非掺杂AlGaN/GaN HEMT微波功率器件

介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果. 制作了几种0.6μm栅长、100～1000μm不同栅宽的器件，对于栅宽分别为100, 300和500μm的器件，典型最大跨导为190～170mS/mm；截止频率比较相近，大约为24GHz；而最高振荡频率随栅宽增加而降低，分别为56, 46和40GHz. 测试了8GHz频率时，不同工作条件下1000μm栅宽器件的连续波微波功率特性：Vds=17V, Id=310mA, Pin=25.19dBm时，Po=30dBm (1W) ,Ga=4.81dB; Vds=18V, Id=290mA, Pin=27dBm时，Po=31.35dBm (1.37W) ,Ga=4.35dB.     

非掺杂AlGaN/GaN HEMT微波功率器件

介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果.制作了几种0.6μm栅长、100～1000μm不同栅宽的器件,对于栅宽分别为100,300和500μm的器件,典型最大跨导为190～170mS/mm;截止频率比较相近,大约为24GHz;而最高振荡频率随栅宽增加而降低,分别为56,46和40GHz.测试了8GHz频率时,不同工作条件下1000μm栅宽器件的连续波微波功率特性:Vds=17V,Id=310mA,Pin=25.19dBm时,Po=30dBm(1W),Ga=4.81dB;Vds=18V,Id=290mA,Pin=27dBm时,Po=31.35dBm(1.37W),Ga=4.35dB.     

非掺杂AlGaN/GaN HEMT微波功率器件

介绍了非掺杂GaN HEMT微波功率器件的结构、制造工艺和测试结果.制作了几种0.6μm栅长、100～1000μm不同栅宽的器件,对于栅宽分别为100,300和500μm的器件,典型最大跨导为190～170mS/mm;截止频率比较相近,大约为24GHz;而最高振荡频率随栅宽增加而降低,分别为56,46和40GHz.测试了8GHz频率时,不同工作条件下1000μm栅宽器件的连续波微波功率特性:Vds=17V,Id=310mA,Pin=25.19dBm时,Po=30dBm(1W),Ga=4.81dB;Vds=18V,Id=290mA,Pin=27dBm时,Po=31.35dBm(1.37W),Ga=4.35dB.     

高功率附加效率的InGaP/GaAs功率HBT

采用发射极-基极金属自对准工艺,成功研制出了InGaP/GaAs功率HBT.发射极尺寸为(3μm×15μm)×16的功率器件的截止频率和最高振荡频率分别为55GHz和35GHz.在片load-pull测试表明:当工作频率为1GHz时,器件工作在AB类,该功率管最大输出功率为23.5dBm,最大功率附加效率达60%,P1dB的输出功率为21dBm,对应增益为16dB,工作电压为3.5V.     

75 GHz 13.92 dBm InP DHBT 共射共基功率放大器

报道了基于InP基双屏质结双板晶体管(DHBT)工艺的四指共射共基75 GHz微波单片集成(MMIC)功率放大器,器件的最高振荡频率fmax为150 GHz.放大器的输出极发射极面积为15μm×4μm.功率放大器在75 GHz时功率增益为12.3 dB,饱和输出功率为13.92 dBm.放大器在72.5 GHz处输入为2 dBm时达到最大输出功率14.53 dBm.整个芯片传输连接采用共面波导结构,芯片面积为1.06 mm×0.75 mm.     

漏源间距对AlGaN/GaN HEMT器件特性的影响

采用相同的欧姆接触,栅长为100 nm的T型栅以及50 nm的氮化硅(SiN)表面钝化等器件工艺,制备了漏源间距分别为2和3μm的AlGaN/GaN高电子迁移率场效应晶体管(HEMT).研究发现,当漏源间距从2μm增加至3μm后,器件的直流特性略有下降,如在Vgs为1V下的饱和电流密度从1.4 A/mm下降至1.3 A/mm.此外,器件的射频特性也略有下降,电流增益截止频率(fT)从121 GHz降至116 GHz,最大振荡频率(fmax)从201 GHz下降至189 GHz.然而,器件的击穿特性却有显著提升,击穿电压从44 V提升至87 V.在实际器件设计制备过程中可考虑适当增加漏源间距,在保持直流和射频特性的前提下,提升器件的击穿特性.     

