盲源分离通信抗干扰技术与实践

针对宽频段压制干扰威胁以及频谱资源与通信抗干扰能力之间的固有矛盾，提出在扩谱抗干扰基础上增加统计域维度的方法，推动通信抗干扰由“硬抗”向“容扰”转变。盲源分离抗干扰技术利用通信信号和干扰信号的统计特性差异进行信号分离，可在不增加频谱资源条件下提高通信抗干扰能力。为认识和完善盲源分离抗干扰从理论算法到工程实践的发展过程，阐述盲源分离通信抗干扰技术的基本原理，重点介绍多通道盲源分离、单通道盲源分离等关键技术，分析盲源分离通信抗干扰技术的主要特点和存在的问题，最后指出该领域的发展重点。     

单通道混合信号盲分离算法

介绍了单通道混合信号的概念及盲源分离的现状,对实时线性混叠盲分离方法展开研究,分类探讨基于变换域滤波、多参数联合估计、符号序列与信道参数联合估计以及多维映射的单通道混合信号盲分离方法,分析比较各类盲源分离方法的处理对象、前提条件和优缺点,并进行了总结.最后通过仿真实验分析了基于粒子滤波与编码辅助的单通道盲分离方法中粒子数目、编码方式、源信号幅度比和频差等对分离算法性能的影响.     

基于EMD和ICA的单通道语音盲源分离算法

针对单通道语音信号盲分离的问题,结合盲源分离和经验模式分解的优点．提出了一种基于经验模式分解的单通道语音信号源数估计和盲源分离方法。对语音混合信号进行经验模式分解,利用贝叶斯算法估计语音源数目,根据源信号数目重组多通道语音混合信号,并采用独立分量分析实现语音信号的盲分离。仿真实验表明,使用此法能有效地估计通道语音信号源数和分离盲源。     

基于盲源分离的数字通信抗干扰技术

分析了现有数字通信抗干扰技术存在的局限性。在研究了盲源分离（Blind Source Separation,BSS）的理论基础上,介绍了一种基于盲源分离的数字通信抗干扰技术。建立了基于最大信噪比算法的盲源分离数字通信抗干扰传输模型,应用MATLAB仿真实现了2FSK通信信号与多种干扰信号的分离提取。仿真结果表明：应用基于盲源分离的抗干扰技术能够获得显著的抗干扰性能。     

基于最大比合并的超定盲源分离

主要研究了超定盲源分离问题,即观测信号个数大于源信号个数情况下的盲源分离.首先给出一种将超定分离转化为多组适定分离的方法,接着通过分析广义Rayleigh商问题最优解和基于四阶累积量代价函数收敛解之间的关系,提出了一种基于最大比合并(MRC)的盲源分离算法(MRC-FastICA).该算法利用多组FastICA来获得同一源信号的多个估计信号,然后利用MRC得到最终的分离信号.理论分析和实验结果表明该算法能够获得分集增益,比传统算法有更好的信干噪比(SINR)性能.     

基于盲源分离的雷达抗干扰技术研究

如何提高雷达的抗干扰能力一直是雷达信号处理的一大问题,问题的解决可以使雷达的检测和跟踪能力得以提高.在日趋复杂的信号环境下,传统的信号处理方法的局限性愈来愈大.本文通过对雷达信号处理过程和盲源分离技术的分析研究,提出采用基于高斯矩的ICA/BSS盲源分离方法进行雷达抗干扰信号处理.通过仿真试验结果证明基于盲源分离的雷达抗干扰处理方法是可行和令人满意的.     

混响环境下基于卷积模型的欠定盲源分离

为了提高盲源分离(blind source separation, BSS)算法在混响和噪声环境下的鲁棒性,提出了一种适用于欠定情况下用于卷积混合信号的盲源分离算法。在该算法中,利用高混响环境下混合模型即使在时频(time-frequency, TF)域中仍具有卷积特性,并结合房间冲激响应(room impulse response, RIR)的统计规律,将时频域中的瞬时模型扩展到更适合高混响环境的卷积模型,进而构建一欠定盲源分离优化问题,最后,采用交替方向乘子法(alternating direction method of multipliers, ADMM)优化框架来求解该问题。仿真实验结果表明:在混响环境下,本文提出的基于卷积模型的盲源分离算法与现有盲源分离算法相比,具有非常明显的性能优势。      

面向多路源信号的单通道盲去卷积算法研究

传统的单通道盲去卷积的方法存在仅能从混合信号中分离出2路源信号的局限,考虑到以上问题,该文提出一种基于优化的深度卷积生成对抗网络的单通道盲去卷积算法(SCBDC),能从1路混合信号中分离和解卷积出3路以上的独立源信号和混合矩阵.该文实验在汉字和遮挡图像数据集上进行,随机选择4路信号与混合矩阵进行卷积混合,实验结合峰值信...     

一种鲁棒的病态混叠信号欠定盲源分离算法

噪声环境下的病态混叠信号具有较强的空间复共线性,因此基于聚类的稀疏分量分析(SCA)方法难以在欠定条件下对其进行有效的分离。针对这一问题,该文首先建立了噪声环境下病态混叠信号欠定盲源分离问题的数学模型,分析了基于线性聚类的SCA方法在解决该问题时的局限性,提出了一种基于SCA和非正交联合对角化(NJD)的分离算法,该方法利用NJD不要求混叠矩阵为酉矩阵的特性,较好地解决了欠定盲源分离中的病态混叠问题。仿真实验表明,该方法在信号分离效果、噪声鲁棒性以及病态混叠鲁棒性上都明显优于基于启发式聚类粒子群优化的(CGPSO)的SCA方法。     

一种欠定盲源分离算法通用模型

针对传感器数目小于源信号数目的欠定情形,研究了基于压缩感知(CS)的欠定盲源分离(UBSS)问题。从欠定盲源分离和压缩感知的数学模型入手,在源信号具有稀疏性的前提下,将其转化为CS理论中的稀疏信号重构问题。在Sparco框架下建立了CS-UBSS两步法算法通用模型,并理论证明了该模型的有限等距特性(RIP)。仿真结果说明了该算法模型针对语音信号和图像信号的可行性与适用性,拓宽了UBSS问题的解决思路,尤其是CS理论中性能优越的重构算法可以直接应用于源信号的恢复。     

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.