一种ISM 2.4GHz的低功耗低中频射频接收机前端

本文描述了一种工作在2.4GHz ISM频段的低功耗、低中频射频接收机前端电路,使用TSMC 0.13um CMOS工艺。整个前端包括一个低噪声放大器以及两次变频下变换混频器。低噪声放大器通过在输入级引入额外的栅-源电容实现了低功耗与低噪声的设计;在下变换混频器设计中,分别使用一个单平衡射频混频器以及两个双平衡低中频混频器实现两次变频下变换技术;射频混频器输入晶体管源极串联电感-电容谐振网络以及低噪声放大器输出级的电感-电容谐振网络总共实现了30dB的镜像抑制率。整个前端占用芯片面积约0.42mm2,在1.2V的供电电压下,仅耗功率4.5mW,实现了4dB的噪声系数,在高增益模式下,获得-22dBm的三阶交调线性度,整个链路电压增益为37dB。     

用于便携式GPS接收机中的5.4mW低噪声高增益CMOS射频前端电路设计

设计了应用于便携式GPS接收机射频前端中的CMOS低噪声放大器和正交混频器. 该电路中的低噪声放大器采用带源端电感负反馈的输入级,并引入功耗约束下的噪声和输入同时匹配技术. 正交混频器基于吉尔伯特单元. 电路采用TSMC 0.18μm RF CMOS工艺实现,总的电压转换增益为35dB,级联噪声系数为2.4dB,输入1dB压缩点为-22dBm,输入匹配良好,输入回损为-22.3dB, 在1.8V电压供电下,整个全差分电路功耗为5.4mW.     

应用于TD-SCDMA/LTE/LTE-Advanced收发机的多频多模CMOS射频接收前端电路设计

设计了应用于TD-SCDMA/LTE/LTE-Advanced收发机中的多频段、多模式射频接收前端电路. 该前端电路采用直接变频结构,包含两个可调谐差分低噪声放大器、一个正交混频器和两个中频放大器。其中,两个独立的可调谐低噪声放大器覆盖了4个射频频段,在较低的功耗下实现足够的增益和噪声性能. 并且利用开关电容阵列来调节低噪声放大器的谐振频率点. 低噪声放大器通过混频器的驱动级跨导晶体管实现结合。正交混频器采用折叠式双平衡吉尔伯特结构,利用PMOS晶体管作为本振信号的开关对,从而降低1/f噪声. 前端电路具有3种增益模式以获得更大的动态范围. 模式配置和频段选择功能都由片上的SPI模块控制. 该射频前端电路采用TSMC0.18um RF CMOS工艺实现,芯片面积为1.3 mm2. 全部频段上测量的转换增益高于43dB,双边带噪声系数低于3.5dB. 整个电路在1.8V供电电压下,消耗电流约31mA。     

用于便携式GPS接收机中的5.4mW低噪声高增益CMOS射频前端电路设计

设计了应用于便携式GPS接收机射频前端中的CMOS低噪声放大器和正交混频器.该电路中的低噪声放大器采用带源端电感负反馈的输入级,并引入功耗约束下的噪声和输入同时匹配技术.正交混频器基于吉尔伯特单元.电路采用TSMC 0.18μm RFCMOS工艺实现,总的电压转换增益为35dB,级联噪声系数为2.4dB,输入ldB压缩点为-22dBm,输入匹配良好,输入回损为-22.3dB,在1.8V电压供电下,整个全差分电路功耗为5.4mW.     

宽带低噪声放大器单片微波集成电路

从行波放大器设计理论出发,研制了一款基于低噪声GaAs赝配高电子迁移率晶体管(PHEMT)工艺设计的2~20 GHz单片微波集成电路(MMIC)宽带低噪声放大器。该款放大器由九级电路构成。为了进一步提高放大器的增益,采用了一个共源场效应管和一个共栅场效应管级联的拓扑结构,每级放大器采用自偏压技术实现单电源供电。测试结果表明,本款低噪声放大器在外加+5 V工作电压下,能够在2~20 GHz频率内实现小信号增益大于16 dB,增益平坦度小于±0.5 dB,输出P-1 dB大于14 dBm,噪声系数典型值为2.5 dB,输入和输出回波损耗均小于-15 dB,工作电流仅为63 mA,低噪声放大器芯片面积为3.1 mm×1.3 mm。     

低功耗单端输入差分输出低噪声放大器

该文设计了应用于无线局域网2.4GHz低噪声放大器(LNA),采用了SMIC0.18μm CMOS工艺技术和单端输入差分输出的电路结构.电路同时采用了双支路的电流复用技术,实现了低功耗、低噪声和高增益的性能;通过在输出级增加一级共栅级放大电路,有效地增加了电路的对称性;共源支路串联电感,解决了差分信号相位偏差问题.仿真结果表明,设计的LNA的噪声系数为1.76dB,增益为20.9dB,在1.8V电源电压下,功耗为8.5mW.     

