真空高阻区熔Si单晶中的微缺陷及其少子寿命

通过在Ar气氛及真空环境中进行的高阻区熔Si单晶生长实验,分析了晶体直径、晶体生长环境及晶体生长速率对晶体中微缺陷及少子寿命的影响及产生这种影响的原因.单晶生长实验表明,与在Ar气氛下的单晶生长相比,在真空环境下采用较低的晶体生长速率即可生长出无漩涡缺陷的单晶,而当晶体生长速度较高时,尽管可以消除漩涡,但单晶的少子寿命却有明显的下降.     

高阻真空区熔硅单晶的生长

介绍了高阻真空区熔硅单晶的研制工艺,研制出了导电类型为p型,电阻率(3～5)×103 Ω·cm及(1～2)×104Ω·cm两种规格的真空区熔硅单晶,其中电阻率(3～5)×103Ω·cm规格单晶的研制除需要进行真空区熔提纯外,还要进行微量的p型区熔掺杂.单晶直径30～35 mm,晶向〈111〉.经检测无位错及漩涡缺陷,单晶的少数载流子寿命达到1500μs以上.     

直拉区熔联合法硅单晶生长技术研究

通过直拉工艺生长直径60 mm的N型100单晶,之后以该单晶作为原料,采用区熔工艺生长成50 mm(2英寸)N型111单晶,单晶的电阻率为2.71~5.35Ω·cm,少子寿命为500~750μs,氧碳含量均低于1×16 cm-3。实验表明,通过直拉工艺和区熔工艺联合方式研制的低阻硅单晶具有电阻率控制准确、氧碳含量低、工艺易于实施等特点。同时,对直拉区熔联合法生长单晶的技术特点进行了探讨。     

直径52～65mm探测器级Si单晶的真空制备

为了制备纯度11N以上、直 径Φ大于 45mm并且各项性能指标满足探测器级要求的大直径 超高纯单晶Si材料,本文在真空气氛下提纯并生长Φ52～65mm探测器级区熔(FZ,float zone)Si单晶, 并对真空气氛和直径增加所带来的晶体不稳定生长、高断面电阻率不均匀率和漩涡缺陷 等问题的产生原因和解决方式进行了深入研究。结果表明,丹麦加热线圈表面带有台阶 和十字开口,是提纯和生长Φ大于45mm 多晶Si和单晶Si的理想线圈;适当提高单晶转速和 生长速度有利于降低断面电阻率不均匀率,且提高转速的效果更加明显;真空气氛下, 提高热场对中性可抑制漩涡缺陷的产生,其对漩涡缺陷的影响比单晶Si生长速度更加显 著,这是与Ar气气氛FZ不同的;多晶Si提纯次数越多单晶Si寿命越低,降低多晶Si原 料中的P/B和重金属原始含量有利于提高单晶Si寿命;若要制备少子寿命大于800μs, 符合探测器级标准的Φ52～65mm Si单晶 ,多晶Si原料少子寿命应大于3000μs。     

中子嬗变掺杂(NTD)硅单晶在压阻传感器中的应用

半导体器件用的硅单晶,通常是在直拉或区熔时从外部引入杂质制备的,即在硅单晶体生长时掺入所需杂质.因此,在掺杂时,由于杂质在硅中的分凝效应,导致掺入杂质分布的不均匀,再加上拉晶工艺因素的影响,使硅单晶产生杂质条纹等缺陷,使单晶在轴向和径向都会有较大的掺杂分布起伏,导致单晶电阻率的非均匀性.对大直径、高电阻率的硅单晶电阻率的不均匀性更为突出.硅压阻传感器对硅单晶电阻率的均匀性同样有较高的要求,如果原始单晶电阻率均匀性     

生长系统对高阻区熔硅单晶径向电阻率变化的影响

分别采用L4375-ZE区熔炉和CFG/1400P区熔炉,生长了N型、(1.5～4.5)×103Ω.cm和P型、(1.0～5.0)×104Ω.cm两种规格的高阻区熔硅单晶,单晶的直径为52～54 mm,晶向为<111>。经对单晶的电阻率及其径向分布进行检测对比后发现,在加热线圈几何结构(包括上下表面角度、内径尺寸及台阶设计)基本相同、单晶生长速率相同且上、下晶轴旋转具有相同配置的情况下,不同的单晶生长系统所生长的单晶,其电阻率径向均匀性有明显差异,用L4575-ZE区熔炉生长的单晶的电阻率径向分布更均匀。     

微波反射光电导衰退技术在InGaAs台面结器件工艺中的应用

微波反射光电导衰退法是一种非接触式的半导体材料少子寿命表征手段,本文用微波反射光电导衰减法测试了台面InGaAs光电器件制备中各单项工艺(刻蚀、腐蚀、硫化)中InCaAs样品的少子寿命分布,结果表明,离子刻蚀使得样品少子寿命降低,非均匀性增大,而湿法腐蚀能够在一定程度上修复离子刻蚀带来的损伤,损伤区域中心的少子寿命增大,寿命分布也更加均匀,硫化钝化能够进一步提高损伤区域少子的寿命,却使寿命分布均匀性变差.可见,微波反射光电导衰减法可以简单无损地得到样品少子寿命分布,对工艺改进具有重要的指导意义.     

线圈台阶对区熔硅单晶生长影响的数值计算分析

悬浮区熔法是生长硅单晶的重要方法之一,线圈形状作为主要的工艺参数直接影响能量分布并最终决定硅单晶的生长情况.通过有限元法对区熔硅单晶生长进行数值模拟,考虑二维轴对称情况下由高频线圈产生的电磁场对熔区产生的影响,主要对比分析了线圈上方有无台阶对单晶生长的不同影响.同时结合相应的试验结果及现象,得到了线圈台阶的引入提高了晶体成晶的质量.     

φ200mm太阳能电池用直拉硅单晶生长中导流系统的研究

利用数值模拟,对CZ硅单晶生长系统中导流系统调整和改进,得到不同导流系统下的氩气流场和全局温场. 研究发现在导流系统中引入导流筒及冷却功能后,氩气流场得到明显的改善,晶体中纵向温度梯度均匀性改善,固液界面趋于平坦,有利于结晶潜热的散发和单晶径向电阻率的均匀性. 研究表明改进导流系统能提高结晶潜热散发速率,有利于提高晶体拉速.     

微波反射光电导衰退技术在InGaAs台面结器件工艺中的应用

微波反射光电导衰退法是一种非接触式的半导体材料少子寿命表征手段，本文用微波反射光电导衰减法测试了台面InGaAs光电器件制备中各单项工艺(刻蚀、腐蚀、硫化)中InCaAs样品的少子寿命分布，结果表明，离子刻蚀使得样品少子寿命降低，非均匀性增大，而湿法腐蚀能够在一定程度上修复离子刻蚀带来的损伤，损伤区域中心的少子寿命增大，寿命分布也更加均匀，硫化钝化能够进一步提高损伤区域少子的寿命，却使寿命分布均匀性变差。可见，微波反射光电导衰减法可以简单无损地得到样品少子寿命分布，对工艺改进具有重要的指导意义。     

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.