一种通用雷达信号模拟器的设计与实现

提出了一种通用雷达信号模拟器的实现方法。该方法采用通用计算机产生雷达回波数据,利用打印机接口实现PC机向外设传送数据,采用D/A变换器产生模拟视频回波信号;它具有极大的灵活性和通用性,只要改变计算机的软件,就可以实现不同体制雷达回波的模拟,解决了硬件设计和软件算法中的关键技术问题。     

一种通用雷达信号模拟器的设计与实现

提出了一种通用雷达信号模拟器的实现方法。该方法采用通用计算机产生雷达回波数据,利用打印机接口实现PC机向外设传送数据,采用D／A变换器产生模拟视频回波信号,它具有极大的灵活性和通用性,只要改变计算机的软件,就可以实现不同体制雷达回皮的模拟,解决了硬件设计和软件算法中的关键技术问题。     

通用搜索雷达模拟器的设计

介绍了通过软件和硬件相结合的办法，实现多体制多频段搜索雷达信号和处理的模拟。该模拟器通过设置和加载不同体制的雷达参数和软件，采用灵活的数字波形产生方式形成数字基带信号，经混频放大形成射频小信号，再通过方向图模拟形成不同形式的雷达回波信号，从而实现通用搜索雷达的模拟。仿真证明该模拟器是可行的。     

一种非相参雷达回波信号模拟器的设计

分析雷达回波特性,从非相参信号模拟开始,提出一种雷达回波模拟器的实现方法。该方法可以利用已知或计算机产生的目标信息运算获得回波信号数据,通过FPGA或DSP芯片控制DDS产生中频回波信号。这种方法具有极大的灵活性和通用性,只要改变计算机回波信号计算模型或参数,即可实现不同回波信号的模拟。     

机载相控阵雷达信号模拟器的设计

介绍了一套基于PC机和通用DSP芯片结构的机载相控阵雷达信号模拟器,该模拟器采用软硬件相结合的方法,由计算机根据雷达工作参数预先设定并计算目标、杂波数据,然后将数据加载到硬件电路中,硬件电路实时合成雷达回波信号。信号输出形式包括数字信号、视频信号、射频信号和天线信号。     

基于高速数模转换器的通用雷达信号模拟器的设计

针对雷达设计调试困难的问题,提出一种通用雷达信号模拟器的设计方案,以一个FPGA和两个高速DA芯片为核心,另外配置大容量存储器.目标及环境数据采用DDS方法产生或通过外部接口加载,再经过DAC输出雷达回波信号,供雷达信号处理机调试使用,文中给出了模拟器应用实例.     

雷达目标回波数字模拟的TMS320C6201实现

雷达信号模拟器是数字模拟技术与雷达技术相结合的产物,他通过模拟的方法产生机载雷达回波信号,以便在实际雷达系统不进行试飞的条件下,对雷达系统进行调试。特别是现代雷达功能越来越复杂,对其各部分及系统的调试和测试变得越来越困难,外场试飞实验和调试成本高,因此,研制雷达信号模拟器是非常必要的。而且,随着电子干扰与反干扰技术的迅速发展,如何测试和评估电子干扰与反干扰效果也逐渐成了一个难题。通过雷达信号模拟器,可以在模拟的雷达回波中加入各种类型的干扰,因而可以方便地对雷达的抗干扰能力进行全面测试。介绍了一种新的机载相控阵雷达视频信号模拟器中目标信号的模拟方法和基于TMS320C6201的硬件实现。该模拟器采用软硬件相结合的方法,由计算机根据雷达工作参数预先设定并计算目标数据,然后将数据加载到硬件电路中,硬件电路实时合成视频雷达回波信号并输出。     

一种新的机载相控阵雷达杂波模拟及实现

论述了一种新的机载相控阵雷达视频信号模拟器中杂波信号的模拟方法和基于TMS320C6201的硬件实现,该模拟器采用软硬件相结合的方法,由计算机根据雷达工作参数预先并计算、杂波数据,然后将数据加载到硬件电路中,硬件电路实时合成视频雷达回波信号并输出。     

基于CPCI总线的通用雷达回波信号模拟器

为了在实验室环境下对雷达信号处理系统进行调试和工作效能测试，设计了一种基于紧凑型外部设备互联总线（CPCI）和现场可编程门阵列技术的通用雷达回波信号模拟器，利用MATLAB的强大仿真功能，模拟产生各种体制雷达的回波信号数据，通过CPCI总线把它们写入该信号模拟器的同步动态随机存储器中，雷达信号处理模块再从该模拟器中反复读出数据进行处理，从而调试和检测雷达信号处理模块在各种杂波及无源干扰条件下对目标的处理。结果证明，该模拟器具有良好的通用性和精确度，并且运行可靠。     

一种通用雷达回波模拟器的设计与实现

介绍了一种基于直接数字波形合成技术的通用雷达回波模拟器。通过加载数据波形，该模拟器可以实现波形数据回放，也可产生各种标准信号波形。该模拟器以FPGA为控制核心，利用大容量FLASH作为数据存储介质，在接口通用性、控制逻辑重配置和器件兼容性3个方面作了专门设计。该模拟器具有良好的通用性和友好的用户交互接口，给出了本模拟器所模拟的面目标成像结果和产生的Chirp信号脉压结果。     

Development of the readout system for waveguide multilayer optical card

Waveguide multilayer optical card （WMOC） is a novel storage device of three-dimensional optical information. An advanced readout system fitting for the WMOC is introduced in this paper. The hardware mainly consists of the light source for reading, WMOC, motorized stages addressing unit, microscope imaging unit, CCD detecting unit and PC controlling ＆ processing unit. The movement of the precision motorized stage is controlled by the computer through Visual Basic （VB） language in software. A control panel is also designed to get the layer address and the page address through which the position of the motorized stages can be changed. The WMOC readout system is easy to manage and the readout result is directly displayed on computer monitor.     