S 频段pHEMT 双通道低噪声放大器芯片的设计

采用GaAs 0.13μmp HEMT MMIC流片工艺设计和制作了一种S频段双通道低噪声放大器芯片,芯片内部集成了两个低噪声放大器通道、一级单刀双掷(SPDT)开关和一个晶体管-晶体管逻辑(TTL)电平转换电路。低噪声放大器电路采用一级共源共栅场效应管(Cascode FET)结构实现,使其具有比单管更高的增益,简化了芯片拓扑,降低了芯片设计难度。经流片测试,在1.9~2.1GHz的工作频带内,芯片噪声系数优于1.4dB,增益大于22.5dB,输入驻波优于1.8,输出驻波优于1.4,输出1dB压缩点(P1dB)为10dBm。大量芯片样本在片测试统计数据表明该低噪声放大器成品率大于90%,性能指标优于目前同类商业芯片指标。     

220GHz低噪声放大器研究

基于IHP锗硅BiCMOS工艺,研究和实现了两种220 GHz低噪声放大器电路,并将其应用于220 GHz太赫兹无线高速通信收发机电路。一种是220 GHz四级单端共基极低噪声放大电路,每级电路采用了共基极（Common Base, CB）电路结构,利用传输线和金属-绝缘体-金属(Metal-Insulator-Metal, MIM)电容等无源电路元器件构成输入、输出和级间匹配网络。该低噪放电源的电压为1.8 V,功耗为25 mW,在220 GHz频点处实现了16 dB的增益,3 dB带宽达到了27 GHz。另一种是220 GHz四级共射共基差分低噪声放大电路,每级都采用共射共基的电路结构,放大器利用微带传输线和MIM电容构成每级的负载、Marchand-Balun、输入、输出和级间匹配网络等。该低噪放电源的电压为3 V,功耗为234 mW,在224 GHz频点实现了22 dB的增益,3 dB带宽超过6 GHz。这两个低噪声放大器可应用于220 GHz太赫兹无线高速通信收发机电路。     

一种共基差分低噪声放大器设计

在无线通信终端中,低噪声放大器是射频接收系统中的第一级有源电路,对系统性能有重要影响.在深入分析噪声的基础上,提出一种采用共基差分输入结构的低噪声放大器,电路包括可控增益放大器和增益控制电路.该结构的低噪声放大器的输出电压直接反映到自动增益控制电路的输入端,根据输出电压幅值的大小,自动增益控制电路的输出电压反馈到低噪声放大器的增益控制电路比较器的输入端,进而影响放大器的总体增益.基于JAZZ 0.35 μmBICMOS工艺设计放大器电路结构,并对电路进行了仿真和分析,结果表明设计的放大器可以更加有效地抑制噪声,低噪声放大器能提供25 dB的增益,噪声系数小于1 dB,灵敏度达到2μV.     

基于GaAs肖特基二极管的330GHz接收前端技术研究

基于GaAs肖特基二极管,设计实现了310~330 GHz的接收机前端.接收机采用330 GHz分谐波混频器作为第一级电路,为降低混频器变频损耗,提高接收机灵敏度,分析讨论了反向并联混频二极管空气桥寄生电感和互感,采用去嵌入阻抗计算方法,提取了二极管的射频、本振和中频端口阻抗,实现了混频器的优化设计,提高了变频损耗仿真精度.接收机的165 GHz本振源由×6×2倍频链实现,其中六倍频采用商用有源器件,二倍频则采用GaAs肖特基二极管实现,其被反向串联安装于悬置线上,实现了偶次平衡式倍频,所设计的倍频链在165 GHz处输出约10 dBm的功率,用以驱动330 GHz接收前端混频器.接收机第二级电路采用中频低噪声放大器,以降低系统总的噪声系数.在310~330 GHz范围内,测得接收机噪声系数小于10.5 dB,在325 GHz处测得最小噪声系数为8.5 dB,系统增益为(31±1)dB.     

