与折射率关系的研究

利用激光照射高折射率玻璃微珠下形成的二次彩虹现象,以艾里的虹理论为基础对玻璃微珠折射率进行了测量。推导了玻璃微珠尺寸对折射率影响的计算公式,表明半径差异在10μm时,折射率的测量误差为10^-3数量级。此外,通过软件模拟计算玻璃微珠的二次彩虹现象,并对微珠的折射率进行了测量,验证了二次彩虹方法的正确性,同时也表明玻璃微...     

部分相干光束通过硬边光阑的推广光束传输M2因子

给出部分相干光通过硬边光阑后的强度二阶矩的计算公式，由此可得到部分相干光通过硬边光阑后的推广光束传输M^2因子。以部分相干高斯－谢尔模型光束为例，推导出相应的M^2因子，并作了数值计算和分析讨论。     

光场电离气体原子体系的剩余电子能量

总结并推导了在考虑激光脉冲包络时超短强激光脉冲光场电离多电子气体原子体系的阈上电离能量的计算公式,消除了以往研究中的唯象假设。发展了产生各阶离化态离子的阈值光强和饱和光强的计算方法。数值模拟表明,随激光能量升高,平均剩余电子能量呈现出类似阶梯型平台的饱和行为。     

端面反射率的波长特性对外腔半导体激光器调谐范围的影响

端面镀增透膜的激光二极管构成的光栅外腔激光器（ECLD）中,考虑到镀膜端面剩余反射率对波长的依赖关系以后,利用等效腔法导出了该激光器阈值载流子密度随波长变化的解析表达式,以此为出发点,讨论了增透膜反射率极小位置对调谐范围的影响。结果表明,除了增大剩余反射率工和降低剩余反射率能够提高调谐范围这一明显结论这外,在镀膜工艺确定的情况下,即假定剩余反射率带宽和剩余反射率极小值变化不大时,通过控制剩余反射率极小值所对应的波长相对于镀膜前增益峰的偏移量,可进一步拓宽波长调谐范围。     

激光辐照下复合材料树脂基热分解3维温度场模型

 采用控制体积法,从质量和能量守恒角度,推导了激光辐照下复合材料树脂基热分解时温度变化的基本方程。用多步模型描述树脂的热分解反应。提出了热分解气体的1维运动假设,这使得可以在3维情况下考虑热分解气体对流传输的影响,且在不引入力学量的前提下实现3维温度场模型的封闭。考虑到树脂基复合材料的各向异性,对部分分解材料的导热率计算公式进行了推导,并重新推导了部分分解材料对激光的吸收系数计算公式。在一定的简化下,推导的能量守恒方程与文献结果一致。     

微型铒玻璃激光器研究

报道了微型铒玻璃激光器的阶段性研究成果，研究了在自由振荡情况下输出膜片反射率、氙灯气压以及激光电容的大小对激光输出的影响。采用电光调Ｑ，获得了８ｍＪ的巨脉冲输出；采用转镜调Ｑ，获得了１２ｍＪ的巨脉冲输出，脉宽８０ｎｓ。     

微型饵玻璃激光器研究

报道了微型饵玻璃激光器的阶段性研究成果，研究在自由振荡情况下输出膜片反射率，氙灯气压及激光电容的大小对激光输出的影响，采用电光调Ｑ，获得了８ｍＪ的巨脉冲输出，采用转镜调Ｑ，获得了１２ｍＪ的巨脉冲输出，脉宽８０ｎｓ。     

基于激光自混合传感器的齿轮局部故障振动信号分析

建立了齿圈局部故障调频现象模型,分析了故障轮齿啮合频率及其倍频两侧边频带的产生机理,给出了齿圈局部故障特征频率的计算公式,建立了倒频谱分析模型。采用激光自混合传感器,分别从径向和轴向两个方向采集齿轮箱振动信号波形。在齿轮箱1Hz和2Hz两种不同输出转频下,分别研究了无故障齿轮箱和故障齿轮箱的振动信号特征。通过实验研究验证了理论推导结果。     

倾斜离轴高斯光束通过猫眼光学镜头的传输特性

运用矩阵光学理论以及将硬边光阑窗口函数展开为有限个复高斯函数之和的方法,进一步推导了倾斜离轴高斯光束通过猫眼光学镜头的解析传输公式,通过数值计算分析得到了倾斜系数和离轴量对猫眼效应反射光光强分布的影响规律.结果表明,斜入射情况下猫眼效应反射光光强分布发生非对称畸变,且倾斜系数较小和较大时有着不同的分布规律.并且,离轴量与倾斜系数共同决定着猫眼效应反射光应用于激光主动探测的可行性.     

