一种新型电荷泵电路的设计

文章提出了一种新的全差分电荷泵结构，与传统电荷泵电路相比，这个电路具有输出范围大和无跳跃现象的优点，同时还可以有效地解决电荷泄漏和充放电失配等问题。     

基于常数跨导轨到轨运算放大器的新型电荷泵

针对传统电荷泵电荷共享引起的输出电压波动、充放电电流失配引起的电路杂波问题,设计了一种新型电荷泵。该电荷泵电路采用常数跨导轨到轨运算放大器,降低了电荷共享引起的输出电压波动;采用基于全差分放大器的负反馈结构,解决了充放电电流失配的问题。基于SMIC 0.18 μm CMOS工艺,利用Cadence软件完成了电路的设计与仿真。结果表明,在0.5～1.5 V输出电压范围内,该电荷泵充放电电流失配小于2%;与传统电荷泵相比,该电荷泵输出电压的波动减小了1.5 mV,并且采用该电荷泵的锁相环输出频谱噪声减小了10 dB。     

一种采用LC谐振电路的高频差分有源电感

提出了一种采用LC并联谐振电路的新型差分有源电感,实现了宽的工作频带、高的Q值、较大的电感值和可调谐功能。采用无源电感和MOS晶体管可变电容构成LC谐振电路,减小了等效串联电阻和等效并联电容,在增大电感值、Q值的同时,扩大了工作频带。仿真结果表明,在2~7.6 GHz频率范围内,该新型差分有源电感的电感值大于26 nH,Q值大于138;在7.6 GHz高频下,电感值达130 nH,Q值达418,实现了宽工作频带范围内的高Q值和高电感值。与传统差分有源电感和带LC谐振电路的单端有源电感相比,该新型差分有源电感的性能较好。     

兼有高Q值、高电感值、高线性度的新型全差分有源电感

联合采用Cascode拓扑、电阻反馈网络和电流前馈技术,提出了一款兼有高Q值、高电感值、高线性度的可调谐的Cascode新型全差分有源电感。基于TSMC 0.18μm CMOS工艺,利用安捷伦公司的射频仿真工具ADS完成了有源电感的设计与仿真验证,应用Cadence Virtuoso工具完成了版图的绘制。结果表明,通过改变差分有源电感外加偏置,可以实现Q和电感值的可调,在1.2 GHz时Q值达到了最大值2 653,并且在此频率下电感值也高达15.563 n H,同时电感的线性度与没加电流前馈时相比提高了11.3 d BV。     

新型全差分电荷泵设计

采用差分输入和差分输出方案，设计了一种新型的全差分电荷泵。采用差分输出不仅能够降低电荷泄满所带来的电压噪声，而且能够提高电荷泵的上升和下降速度，从而提高锁相环的工作速度，还能增大输出电压的范围。在差分输入端，采用正反馈电路结构，以提高开启和关断速度，并降低功耗。上拉泵电路和下拉泵电路完全对称，能够消除电流失配所带来的噪声。     

用分布电容模型分析和优化差分电感

建立了预测片上等效寄生电容的片上电感分布电容模型.预测和解释了差分电感的自激振荡频率的差异.实测数据显示,与单端驱动模式下的相同对称电感相比,差分驱动模式电感提高最大品质因数127%,具有更大的工作频率范围.设计和验证了低寄生电容的差分电感.     

低失配GaAs HBT 1.5 bit高速模数转换器设计

介绍了一款基于GaAs HBT工艺的1 GS/s 1.5 bit模数转换器。通过分析模数转换器(ADC)的参考电压失配的来源,引入一种能提高电路对称性的新型差分参考网络架构,提出了减小失配的设计方法,显著提高了参考电平的对称性和一致性,从而减小参考电平的失配。此外,分析了比较器的静态和动态失配电压,对迟滞现象进行了解释。针对ADC的特点,详细分析了新型差分参考网络和比较器的关键设计参数。芯片实测结果表明,片内参考电平失配不超过1 mV,采样频率达到1 GS/s,功耗为350 mW。     

集成电感设计优化方法

分析了已有电感结构,提出了一种独特的高性能的优化方案,使得螺旋电感的品质因数和差分特性都有了显著的提高.该优化设计尤其适合高性能全差分压控振荡器对高性能螺旋电感的需要.选取典型的单层正方形螺旋电感作为测试对象,工作频率2.439 GHz,芯片面积最大值限定为250 μm×250 μm,最小线间距为5 μm.     

射频集成电路对称型螺旋电感研究

针对片上集成螺旋电感的建模,研究并设计了相关的优化方法。分析了已有电感结构,提出了一种高性能的优化方案,使螺旋电感的品质因数和差分特性都有了显著的提高,为螺旋电感设计中品质因数和电感值的折中提供更大的选择面。该优化设计尤其适合高性能全差分压控振荡器对高性能螺旋电感的需要;优化设计选取典型的单层螺旋电感作为测试对象,工作频率为2.439GHz,芯片面积最大值限定为250μm×250μm,采用ASITIC提供的默认工艺。     

采用Cascode拓扑和RC反馈网络的高Q差分有源电感

针对传统全差分有源电感在高频下品质因子Q较低的问题,联合使用Cascode拓扑和RC反馈网络对其进行优化。组合电路引入的双重负阻有效抵消了有源电感的寄生电阻,进而有效提高了高频下的Q值。基于Jazz 0.35 μm SiGe BiCMOS工艺,利用射频仿真软件ADS完成电路设计与仿真。仿真结果表明,在联合采用了Cascode拓扑和RC反馈网络后,在频率大于1 GHz时,有源电感的Q值明显提高;在1.3～3 GHz频率范围内,Q值均大于20;在2.1 GHz时,Q值达到最大值4 416,电感值变化范围为6.9～12 nH。     

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.     

Cost-effective test solutions for smart card and other integrated flash applications

From its emergence in the late 1980s as a lower cost alternative to early EEPROM technologies, flash memory has evolved to higher densities and speedsand rapidly growing acceptance in mobile applications.In the process, flash memory devices have placed increased test requirements on manufacturers. Today, as flash device test grows in importance in China, manufacturers face growing pressure for reduced cost-oftest, increased throughput and greater return on investment for test equipment. At the same time, the move to integrated flash packages for contactless smart card applications adds a significant further challenge to manufacturers seeking rapid, low-cost test.     

An improved parallel thinning algorithm with two subiterations

The parallel thinning algorithm with two subiterations is improved in this paper. By analyzing the notions of connected components and passes, a conclusion is drawn that the number of passes and the number of eight-connected components are equal. Then the expression of the number of eight-connected components is obtained which replaces the old one in the algorithm. And a reserving condition is proposed by experiments, which alleviates the excess deletion where a diagonal line and a beeline intersect. The experimental results demonstrate that the thinned curve is almost located in the middle of the original curve connectivelv with single pixel width and the processing speed is high.