980 resultados para Langmuir-Schaefer (LS)
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The physical properties of low-temperature-deposited GaN buffer layers with different thicknesses grown by metal-organic vapor-phase epitaxy have been studied. A tentative model for the optimum thickness of buffer layer has been proposed. Heavily Si-doped GaN layers have been grown using silane as the dopant. The electron concentration of Si-doped GaN reached 1.7 x 10(20) cm(-3) with mobility 30 cm(2)/V s at room temperature. (C) 1998 Published by Elsevier Science B.V. All rights reserved.
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Single crystal GaN films of hexagonal modification have been fabricated on Al2O3/Si (001) substrates via a low pressure metalorganic chemical deposition (LP-MOCVD) method. The full width at half-maximum of (0002) X-ray diffraction peak for the GaN film 1.1 mu m thick was 72 arcmin. and the mosaic structure of the film was the main cause of broadening to the X-ray diffraction peak. Al room temperature, the photoluminescence (PL) spectrum of GaN exhibited near band edge emission peaking at 365 nm.
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Deep Level Transient Spectroscopy (DLTS) has been applied to investigate the electronic properties of self-organized InAs quantum dots. The energies of electronic ground states of 2.5ML and 1.7ML InAs quantum dots (QDs) with respect to the conduction band of bulk GaAs are about 0.21 eV and 0.09 eV, respectively. We have found that QDs capture electrons by lattice relaxation through a multi-phonon emission process. The samples are QDs embedded in superlattices with or without a 500 Angstrom GaAs spacing layer between every ten periods of a couple of GaAs and InAs layers. The result shows that the density of dislocations in the samples with spacer layers is much lower than in the samples without the spacer layers.
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The electronic state of a two-dimensional electron system (2DES) in the presence of a perpendicular uniform magnetic field and a lateral superlattice (LS) is investigated theoretically. A comparative study is made between a LS induced by a spatial electrostatic potential modulation (referred to as a PMLS) and that induced by a spatial magnetic-field modulation (referred ro asa MMLS). By utilizing a finite-temperature self-consistent Hartree-Fock approximation scheme; the dependence of the electronic state on different system parameters (e.g., the modulation period, the modulation strength, the effective electron-electron interaction strength, the averaged electron density, and the system temperature) is studied in detail. The inclusion of exchange effect is found to bring qualitative changes to the electronic state of a PMLS, leading generally to a nonuniform spin splitting, and consequently the behavior of the electronic state becomes similar to that of a MMLS. The Landau-level coupling is taken into account, and is found to introduce some interesting features not observed before. It is also found that, even in the regime of intermediate modulation strength, the density dependence of the spin splitting of energy levels, either for a PMLS or a MMLS, can be qualitatively understood within the picture of a 2DES in a perpendicular magnetic field with the modulation viewed as a perturbation. [S0163-1829(97)02248-0].
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Wurtzite GaN films have been grown on (001) Si substrates using gamma-Al2O3 as an intermediate layer by low pressure (similar to 76 Torr) metalorganic chemical vapor deposition. Reflection high energy electron diffraction and double crystal x-ray diffraction measurements revealed that the thin gamma-Al2O3 layer of "compliant" character was an effective intermediate layer for the GaN film grown epitaxially on Si. The narrowest linewidth of the x-ray rocking curve for (0002) diffraction of the 1.3 mu m GaN sample was 54 arcmin. The orientation relationship of GaN/gamma-Al2O3/Si was (0001) GaN parallel to(001) gamma-Al2O3 parallel to(001) Si, [11-20] GaN parallel to[110] gamma-Al2O3 parallel to[110] Si. The photoluminescence measurement for GaN at room temperature exhibited a near band-edge peak of 365 nm (3.4 eV). (C) 1998 American Institute of Physics.
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Pt/AlGaN/AlN/GaN Schottky diodes have been fabricated and characterized for H-2 sensing. Platinum (Pt) with a thickness of 20nm was evaporated on the sample to form the Schottky contact. The ohmic contact, formed by evaporated Ti/Al/Ni/Au metals, was subsequently annealed by a rapid thermal treatment at 860 degrees C for 30 s in N-2 ambience. Both the forward and reverse current of the device increased greatly when exposed to H-2 gas. The sensor's responses under different hydrogen concentrations from 500ppm to 10% H-2 in N-2 at 300K were investigated. A shift of 0.45V at 297K is obtained at a fixed forward current for switching from N-2 to 10% H-2 in N-2. Time response of the sensor at a fixed bias of 0.5 V was also measured. The turn-on response of the device was rapid, while the recovery of the sensor at N-2 atmosphere was rather slow. But it recovered quickly when the device was exposed to the air. The decrease in the barrier height of the diode was calculated to be about 160meV upon introduction of 10% H-2 into the ambient. The sensitivity of the sensor is also calculated. Some thermodynamics analyses have been done according to the Langmuir isotherm equation.
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An index-coupled distributed feedback laser with the sampled grating has been designed and fabricated. The +1(st) order reflection of the sampled grating is utilized for laser single mode operation, which is 1.5329 mu m in the experiment. The sampled grating is formed by a conventional holographic exposure combined with the usual photolithography. The typical threshold current of DFB laser with the sampled grating is 25mA, and the optical output is about 10mW at the injected current of 100mA.
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A new ECTT-DHPT with InGaAsP(lambda=1.55 mu m) as base and InGaAsP(lambda=1.3 mu m) as collector as well as waveguide was designed and fabricated, the DC characteristics reveal that the ECTT-DRPT can perform good optoelectronic mix operation and linear amplification operation by optically biased at two appropriate value respectively. Responsivity of more than 52A/W and dark current of 70nA (when V-ce=1V) were obtained.