Efficient Analysis of Millimeter Wave Ferrite Circulators by the GMRES Iterative Algorithm

The finite element method (FEM) combined with the perfectly matched layers (PML) is given for simulation of waveguide ferrite circulators. The generalized minimal residual (GMRES) iterative method is applied to solve such sparse large non-symmetric system of linear equations resulting from the use of edge-based finite element method. The formulation of FEM and the algorithm of GMRES method are described in detail. The reflection and insertion losses of millimeter wave waveguide circulator are analyzed and the results are compared with those obtained from literature.     

The effects of residual gases on optical constants of Al films

Using the attenuated total reflection technique, the effects of residual gases on optical constants of Al films have been investigated in situ during and after growth of films. It has been found that the optical constants of Al films are strongly affected by residual gases even under ultrahigh vacua (UHV) in the order of 10⁻⁶ Pa. In order to explore the origin of a variation in optical constants produced by the residual gases, the optical constants of Al films exposed to oxygen, nitrogen or hydrogen gases have been measured.     

Accuracy design of ultra-low residual reflection coatings for laser optics

Refractive index inhomogeneity is one of the important characteristics of optical coating material, which is one of the key factors to produce loss to the ultra-low residual reflection coatings except using the refractive index inhomogeneity to obtain gradient-index coating. In the normal structure of antireflection coatings for center wavelength at 532 nm, the physical thicknesses of layer H and layer L are 22.18 nm and 118.86 nm, respectively. The residual reflectance caused by refractive index inhomogeneity(the degree of inhomogeneous is between -0.2 and 0.2) is about 200 ppm, and the minimum reflectivity wavelength is between 528.2 nm and 535.2 nm. A new numerical method adding the refractive index inhomogeneity to the spectra calculation was proposed to design the laser antireflection coatings, which can achieve the design of antireflection coatings with ppm residual reflection by adjusting physical thickness of the couple layers. When the degree of refractive index inhomogeneity of the layer H and layer L is-0.08 and 0.05 respectively, the residual reflectance increase from zero to 0.0769% at 532 nm. According to the above accuracy numerical method, if layer H physical thickness increases by 1.30 nm and layer L decrease by 4.50 nm, residual reflectance of thin film will achieve to 2.06 ppm. When the degree of refractive index inhomogeneity of the layer H and layer L is 0.08 and -0.05 respectively, the residual reflectance increase from zero to 0.0784% at 532 nm. The residual reflectance of designed thin film can be reduced to 0.8 ppm by decreasing the layer H of 1.55 nm while increasing the layer L of 4.94 nm.     

High efficiency infrared antireflection coatings (ARCs) for space optics

Simple ARC designs for germanium (Ge) optics useful in spaceborne electro-optical systems have been generated. It is seen that the designs which are non-quarterwave in nature are efficient in terms of spectral coverage and residual reflection loss. They have been realised experimentally and the resulting ARCs are found to have very good spectral and durability properties.     

Analytical properties of the spectral characteristics of antireflection coatings

The spectral dependences of the coefficients of multilayer antireflection optical coatings are analyzed. The results can be used in research directed toward determining the lower limit of residual reflection.     

Application of Preconditioned GMRES Algorithm for Analysis of Millimeter Wave Ferrite Sphere Circulators

The generalized minimal residual (GMRES) iterative method is applied to solve such sparse large non-symmetric system of linear equations resulting from the use of edge-based finite element method. In order to speed up the convergence of GMRES, the symmetric successive overrelaxation (SSOR) preconditioning scheme is applied for the analysis of millimeter wave ferrite circulator. Consequently, this preconditioned GMRES (PGMRES) approach can reach convergence ten times faster than GMRES. The reflection and insertion losses of millimeter wave waveguide circulator are compared with those obtained from literature.     