0.18 μm射频SOI LDMOS功率器件的研究

在提出0.18μm射频SOI LDMOS功率器件研究方法的基础上,对工艺进行了设计,并制备了栅宽为1 200μm,栅长为0.7μm,漏的注入区与栅的距离为1.5μm的0.18μm射频SOILDMOS功率器件。对器件进行了测试和模拟,在工作频率为3 GHz,直流偏置电压VDS为3 V,VGS为1.5 V,输入功率Pin为5 dBm时,Pout、增益和PAE分别为15 dBm1、0 dB和35%。     

高功率附加效率的InGaP/GaAs功率HBT

采用发射极基极金属自对准工艺，成功研制出了InGaP/GaAs功率HBT．发射极尺寸为(3μm×15μm)×16的功率器件的截止频率和最高振荡频率分别为55GHz和35GHz．在片load-pull测试表明：当工作频率为1GHz时，器件工作在AB类，该功率管最大输出功率为23.5dBm，最大功率附加效率达60%，P1dB的输出功率为21dBm，对应增益为16dB，工作电压为3.5V．     

光纤无线通信系统中用高非线性光纤实现全光频率上转换

研究了一种基于高非线件光纤(HNLF)中交叉相位调制效应的全光频率上转换射频耦合到光纤无线通信(ROF)系统.数值计算结果表明,由于交叉相化调制引起的调制不稳定性.波长1.54μm,重复频率为40 GHz的抽运光可使波长为1.56μm,载有速率为2.5 Gbit/s的非归零码作为下行链路数据的弱信号光光波分裂,产生与载波距离为40 GHz且与载波相干的两个一阶调制边带,抽运光脉宽、抽运光功率和光纤长度对载波与边带功率差有较大影响.仿真实验结果证实了以上原理,速率为2.5 Gbit/s的数据信号在高非线性光纤中被上转换到40 GHz毫米波上.信号光功牢为0 dBm时,得到的优化光纤长度为600 m,抽运光功率为17 dBm.     

110～200GHz频段InP单行载流子光电二极管

设计制备了一种基于InP材料低偏压工作的单行载流子光电二极管(UTC-PD),该器件的工作频率范围为110～200 GHz。为提升器件的带宽特性，UTC-PD芯片的吸收层采用p型高斯掺杂的InGaAs材料，芯片的InP衬底减薄至12μm。UTC-PD采用背照式的方式输入光信号。通过倒装焊的形式将芯片安装在厚度为50μm的AlN基片上的共面波导焊盘上进行测试。在-3 V偏压和1.55μm波长输入光条件下，制备器件的响应度超过0.2 A/W;在110 GHz处获得最高输出功率为-5.6 dBm, 197.83 GHz处的输出功率最低为-10.6 dBm。     

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.     

Electronic Structure of Semiconductor Nanocrystals

This paper reviews our recent development of the use of the large-scale pseudopotential method to calculate the electronic structure of semiconductor nanocrystals, such as quantum dots and wires, which often contain tens of thousands of atoms. The calculated size-dependent exciton energies and absorption spectra of quantum dots and wires are in good agreement with experiments. We show that the electronic structure of a nanocrystal can be tuned not only by its size,but also by its shape. Finally,we show that defect properties in quantum dots can be significantly different from those in bulk semiconductors.     

Critical Stage Rule-Based Real Time Dispatch（RTD）System in Highly-Mixed-Products （HMP） FAB

An improving utilization and efficiency of critical equipments in semiconductor wafer fabrication facilities are concerned. Semiconductor manufacturing FAB is one of the most complicated and cost sensitive environments. A good dispatching tool will make big difference in equipment utilization and FAB output as a whole. The equipment in this paper is In-Line DUV Scanner. There are many factors impacting utilization and output on this equipment group. In HMP environment one of the issues is changing of reticule in this area and idle counts due to load unbalance between equipments. Here we'll introduce a rule-based RTD system which aiming at decreasing the number of recipe change and idle counts among a group of scanner equipment in a high-mixed-products FAB.     

