单级静态高峰值功率灯抽运脉冲Nd∶YAG固体激光器

报道了采用对称平面平行腔结构实现单级静态输出30 kW高峰值功率灯抽运Nd∶YAG固体激光器的研究结果。从速率方程出发,推导出脉冲Nd∶YAG固体激光器的单脉冲能量表达式,模拟出输出镜最佳透过率及最大输出能量。通过实验选取激光器工作的最佳参数,研制出一台高峰值功率灯抽运脉冲Nd∶YAG激光器,理论模拟和最佳实验结果基本一致。激光器在最大输入电压为800 V,脉宽为2 ms时,输出最大单脉冲能量60 J,最大峰值功率30 kW,光束质量M2为5.9,总体电光转换效率3.3%。在最大输入电压为800 V,脉宽为1.5 ms时最大平均功率405 W。采用该激光器切割6 mm低碳钢和4 mm不锈钢,在脉宽为2 ms,频率为6 Hz,峰值功率为30 kW时,切割4 mm不锈钢速度为1 mm/s,切割6 mm低碳钢速度为1.5~2 mm/s。     

基于中国典型地区大气模式的红外透过率变化特征

利用已经建立的通用大气辐射传输软件(CART)中嵌入的我国典型地区大气模式,分析了红外波段大气透过率随月份的变化特征,并分析了用国外模式近似可能带来的误差.结果分析表明:我国典型地区大气透过率随月份变化很大,夏季比冬季要小10%以上,相邻两个月之间的红外大气透过率之差可能达到10%左右;采用近似国外模式带来的误差可达到50%以上.这些结果进一步说明:在大气遥感、目标辐射测量、图像仿真和光电工程的设计与性能评估等方面的研究中,我国区域内的大气透过率的准确计算必须考虑我国的大气模式及月份.     

系统极零点与频率特性的关系

采用定量计算的方法,分析了单极点、单零点以及共轭极点、共轭零点对系统频率响应的影响.分析表明单极、零点时以及共轭极点、共轭零点位于特定区域时,系统频率响应的幅频峰值,谷值的频率与极、零点位置所在频率严格一致.通过对多极、零点系统幅频响应的分析得出结论,出现幅频峰值,谷值的频率相对极、零点位置所在频率可能有偏移,但是仍然可以说:极点所在频率位置附近频率响应幅度出现峰值,零点所在频率位置附近频率响应幅度出现谷点.     

峰值电流控制开关电源的反馈补偿问题研究

针对电流控制模式降压型开关电源芯片,探讨了输入电压的不同以及工作温度的差异造成对输出带负载能力和峰值电流的影响。在电流反馈回路的斜坡补偿模块中,加入随输入电压线性变化的基准电流源,以补偿不同输入电压对采样与斜坡补偿峰值电压造成的差异。此外,对反馈环中的比例电阻采用不同的工艺制作,通过电阻的温度系数补偿由采样电阻随温度变化所造成的采样电压的变化,减小温度对电路的带负载能力和峰值电流的影响。改进后,在相同环境温度下,4．7V到30V输入时,输出最大负载电流差异由2A降为0．5A。电阻改进后,从27℃到150℃,输出最大负载电流几乎不变。     

雷达回波A显在光栅上的实现

作为雷达回波的一种重要显示模式,A显是重要的目标识别辅助手段。本文介绍了采用SDRAM作为缓存存储器,利用大规模可编程逻辑器件进行控制和处理,在光栅显示器上实现雷达回波A显的一个设计实例。     

Quantitative Analysis of Main Components of Natural Gas Based on Raman Spectroscopy

