B在SiGe中的应变补偿作用

用超高真空化学气相淀积方法生长出不同硼(B)掺杂浓度的应变SiGe合金材料,研究了B对SiGe合金的应变补偿作用.结果表明,B的掺入使SiGe的应变减小,B对Ge的应变补偿率为7.3,即平均掺入1个B原子可以补偿7.3个Ge原子引起的应变.同时获得B的晶格收缩系数为6.23×10-24cm3/atom.     

B在SiGe中的应变补偿作用

用超高真空化学气相淀积方法生长出不同硼(B)掺杂浓度的应变SiGe合金材料,研究了B对SiGe合金的应变补偿作用.结果表明,B的掺入使SiGe的应变减小,B对Ge的应变补偿率为7.3,即平均掺入1个B原子可以补偿7.3个Ge原子引起的应变.同时获得B的晶格收缩系数为6.23×10-24cm3/atom.     

用减压化学气相沉积技术制备应变硅材料

利用减压化学气相沉积技术，制备出应变Si/弛豫Si0.9Ge0.1/渐变组分弛豫SiGe/Si衬底. 通过控制组分渐变SiGe过渡层的组分梯度和适当优化弛豫SiGe层的外延生长工艺，有效地降低了表面粗糙度和位错密度.与Ge组分突变相比，采用线性渐变组分后，应变硅材料表面粗糙度从3.07nm减小到0.75nm，位错密度约为5E4cm-2，表面应变硅层应变度约为0.45%.     

氧化对SOI基SiGe薄膜残余应变弛豫的影响

研究了氧化对外延在SOI衬底上的SiGe薄膜的残余应变弛豫过程的影响.通过对SiGe薄膜采用不同工艺的氧化,从而了解不同氧化条件对SOI基SiGe薄膜的应变弛豫过程的影响.氧化将会促使SiGe薄膜中的Ge原子扩散到SOI材料的顶层硅中.而SiGe薄膜的残余应变弛豫过程将会与Ge原子的扩散过程同时进行,通过对SiGe薄膜和SOI顶层硅中位错分布的分析发现:在氧化过程中,SiGe薄膜和SOI衬底之间存在一个应力传递的过程.     

氧化对SOI基SiGe薄膜残余应变弛豫的影响

研究了氧化对外延在SOI衬底上的SiGe薄膜的残余应变弛豫过程的影响.通过对SiGe薄膜采用不同工艺的氧化,从而了解不同氧化条件对SOI基SiGe薄膜的应变弛豫过程的影响.氧化将会促使SiGe薄膜中的Ge原子扩散到SOI材料的顶层硅中.而SiGe薄膜的残余应变弛豫过程将会与Ge原子的扩散过程同时进行,通过对SiGe薄膜和SOI顶层硅中位错分布的分析发现:在氧化过程中,SiGe薄膜和SOI衬底之间存在一个应力传递的过程.     

干法氧化制备SiGe弛豫缓冲层及其表征

SiGe弛豫缓冲层是高性能Si基光电子与微电子器件集成的理想平台.通过1000℃干法氧化组分均匀的应变Si0.88Ge0.12层,在Si衬底上制备了表面Ge组分大于0.3,弛豫度大于95%,位错密度小于1.2×105cm-2的Ge组分渐变SiGe弛豫缓冲层.通过对不同氧化时间的样品的表征,分析了氧化过程中SiGe应变弛豫的主要机制.     

干法氧化制备SiGe弛豫缓冲层及其表征

SiGe弛豫缓冲层是高性能Si基光电子与微电子器件集成的理想平台.通过1000℃干法氧化组分均匀的应变Si0.88Ge0.12层,在Si衬底上制备了表面Ge组分大于0.3,弛豫度大于95%,位错密度小于1.2×105cm-2的Ge组分渐变SiGe弛豫缓冲层.通过对不同氧化时间的样品的表征,分析了氧化过程中SiGe应变弛豫的主要机制.     

用减压化学气相沉积技术制备应变硅材料

利用减压化学气相沉积技术,制备出应变Si/弛豫Si0.9Ge01/渐变组分弛豫SiGe/Si衬底.通过控制组分渐变SiGe过渡层的组分梯度和适当优化弛豫SiGe层的外延生长工艺,有效地降低了表面粗糙度和位错密度.与Ge组分突变相比,采用线性渐变组分后,应变硅材料表面粗糙度从3.07nm减小到0.75nm,位错密度约为5×104 cm-2,表面应变硅层应变度约为0.45%.     

用减压化学气相沉积技术制备应变硅材料

利用减压化学气相沉积技术,制备出应变Si/弛豫Si0.9Ge01/渐变组分弛豫SiGe/Si衬底.通过控制组分渐变SiGe过渡层的组分梯度和适当优化弛豫SiGe层的外延生长工艺,有效地降低了表面粗糙度和位错密度.与Ge组分突变相比,采用线性渐变组分后,应变硅材料表面粗糙度从3.07nm减小到0.75nm,位错密度约为5×104 cm-2,表面应变硅层应变度约为0.45%.     

压应变SiGe和张应变Si的能带结构研究

根据体Si和体Ge的能带结构特点,基于形变势理论,计算了SiGe合金的应变对其能级的影响。静压应变导致能级偏移,单轴应变导致简并能级分裂,使得应变SiGe合金的禁带宽度随应变的增加而减小。共度生长在体Si衬底上的SiGe合金,以及共度生长在体SiGe衬底上的Si,它们的禁带宽度随Ge组份的增加近乎线性减小。完全压应变的Si_(0.5)Ge_(0.5)合金,其禁带宽度从无应变时的0.93eV减小为0.68eV。Ge组份为0.5时,完全张应变的Si,其禁带宽度从无应变时的1.12eV减小为0.85eV。     

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.