立方相GaN外延层的表面起伏和高密度孪晶与六角相

利用扫描电子显微镜(SEM)、原子力显微镜(AFM)、透射电子显微镜(TEM)和X射线衍射(XRD)技术研究了低压金属有机化学气相淀积(LP-MOCVD)的立方相GaN/GaAs(001)外延层的表面起伏特征，及其与外延层极性和内部六角相、立方相微孪晶之间的联系。结果表明外延表面存在有大量沿[1-10]方向延伸的条带状台阶，而表面起伏处对应着高密度的六角相或立方相微孪晶，在表面平整的区域内其密度则较低。{111}_(Ga)和{111}_N面上形成六角相和微孪晶概率的明显差异是导致外延层表面台阶状起伏特征的根本原因。

InGaAs/GaAs多量子阱SEED设计和特性研究

分析计算了InGaAs/GaAs多量子阱(SEED)的激子吸收行为,对器件的多量子阱及谐振腔结构进行了设计和理论分析, 用MOCVD系统生长了多量子阱外延材料,并且对器件的反射谱和光电流谱特性进行了测试。

InGaAs/GaAs多量子阱 SEED面阵结构特性与设计（英文）

讨论了谐振腔中的DBR对InGaAs/GaAs多量子阱SEED面阵光反射特性的影响。采用InGaAs/GaAs作为多量子阱SEED器件的有源区，从而获得了980nm工作波长。设计和分析了InGaAs/GaAs多量子阱SEED中的一种用于倒装焊的新型谐振腔结构。多量子阱材料是用MOCVD系统生长，利用微区光反射谱、PL谱以及X射线双晶衍射对多量子阱材料进行了测量和分析，测量结果表明多量子阱材料具有良好的质量，证明了器件结构的设计和分析是准确的。

高质量立方相InGaN的生长

利用LP-MOCVD技术在GaAs(001)衬底上生长了高质量的立方相InGaN外延层。研究了生长速率对InGaN质量的影响，提出一个简单模型解释了在改变TEGa流量条件下出现的In组分的变化规律，实验结果与模型的一次项拟合结果较为吻合，由此推断，在现在的生长条件下，表面单个Ga原子作为临界晶核吸附Ga或In原子实现生长的模型与实际情况较为接近。对于晶体质量的变化也给予了说明。得到的高质量立方相InGaN室温下有很强的发光峰，光致发光峰半高宽为128meV左右。

Au-GaN肖特基结的伏安特性

在MBE和MOCVD两种方法制备的n-GaN材料上制作了Au-GaN肖特基结，测定了肖特基结的室温I-V特性。分析表明

InAlGaAs/GaAs量子阱的生长及其界面特性

该文研究了以InAlGaAs作垒层的InAlGaAs/GaAs量子阱的低压金属有机化合物化学汽相淀积(LP-MOCVD)生长及其界面特性，发现在适当生长条件下可以解决InGaAs和AlGaAs在生长温度范围不兼容的问题，得到了高质量的InAlGaAs/GaAs量子阱材料。同时用X光和低温光致发光(PL)谱研究了量子阱结构的界面特性，表明适当的界面生长中断不仅可以改善界面平整度，而且能改善垒层InAlGaAs的质量。

表面电场导致InGaAs/GaAs量子阱子带跃迁选择定则的改变

报道用MOCVD方法制作高质量的InGaAs/GaAs应变量子阱材料.单量子阱样品在室温光伏谱中出现清晰的11H、12H、21H和22H激子吸收峰.首次用室温光伏方法研究表面自建电场导致InGaAs/GaAs量子阱中子带间跃迁选择定则的改变.

优化生长的In_xGa_(1-x)As缓冲层上双势垒In_yGa_(1-y)As/Al_zGa_(1-z)As/GaAs/Al_zGa_(1-z)As多量子阱应变状态测量

一种多步生长方法应用于GaAs衬底上的In_xGa_(1-x)As缓冲层的MOCVD生长.在这种In_xGa_(1-x)As缓冲层上生长的In_yGa_(1-y)As/Al_zGa_(1-z)As/GaAs/Al_zGa_(1-x)As双垫垒量子阱材料表现出了很好的晶格特性和光学性质.超晶格的室温光伏谱中出现很强的22H高阶机制吸收峰,表明超晶格界面质量很好.主要应用X射线双晶衍射方法,给出了样品中各层的应变状态.据此,合理地解释了样品的光学测试结果.