Nanoimprint Lithography -A Next Generation High Volume Lithography Technique

IntroductionNanoimprint Lithography is a well-acknowl-edged low cost, high resolution, large area pattern-ing process. It includes the most promising methods,high-pressure hot embossing lithography (HEL) [2],UV-cured imprinting (UV-NIL) [3] and micro contactprinting (m-CP, MCP) [4]. Curing of the imprintedstructures is either done by subsequent UV-lightexposure in the case of UV-NIL or by cooling downbelow the glass transition temperature of the ther-moplastic material in case of HEL…     

Collinear phase-matching study of terahertz-wave generation via difference frequency mixed in GaAs and Inp

The collinearly phase-matching condition of terahertz-wave generation via difference frequency mixed in GaAs and InP is theoretically studied. In collinear phase-matching, the optimum phase-matching wave hands of these two crystals are calculated. The optimum phase-matching wave bands in GaAs and lnP are 0.95-1.38μm and 0.7-0.96μm respectively. The influence of the wavelength choice of the pump wave on the coherent length in THz-wave tuning is also discussed. The influence of the temperature alteration on the phase-matching and the temperature tuning properties in GaAs crystal are calculated and analyzed. It can serve for the following experiments as a theoretical evidence and a reference as well.     

Effects of the alloy compositions on the phonon-polaritons in ternary mixed crystals

Composition dependence of bulk and surface phonon-polaritons in ternary mixed crystals are studied in the framework of the modified random-element-isodisplacement model and the Bom-Huang approximation. The numerical results for Several Ⅱ - Ⅵ and Ⅲ- Ⅴ compound systems are performed, and the polariton frequencies as functions of the compositions for ternary mixed crystals AlxGa1-xAs, GaPxAS1-x, ZnSxSe1-x, GaAsxSb1-x, GaxIn1-xP, and ZnxCd1-xS as examples are given and discussed. The results show that the dependence of the energies of two branches of bulk phonon-polaritons which have phonon-like characteristics, and surface phonon-polaritons on the compositions of ternary mixed crystals are nonlinear and different from those of the corresponding binary systems.     

Influence of PVK ： NPB hole transporting layer on the characteristics of organic light-emitting devices

A doping system consisting of NPB and PVK is employed as a composite hole transporting layer （CHTL）. By adjusting the component ratio of the doping system, a series of devices with different concentration proportion of PVK ： NPB are constracted. The result shows that doping concentration of NPB enhances the competence of hole transporting ability, and modifies the recombination region of charge as well as affects the surface morphology of doped film. Optimum device with a maximum brightness of 7852 cd/m^2 and a power efficiency of 1.75 lm/W has been obtained by choosing a concentration proportion of PVK ： NPB at 1：3.     

New insert layer structure OLEDs

An insert layer structure organic electroluminescent device（OLED） based on a new luminescent material （Zn（salen）） is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn（salen）/Liq/LiF/A1/CuPc/NPD/Zn（salen）/Liq/LiF/A1. Effective insert electrode layers comprising LiF（1nm）/Al（5 nm） are used as a single semitransparent mirror, and bilayer cathode LiF（1 nm）/A1（100 nm） is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.     

Analysis of error performance on Turbo coded FDPIM

Due to variable symbol length of digital pulse interval modulation（DPIM）, it is difficult to analyze the error performances of Turbo coded DPIM. To solve this problem, a fixed-length digital pulse interval modulation（FDPIM） method is provided. The FDPIM modulation structure is introduced. The packet error rates of uncoded FDPIM are analyzed and compared with that of DPIM. Bit error rates of Turbo coded FDPIM are simulated based on three kinds of analytical models under weak turbulence channel. The results show that packet error rate of uncoded FDPIM is inferior to that of uncoded DPIM. However, FDPIM is easy to be implemented and easy to be combined, with Turbo code for soft-decision because of its fixed length. Besides, the introduction of Turbo code in this modulation can decrease the average power about 10 dBm, which means that it can improve the error performance of the system effectively.     

A method for calculating the center position of collimated light

It is a key problem to accurately calculate beam spots＇ center of measuring the warp by using a collimated laser. A new method, named double geometrical center method （DGCM）, is put forward for the first time. In this method, a plane wave perpendicularly irradiates an aperture stop, and a charge couple device （CCD） is employed to receive the diffraction-beam spots, then the geometrical centers of the fast and the second diffraction-beam spots are calculated respectively, and their mean value is regarded as the center of datum beam. In face of such adverse instances as laser intension distributing defectively, part of the image being saturated, this method can still work well. What＇s more, this method can detect whether an unacceptable error exits in the courses of image receiving, processing and calculating. The experimental results indicate the precision of this method is high.     

Preparation and Characterization of TaN ALD Precursors

High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET ＞ PDMAT ＞ TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.     

Curved crystal spectrometer for the measurement of X-ray lines from laser-produced plasmas

In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal （200） （2d = 0.4027 nm） is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line（w）, the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line（x）, the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines（y）, the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line（z） in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line（q） in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution（λ/△ 2） is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.