Natural gas is composed of methane, ethane, propane, carbon dioxide, nitrogen, hydrogen, carbon monoxide and unknown alkane components of C4 or more (denoted as C4⁺) after desulfurization and dehydration treatment. The concentrations of the first seven components account for more than 90% of natural gas. When analyzing the natural gas composition using Raman spectral analysis methods, a small amount of unknown alkane components C4⁺ will have a negative impact on the analytical precision. In this work, a novel method that consists of an automatic decomposition algorithm of Raman spectra and a model for quantitative analysis was developed for the analysis of components of natural gas. The Raman spectrum of a natural gas sample could be decomposed into the sum of the Raman spectra of pure constituents and several Lorentz peaks by a nonlinear least-square optimization algorithm based on a linear additivity of Raman spectra. The concentration of the unknown alkane component C4⁺ was determined according to the area of the C-H deformation vibration peak which was common for most alkane molecules. Some training samples were used to establish the model between Raman characteristic peak areas and corresponding concentrations for each component. Compared with the existing Raman analysis methods, the new method solved the problem of analyzing natural gas containing unknown alkane components with good stability and accuracy. The experiments showed that the maximum absolute errors of this algorithm for methane, ethane, propane, carbon dioxide, nitrogen, hydrogen, and carbon monoxide respectively reached 0.57%, 0.37%, 0.21%, 0.07%, 0.18%, 0.04%, 0.13%, and the correlation coefficient to gas chromatographic results also reached 0.997, 0.986, 0.991, 0.998, 0.993, 1.000, 0.995, 0.982, respectively.     

110°C thermoluminescence glow peak of quartz — A brief review

The 110°C glow peak of quartz, though unstable at room temperature, has worked wonderfully in archaeology and retrospective dosimetry due to its pre-dose sensitization property. Various aspects of the peak, like its nature, defect centres involved, the impact of different stimuli and its application have been extensively studied. The main aims of this review are to (i) summarize briefly the work carried out on the various facets of this TL glow peak during the last four decades and (ii) identify the areas which need further attention in order to have a better understanding of the luminescence characteristics of this TL peak.      

纳米ZnO和ZnO-SiO2复合薄膜的光学性质研究

通过溶胶凝胶(sol-gel)法分别在玻璃衬底上制备了ZnO纳米薄膜和ZnO-SiO₂纳米复合薄膜,并利用紫外-可见光分光光度计对薄膜的光学性能进行了分析.可见光-紫外透射谱显示,随着ZnO溶胶浓度从0.7mol/L降低到0.006mol/L,制备的ZnO薄膜从只出现一个380nm(对应的光学禁带宽度为3.27eV)左右的吸收边到在380和320nm(对应的光学禁带宽度为3.76eV)左右各出现一个吸收边,并且随着ZnO溶胶浓度的降低,在380—320nm波段内的透过率明显提高.而Z 关键词： 纳米ZnO 2复合薄膜')" href="#">ZnO-SiO₂复合薄膜 溶胶凝胶法 透射率     

亚波长分形结构太赫兹透射增强的机理研究

利用太赫兹时域光谱(terahertz time domain spectroscopy,简称THz-TDS),研究了亚波长金属分形结构在THz波段的透射增强特性.分别从实验和理论两个方面,研究了铜箔上各级分形结构THz透射增强现象的产生机理.结果表明,在低频区的透射增强主要是由低级分形线中电子运动的共振引起的,而高频区的透射增强则主要由高级分形线中电子运动的共振引起的.从而将这种透射增强效应归结为分形结构中电子的共振辐射,即分形结构的局域共振效应. 关键词： 分形 太赫兹 透射 共振峰     

A novel simplified tone reservation combined with cross antenna rotation and inversion to reduce PAPR for MIMO‐OFDM system

In this paper, we first propose a simplified tone reservation (STR) method with low computational complexity which is based on the Fourier series expansion. Then, we analyze how to combine the STR method with the cross antenna rotation and inversion method to reduce the peak‐to‐average power ratio (PAPR) for multi‐input multi‐output orthogonal frequency division multiplexing (MIMO‐OFDM) system. To validate the analytical results, extensive simulations are conducted and the numerical results show the efficiency of the proposed schemes including the PAPR reduction and low computational complexity for MIMO‐OFDM system. Copyright © 2010 John Wiley & Sons, Ltd.