抛物形量子阱的共振隧穿

文中通过求解薛定谔方程得到抛物型形量子阱的变换矩阵与透射系数。利用这一结果计算透射系数可以达到任意高的精度，最后，讨论了结构变化对抛物型量子阱的共振隧穿的影响。     

电子隧穿问题的数值算法

文中给出了计算电子隧穿问题的一种新的数值方法，该方法适用于任意形状的一维势垒。在该算法中，首先用Ｎｕｍｅｒｏｖ算法注解薛定谔方程，然后再利用所得结果计算电子透射系数，为检测算法的精度，计算了电子对矩形双势垒及三角形势垒的透射系数，并与相应的精确解做了比较，结果表明该方法具有很高的精度。     

半导体技术

TN301 98040264多抛物t子阱的共振隧穿/李存志,刘云鹏,罗恩泽(西安电子科技大学)才西安电子科技大学学报·一1997,24(4).一544~548通过求解薛定谬方程得到多抛物量子阱的变换矩阵和透射系数。利用这一结果计算透射系数可以达到任意高的精度。最后讨论了抛物阱的个数对共振隧穿的影响。图2表z参5(金)该方法适用于任意形状的一维势垒。在该算法中,首先用Nl:111。1’()v算法求解薛定谬方程,然后再利用所得结果计算电子透射系数。为检验算法的精度,计算了电子对矩形双势垒及三角形势垒的透射系数,并与相应的精确解做了比较,结果表明该方法具有…     

一维光子晶体禁带结构的MATLAB分析计算

一维光子晶体禁带结构可以通过光子晶体的透射系数谱来分析.在计算光子晶体的透射系数时,根据不同介质界面处的连续性条件,将界面两侧的波函数展开为一个以矩阵方程描述的线性方程组,利用MATLAB提供的矩阵左除命令,即可获得光子晶体的透射系数谱.与其他方法例如递推法、转移矩阵法相比,该方法不需要花费较多精力编程,具有概念简单、...     

一维多势垒结构准束缚态的MATLAB分析计算

一维多势垒结构的准束缚态可以通过计算其透射系数的状态来分析.根据势垒与势阱界面的连续性条件,将界面两侧的波函数展开为一个以矩阵方程描述的线性方程组,利用MATLAB提供的矩阵左除命令,即可获得多势垒结构的透射系数.给出了通用计算程序,介绍了计算结果正确性的判断技巧.该方法不需要花费较多精力编程,具有概念简单、使用方便、...     

楔形发射体的电子场发射理论

本文提出楔形发射体的电子场发射理论并给出计算实例；该理论以单原子发射点假设为基础，用经典电动力学方法计算楔形发射体的隧道势垒，然后用Ｎｕｍｅｒｏｖ方法计算其透射系数，最后用到场发射体伏安特性。     

多层平板屏效计算中的等效传输线法

讨论了多层平板屏效计算中的等效传输线法。定义了不同传输线间的反射系数与透射系数,求出了反射系数和透射系数表达式。文中透射系数的定义是对传线基本理论的有益补充。     

多层双各向同性媒质中电磁波的传输特性

用不对称传输线模型分析了平面电磁波垂直入射于多层双各向同性媒质的反射和透射问题，导出了形式上较简单的计算多层双各向同性媒质界面反射和透射系数公式。为了便于和已有的文献结果相比较，给出计算实例，结果表明，用此公式得出的结果和文献结果一致，为计算多层双各向同性媒质的反射和透射带来方便；同时，对双各向同性媒质，非互易参数和手征参数的改变对反射和透射系数都有较大的影响。     

双轴各向异性介质特征参数的测试模型

介质参数测试的关键理论步骤是求解相应的电磁逆问题。本文利用等效传输线法导出了已知双轴各向异性电磁材料复介电常数张量ε^-和复磁导率张量μ^-，计算出反射系数和透射系数（正问题）的理论公式后，提出了一种新的求解逆问题的理论方法。由介质对正入射TE、TM波的反射系数与透射系数，可用公式直接反演得到ε^-和μ^-的复分量εx、μy和εy,μx然后利用介质对斜入射TE、TM波的透射系数由大为简化的反演算法迭代求解它们的z分量εz和μz。计算机模拟实验给出了比较理想的结果。     

光波在具有柱状结构的双折射薄膜中的传输特性

根据电磁场理论的矩阵分析方法推导了光波在具有柱状结构的双轴薄膜中的反射系数、透射系数和相位关系等光学特性.这些关系包含了界面处的多点反射,可以推广到一般的各向异性的多层膜系统.给出了各向同性入射媒质-双轴各向异性膜层-各向同性基底薄膜系统的计算结果,验证了该计算方法的可行性,为双折射多层膜结构及其器件的理论分析和设计提供了理论参考.     

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.