无制冷高速直调1.5 μm AlGaInAs-InP DFB激光器

利用AlGaInAs-InP应变多量子阱(MQW)材料导带偏移量大的特点,制作了基于AlGaInAs-InP材料的无制冷脊波导分布反馈式(DFB)激光器.为提高器件调制速度,制作了2 μm宽的脊波导结构,并在脊波导两侧填充1.5 μm厚的SiO2层,从而有效降低器件寄生电容.室温条件下,DFB激光器典型阈值为15 mA,特征温度达88 K,边模抑制比大于50 dB,3 dB小信号调制响应带宽超过15 GHz.     

窄条AlGaAs激光器自脉动的研究及结构设计

阐述了窄条A1GaAs激光器自脉动现象产生的机理和条件,利用激光器的自脉动可以进行全光3R时钟提取,并研究改变激光器的结构参数对自脉动现象的影响规律。重点提出了一种在窄条AlGaAs激光器中加入量子阱结构的方法,通过仿真实验表明,该种含量子阱结构的窄条AlGaAs激光器能够提高输出光脉冲的频率和功率,减少输出光脉冲散光特性。     

混合光栅型的三段式自脉动DFB激光器

制作了1.55μm InGaAsP-InP三段式混合光栅型DFB激光器.观察到了20GHz左右的自脉动信号.讨论了自脉动的产生机制,并且对调相区所起的作用进行了研究.     

混合光栅型的三段式自脉动DFB激光器

制作了1.55μm InGaAsP-InP三段式混合光栅型DFB激光器.观察到了20GHz左右的自脉动信号.讨论了自脉动的产生机制,并且对调相区所起的作用进行了研究.     

新型分布反馈式气体激光器

本文论述了三种分布反馈(DFB)式气体激光器的理论及其首次实现的情况,这三种气体激光器是线性DFB激光器、螺旋DFB激光器和与二阶DFB效应相关的切向入射光栅式激光器。这些新型激光器是分别把线性周期金属波导、螺旋型金属波导以及带光栅的楔形金属波导应用到496μm光泵远红外CH_3F激光器上而实现的。螺旋DFB结构在激光研究上是一个新的概念,它引起人们的兴趣不仅在微波技术方面,同样在染料激光器和胆甾醇液晶的研究方面。DFB气体激光器未来研究的一个目标是实现10μm波长的CO_2 DFB激光器,它将具有很优异的特性和应用价值。     

窄条AlGaAs激光器自脉动现象研究

阐述了窄条AlGaAs激光器自脉动现象的产生机理和条件,分析了改变激光器的结构参数对自脉动现象的影响规律。提出了一种在窄条AlGaAs激光器中加入量子阱结构来提高窄条AlGaAs激光器的输出光脉冲频率和功率,减少输出光脉冲散光特性的方法。     

GaN基蓝紫光激光器的材料生长和器件研制

报道了国内首次研制成功的GaN基蓝紫光激光器的材料外延生长、器件工艺和特性.用MOCVD生长了高质量的GaN及其量子阱异质结材料,以及异质结分别限制量子阱激光器结构材料.GaN材料的X射线双晶衍射摇摆曲线(0002)对称衍射和(10(-1)2)斜对称衍射半宽分别为180″和185″;3μm厚GaN薄膜室温电子迁移率达到850cm2/(V·s).基于以上材料,分别成功研制了室温脉冲激射增益波导和脊型波导激光器,阈值电流密度分别为50和5kA/cm2,激光发射波长为405.9nm,脊型波导结构激光器输出光功率大于100mW.     

窄条AlGaAs激光器的自脉动研究

分析了利用窄条AlGaAs激光器的自脉动来进行3R时钟提取的基本原理,阐述了F-P腔半导体激光器自脉动产生的机理和条件,同时研究了窄条AlGaAs激光器的结构参数对自脉动的影响,提出了一种在不规则窄条AlGaAs激光器中加入量子阱结构以提高输出光脉冲频率和功率的方法.并使用仿真程序对该方法进行了仿真实验.     

用于产生微波信号的分布反馈激光器与Y形波导单片集成器件的研究

设计并制作了一种在Y形波导的两个分支上集成分布反馈(distributed feedback,DFB)激光器的单片集成器件.DFB激光器的布拉格光栅一次曝光形成,具有相同的光栅周期.当注入电流分别单独加载到两段DFB激光器之上时,从Y形波导端输出光波长在1565nm附近,边模抑制比大于30dB.当大于阈值且相差大于20mA的两个电流同时加载到两段DFB激光器上时,从Y形波导端输出的光谱具有双模分布,双模频率的差值可以拍频产生微波频段的信号.通过调节两段DFB的注入电流,微波信号的频率可以在13～42GHz之间快速连续调谐.这种基于Y形波导的两段DFB并联的拍频光源比传统的双段级联DFB器件有较好的光学和电学隔离,可以作为光学拍频源的一种新的实现方法.     

用于产生微波信号的分布反馈激光器与Y形波导单片集成器件的研究

设计并制作了一种在Y形波导的两个分支上集成分布反馈(distributed feedback,DFB)激光器的单片集成器件.DFB激光器的布拉格光栅一次曝光形成,具有相同的光栅周期.当注入电流分别单独加载到两段DFB激光器之上时,从Y形波导端输出光波长在1565nm附近,边模抑制比大于30dB.当大于阈值且相差大于20mA的两个电流同时加载到两段DFB激光器上时,从Y形波导端输出的光谱具有双模分布,双模频率的差值可以拍频产生微波频段的信号.通过调节两段DFB的注入电流,微波信号的频率可以在13～42GHz之间快速连续调谐.这种基于Y形波导的两段DFB并联的拍频光源比传统的双段级联DFB器件有较好的光学和电学隔离,可以作为光学拍频源的一种新的实现方法.     

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.