Resolution Enhancement Technology:Integrated Process Solutions using OPC

DUV lithography, using the 248 nm wavelength, is a viable manufacturing option for devices with features at 130 nm and less. Given the low kl value of the lithography, integrated process development is a necessary method for achieving acceptable process latitude. The application of assist features for rule based OPC requires the simultaneous optimization of the mask, illumination optics and the resist.Described in this paper are the details involved in optimizing each of these aspects for line and space imaging.A reference pitch is first chosen to determine how the optics will be set. The ideal sigma setting is determined by a simple geometrically derived expression. The inner and outer machine settings are determined, in turn,with the simulation of a figure of merit. The maximum value of the response surface of this FOM occurs at the optimal sigma settings. Experimental confirmation of this is shown in the paper.Assist features are used to modify the aerial image of the more isolated images on the mask. The effect that the diffraction of the scattering bars (SBs) has on the image intensity distribution is explained. Rules for determining the size and placement of SBs are also given.Resist is optimized for use with off-axis illumination and assist features. A general explanation of the material' s effect is discussed along with the affect on the through-pitch bias. The paper culminates with the showing of the lithographic results from the fully optimized system.     

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.     

Theoretical analysis of the relationship between the Brillouin gain coefficient and the strain in the optical-fiber sensors

The relation between the power of the Brillouin signal and the strain is one of the bases of the distributed fiber sensors of temperature and strain. The coefficient of the Bfillouin gain can be changed by the temperature and the strain that will affect the power of the Brillouin scattering. The relation between the change of the Brillouin gain coefficient and the strain is thought to be linear by many researchers. However, it is not always linear based on the theoretical analysis and numerical simulation. Therefore, errors will be caused if the relation between the change of the Brillouin gain coefficient and the strain is regarded as to be linear approximately for measuring the temperature and the strain. For this reason, the influence of the parameters on the Brillouin gain coefficient is proposed through theoretical analysis and numerical simulation.     

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.     

Novel fiber-optical interferometer with miniaturized probe for in-hole measurements

Today, micro-system technology and the development of new MEMS （Micro-Electro-Mechanical Systems） are emerging rapidly. In order for this development to become a success in the long run, measurement systems have to ensure product quality. Most often, MEMS have to be tested by means of functionality or destructive tests. One reason for this is that there are no suitable systems or sensing probes available which can be used for the measurement of quasi inaccessible features like small holes or cavities. We present a measurement system that could be used for these kinds of measurements. The system combines a fiber optical, miniaturized sensing probe with low-coherence interferometry, so that absolute distance measurements with nanometer accuracy are possible.     

Study of waveguide coupling efficiency in hybrid silicon lasers

This paper presents a new method to increase the waveguide coupling efficiency in hybrid silicon lasers. We find that the propagation constant of the InGaAsP emitting layer can be equal to that of the Si resonant layer through improving the design size of the InP waveguide. The coupling power achieves 42% of the total power in the hybrid lasers when the thickness of the bonding layer is 100 nm. Our result is very close to 50% of the total power reported by Intel when the thickness of the thin bonding layer is less than 5 nm. Therefore, our invariable coupling power technique is simpler than Intel＇s.     

Teleportation of an arbitrary unknown N-qubit entangled state under the controlling of M controllers

A new quantum protocol to teleport an arbitrary unknown N-qubit entangled state from a sender to a fixed receiver under M controllers(M < N) is proposed. The quantum resources required are M non-maximally entangled Greenberger-Home-Zeilinger (GHZ) state and N-M non-maximally entangled Einstein-Podolsky-Rosen (EPR) pairs. The sender performs N generalized Bell-state measurements on the 2N particles. Controllers take M single-particle measurement along x-axis, and the receiver needs to introduce one auxiliary two-level particle to extract quantum information probabilistically with the fidelity unit if controllers cooperate with it.     

Diode-end-pumped Nd:YVO4/LBO lasers with 4.2W continuous-wave output at 457 nm

A continuous-wave (CW) 457 nm blue laser operating at the power of 4.2 W is demonstrated by using a fiber coupled laser diode module pumped Nd: YVO4 and using LBO as the intra-cavity SHG crystal With the optimization of laser cavity and crystal parameters, the laser operates at a very high efficiency. When the pumping power is about 31 W, the output at 457nm reaches 4.2 W, and the optical to optical conversion efficiency is about 13.5% accordingly. The stability of the out putpower is better than 1.2% for 8 h continuously working.     

A rigorous proof of MIMO channel capacity’s increase with antenna number

It is well known that adding more antennas at the transmitter or at the receiver may offer larger channel capacity in the multiple-input multiple-output（MIMO） communication systems. In this letter, a simple proof is presented for the fact that the channel capacity increases with an increase in the number of receiving antennas. The proof is based on the famous capacity formula of Foschini and Gans with matrix theory.     

Call for Papers

正Wireless Body-area Networks The last decade has witnessed the convergence of three giant worlds:electronics,computer science and telecommunications.The next decade should follow this convergence in most of our activities with the generalization of sensor networks.In particular with the progress in medicine,people live longer and the aging of population will push the development of wireless personal networks