1.27μm吸收型部分增益耦合MQW-DFB激光器

采用LP-MOCVD和LPE相结合,成功地研制出了吸收型部分增益耦合MQW-DFB激光器。扫描显微镜照片显示了清晰的被掩埋的吸收型增益耦合光栅,表明光栅掩埋生长前升温过程磷烷的保护是成功的。宽接触(broad area)脉冲电流大范围单纵模工作,条型器件室温连续直流工作阈电流为22mA至35mA,单模成品率高,边模抑制比(SMSR)超过37dB,没有观察到饱和吸收现象。

高精度双晶衍射（HRDCD）方法检测InGaAs/GaAs超薄应变层量子阱结构参数

应变超薄层结构的组分、厚度应变状态的直接检测,对于器件应用具有重要的意义,该文中,利用MOCVD方法得到高质量的InGaAs/GaAs量子阱材料,采用双晶衍射方法的弱信号收集技术,结合运动学理论模拟,得出同时包含几个不同阱宽的InGaAs/GaAs量子阱结构的重要参数,其检测结果与光致发光(PL)、透射电子显微镜(TEM)等方法的测试结果基本一致,表明X射线双晶衍射方法是检测超薄层应变量子阱结构的一个有效方法。

Growth and photoluminescence of InAlGaN films

Two quaternary InAlGaN films were grown by metal-organic chemical-vapor deposition (MOCVD) on sapphire (0001) substrates with and without high-temperature GaN interlayer, respectively. The structural and optical properties of the quaternary films were investigated by high-resolution X-ray diffraction (HRXRD), high-resolution electron microscopy (HREM), temperature-dependent photoluminescence (PL) spectroscopy and time-resolved photoluminescence (TRPL) spectroscopy. According to the HRXRD and PL results, it is demonstrated that two samples have the same crystal quality. The TRPL signals of both samples were fitted well as a stretched exponential decay from 14 K to 250 K, indicating significant disorder in the materials, which is attributed to recombination of excitons localized in disorder quantum nanostructures such as quantum dots or quantum disks originating from indium (In) clusters or In composition fluctuation. The cross-section HREM measurement further proves that there exist disorder quantum nanostructures in the quaternary. By investigating the temperature dependence of the dispersive exponent beta, it is shown that the stretched exponential decays of the two samples originate from different mechanisms. (C) 2003 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Design and fabrication of polarization-insensitive 1550 mm semiconductor optical amplifiers

Polarization-insensitive semiconductor optical amplifiers (SOA's) with tensile-strained multi-quantum-wells as actice regions are designed and fabricated. The 6x6 Luttinger-Kohn model and Bir-Pikus Hamiltonian are employed to calculate the valence subband structures of strained quantum wells, and then a Lorentzian line-shape function is combined to calculate the material gain spectra for TE and TM modes. The device structure for polarization insensitive SOA is designed based on the materialde gain spectra of TE and TM modes and the gain factors for multilayer slab waveguide. Based on the designed structure parameters, we grow the SOA wafer by MOCVD and get nearly magnitude of output power for TE and TM modes from the broad-area semiconductor lasers fabricated from the wafer.

Tunable MQW-DBR lasers using selective area growth

The tunable ridge waveguide distributed Bragg reflector (DBR) lasers designed for wavelength-division-multiplex (WDM) communication systems at 1.55 um by using selective area growth (SAG) is reported. The threshold current of the DBR laser is 62mA and the output power is more than 8mW. The isolation resistance between the active region and the Bragg region is 30K Ohm. The total tuning range is 6.5nm and this DBR laser can provide 6 continuous standard WDM channels with 100GHz channel spacing; in the tuning range, the single mode suppression ratio (SMSR) is maintained more than 32dB and the maximum output power variation is less than 3dB.

650nm AlGaInP quantum well lasers for the application of DVD

Main application of 650nm band laser diodes are for digital versatile disk (DVD). We demonstrate here the 650nm AlGaInP LD grown by LP-MOCVD with the structure of selected buried ridge waveguide. Excellent performance of LD have been achieved such as threshold current, threshold current density as low as 20mA and 350A/cm(2) respectively at room temperature, the operating temperature up to 90 for the linear power output of 5mw. RIN is about -130db/Hz, The samples of LD have been certified by PUH manufacturers.

High efficiency, low vertical divergence angle 980nnn Al-free active region lasers with novel large optical cavity and asymmetrical cladding layers

980nm InGaAs/InGaAsP/AlGaAs strained quantum well lasers,vitta novel large optical cavity and asymmetrical claddings was fabricated bg MOCVD. Very high differential quantum efficiency elf 90% (1.15W/A) and low vertical divergence angle of 24 degrees at long cavity length were obtained for 100 mu m stripe lasers. The differential quantum efficiency is up to 94% (1.20) at cavity length of 500 mu m.