GaAsSb/InAlAs PA DHBTs Grown by Production MBE

The epi material growth of GaAsSb based DHBTs with InAlAs emitters are investigated using a 4 × 100mm multi-wafer production Riber 49 MBE reactor fully equipped with real-time in-situ sensors including an absorption band edge spectroscope and an optical-based flux monitor. The state-of-the-art hole mobilities are obtained from 100nm thick carbon-doped GaAsSb. A Sb composition variation of less than ± 0.1 atomic percent across a 4 × 100mm platen configuration has been achieved. The large area InAlAs/GaAsSb/InP DHBT device demonstrates excellent DC characteristics,such as BVCEO＞6V and a DC current gain of 45 at 1kA/cm2 for an emitter size of 50μm × 50μm. The devices have a 40nm thick GaAsSb base with p-doping of 4. 5 × 1019cm-3 . Devices with an emitter size of 4μm × 30μm have a current gain variation less than 2% across the fully processed 100mm wafer. ft and fmax are over 50GHz,with a power efficiency of 50% ,which are comparable to standard power GaAs HBT results. These results demonstrate the potential application of GaAsSb/InP DHBT for power amplifiers and the feasibility of multi-wafer MBE for mass production of GaAsSb-based HBTs.     

Noise character analysis and the restraint of self-pulsation laser diodes

We calculate the Langevin noise sources of self-pulsation laser diodes, analyze the effects of active region noise and saturable-absorption region noise on the power fluctuation as well as period fluctuation, and propose a novel method to restrain the noise effects. A visible SIMULINK model is established to simulate the system, The results indicate that the effects of noise in absorption region can be ignored; that with the increase of DC injecting current, the noise effects enhance power jitter, and nevertheless, the period jitter is decreased; and that with external sinusoidal current modulating the self-pulsation laser diode, the noise-induced power jitter and period jitter can be suppressed greatly. This work is valuable for clock recovery in all-optical network.     

High-quality single-crystal CdSe nanoribbons and their optical properties

Large-scale synthesis of single-crystal CdSe nanoribbons is achieved by a modified thermal evaporation method, in which two-step-thermal-evaporation is used to control CdSe sources＇ evaporation. The synthesized CdSe nanoribbons are usually several micrometers in width, 50 nm in thickness, and tens to several hundred micrometers in length. Studies have shown that high-quality CdSe nanoribbons with regular shapes can be obtained by this method. Room-temperature photolumines-cence indicates that the lasing emission at 710 nm has been observed under optical pumping （266 nm） at power densities of 25-153 kW/cm^2. The full width half maximum （FWHM） of the lasing mode is 0.67 nm     

Propagation of hermite-cosh-gaussian beams passing through ABCD optical system with an annular aperture

By using the expansion of the aperture function into a finte sum of complex Gaussian functions, the corresponding analytical expressions of Hermite-cosh-Gaussian beams passing through annular apertured paraxially and symmetrically optical systems written in terms of ABCD matrix were derived, and they could reduce to the cases with squared aperture. In a similar way, the corresponding analytical expressions of cosh-Gaussian beams through annular apertured ABCD matrix were also given. The method could save more calculation time than that by using the diffraction integral formula directly.     

Influence of polarization extinction ratio on distributed polarization coupling detection

Distributed polarization coupling in polarization-maintaining fibers can be detected by using a white light Michelson interferometer. This technique usually requires that only one polarization mode is excited. However, in practical measurement, the injection polarization direction could not be exactly aligned to one of the principal axes of the PMF, so the influence of the polarization extinction ratio should be considered. Based on the polarization coupling theory, the influence of the incident polarization extinction on the measurement result is evaluated and analyzed, and a method for distributed polarization coupling detection is developed when both two orthogonal eigenmodes are excited.     

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正Communications—VLSI Researches and industries of telecommunications have been growing rapidly in the last 20 years and will keep their high growing pace in the next decade.The involved researches and developments cover mobile communications,highway and last-mile broadband communication,domain specific communications,and emerging D2D M2M communications.Radio communication steps into its