Combined implementing the hole-drilling method and reflection hologram interferometry for residual stresses determination in cylindrical shells and tubes

Main features inherent in simplified approach to residual stresses determination in cylindrical shells and tubes, external diameter of which is not less than 60 mm, by combing the hole-drilling method and reflection hologram interferometry are discussed in detail. Initial experimental information in a form of hole diameter increments in principal stress directions is derived from high-quality reflection holograms recorded near cylindrical objects of intermediate curvature value. Converting measured parameters into required stress values is based on the transition model that corresponds to plane stress conditions of pure membrane type. The technique developed is capable of determining residual stress component values within 5% accuracy in an absence of stress gradients over the probe hole diameter when a type of residual stress field corresponds to the transition model adopted. The accuracy analysis involved is based on matrix formulation of conventionally direct problem and an assumption on a pure membrane character of residual stress field under study for thin-walled shell. Required error estimations in a case of inspecting thick-walled cylindrical tube are obtained by combining the above-mentioned approach and an analogy of reconstructed fringe patterns with actual and artificial interferograms, which follow from drilling blind hole of the same geometrical parameters in thick-walled plates. Experimental verification of the developed approach is founded upon a determination of actual stresses in thin-walled cylindrical shell and obtaining residual stress distributions at the proximity of welded joint in thick-walled cylindrical tube.     

A role of fringe pattern catalogue in the course of interferometrically based determination of residual stresses by the hole-drilling method

A further development of the technique for residual stresses determination in thick-walled structures, which is based on a combination of the hole-drilling method and reflection hologram interferometry, is presented. A plane specimen welded from two equal parts of dimensions 130×80 mm² in plane and thickness 12 mm is the object of investigation. Weld seam is performed along the shortest side of the specimen. Residual stress field of interest is formed by a superposition of initial welding-induced field and secondary stress field caused by plastic deformation of the specimen. A set of actual fringe patterns, which corresponds to a wide variety of residual stress components both ratio and sign, are reconstructed and presented as illustrations. A series of reference fringe patterns is simulated for the most typical cases inherent in residual stress field under study. It is shown that actual interferograms obtained belong to three main groups depending on a typical form of fringes configuration. On this base the main principles of creating the general catalogue of fringe patterns are established and the first version of this catalogue, which is related to reflection hologram interferometry, is developed. A structure of the catalogue that consists of both actual interferograms and reference fringe patterns is described. Possible ways of further catalogue completing and its direct implementing in the course of quantitative determination of residual stresses are discussed. It is shown that both experimental and numerical data aggregated into the first version of the catalogue can be effectively used for a verification of various coherent optics techniques with respect to a determination of residual stress components by means of hole drilling. An analysis of capabilities of reflection hologram interferometry in the field of residual stresses determination comparing with dual-beam speckle-interferometric techniques is presented. Superimposed residual stress field is quantitatively described in detail for both specimen sides of dimensions 260×80 mm². It is shown that fine nuances inherent in residual stress distributions over different specimen faces can be reliably derived from recorded fringe patterns of any type. This study serves as an example of residual stress components determination in real structure with a type of residual stress field to be investigated is unknown before the experiment.     

Holographic interferometry for measuring residual stresses by using probing holes

An original method of determining residual stresses by using probing holes and measuring the difference in the holographic interference fringe orders for two sets of pairs of points taken on the principal strain axes is suggested. The optical scheme of the interferometer is based on the use of reflection holograms. The principal residual strains are found by solving an overdetermined set of linear equations. The effect of rigid displacement on the fringe pattern is taken into account. The method is experimentally verified by measuring elastic stresses in uniaxially and biaxially strained specimens.     

Characterizing distortion-product otoacoustic emission components across four species

Distortion-product otoacoustic emissions (DPOAEs) were measured as level/phase (L/P) maps in humans, rabbits, chinchillas, and rats with and without an interference tone (IT) placed either near the 2f(1)-f(2) DPOAE frequency place (f(dp)) or at one-third of an octave above the f(2) primary tone (1/3-oct IT). Vector differences between with and without IT conditions were computed to derive a residual composed of the DPOAE components removed by the IT. In humans, a DPOAE component could be extracted with the expected steep phase gradient indicative of reflection emissions by ITs near f(dp). In the laboratory species, ITs near f(dp) failed to produce any conclusive evidence for reflection components. For all species, 1/3-oct ITs extracted large DPOAE components presumably generated at or basal to the IT-frequency place that exhibited both distortion- and reflection-like phase properties. Together, these findings suggested that basal distortion components could assume reflection-like phase behavior when the assumptions of cochlear-scaling symmetry, the basis for shallow phase gradients for constant f(2)/f(1) ratio sweeps, are violated. The present results contradict the common belief that DPOAE components associated with steep or shallow phase slopes are unique signatures for reflection emissions arising from f(dp) or distortion emissions generated near f(2), respectively.