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An improved selective area growth (SAG) method is proposed to better the fabrication and performance of the Electroabsorption modulated laser The typical threshold current of the EML is 18mA, and the output power is 5.6mW at EAM facet.
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We report highly efficient and stable organic light-emitting diodes (OLEDs) with MoO3-doped perylene-3, 4, 9, 10-tetracarboxylic dianhydride (PTCDA) as hole injection layer (HIL). A green OLED with structure of ITO/20 wt% MoO3: PTCDA/NPB/Alq(3)/LiF/Al shows a long lifetime of 1012 h at the initial luminance of 2000 cd/m(2), which is 1.3 times more stable than that of the device with MoO3 as HIL. The current efficiency of 4.7 cd/A and power efficiency of 3.7 lm/W at about 100 cd/m(2) have been obtained. The charge transfer complex between PTCDA and MoO3 plays a decisive role in improving the performance of OLEDs.
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The tandem organic light-emitting diodes (OLEDs) with an effective charge-generation connection structure of Mg-doped tris(8-hydroxyquinoline) aluminum (Alq(3))/Molybdenum oxide (MoO3)-doped 3, 4, 9, 10-perylenetetracarboxylic dianhydride (PTCDA) were presented. At a current density of 50 mA/cm(2), the current efficiency of the tandem OLED with two standard NPB/Alq(3) emitting units is 4.2 cd/A, which is 1.7 times greater than that of the single EL device. The tandem OLED with the similar connection structure of Mg-doped PTCDA/MoO3-doped PTCDA was also fabricated and the influences of the different connection units on the current efficiency of the tandem OLED were discussed as well.
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在空间图像传感器技术向高分辨率、高精度的应用领域迈进的同时,图像数据量的增长向空间飞行器数据存储和传输设备的性能提出了挑战。 为了解决图像质量和系统瓶颈之间的矛盾, 在地面广泛应用的图像压缩技术也在空间领域逐步取得应用。 空间传感图像的关键性和复杂性使得空间图像系统的设计倾向于选择无损或近无损的图像压缩技术。 尽管本文研究的目的是针对特定工程项目进行图像压缩算法的选型和实现,对空间图像压缩技术特点和算法选型策略进行总结也是本文的一项重要任务。JPEG-LS和CCSDS分别是基于预测的编码技术和基于变换的编码技术的典型代表,两者同样支持图像的无损/有损压缩;同样具有较高的压缩率和较低的复杂度;同样便于软硬件实现,并且已经在国内外的空间项目中获得应用。本文对这两种算法原理进行了详细的研究, 并在此基础上对两者的性能和适用环境进行了对比。本文总结了两种算法各自的优点,并提出了对算法局限性的改进方案。 FPGA在图像处理领域一直具有性能方面的优势。近年来随着技术的成熟,FPGA在空间设备中逐渐获得广泛应用。本文对选定的空间图像压缩算法进行了FPGA 实现,并在硬件平台上对算法进行了验证。测试结果表明,本文提出的FPGA实现性能超过国内外其它 FPGA实现,并接近甚至超过部分 ASIC实现。
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本文简要评述了扫描探针显微学研究的发展过程、目前状况及发展方向,着重介绍了扫描探针显微学(SPM)在分子组装体研究中的一些应用。采用扫描探针显微学结合电化学的方法对自组装膜(SAMs)、表面活性剂(surfactant)、纳米颗粒(nanoparticles)等分子组装体系进行了研究,并结合IR、QCM、XPS、XRD等多种手段对分子组装体在电极表面的形态和结构进行了探讨。主要结果如下:1.SPM研究以杂多酸为基础的分子组装体我们通过将AsMo_(11)V0_(40)~(4-)杂多酸阴离子从其酸性溶液中自吸附至金表面的方法,制备了一类新的无机自组装膜。我们利用QCM、STM和电化学方法分别研究了AsMo_(11)VO_(40)~(4-)自组装膜的吸附过程、在Au表面的结构和电化学性质。QCM数据表明这个自组装过程可以用Langmuir吸附等温式来描述,其吸附自由能为-20 KJ/mol。 通过QCM测得的AsMo_(11)VO_(40)~(4-)自组装膜的表面覆盖度的最大值为1.7 * 10~(-10)mol/cm~2,这相当于一个AsMo_(11)VO_(40)~(4-)阴离子的密堆积单层。AsMo_(11)VO_(40)~(4-)自组装膜的循环伏安图上出现三对可逆的氧化还原峰,每对峰所对应的自组装膜的表面覆盖度都亦为1.78 * 10~(-10) mol/cm2,和QCM结果一致。现场STM图像显示AsMo_(11)VO_(40)~(4-)自组装膜十分的均一没有如何多层或聚集体的结构。高分辨STM图进一步显示在Au(111)表面的sMo_(11)VO_(40)~(4-)自组装膜于+0.7 V(vs.Ag | AgCl)表现出二维有序的四方晶体结构,晶格间距为10-11 A。这个值与sMo_(11)VO_(40)~(4-)阴离子的直径十分接近。从STM图我们也估算出AsMo_(11)VO_(40)~(4-)自组装膜的表面覆盖度为1.8 * 10~(-10) mol/cm~2,这和QCM以及电化学的实验结果都很接近。我们进一步研究了一种新的以杂多酸为基础的有机无机复合膜--砷钼钒杂多酸的十一烷基吡啶盐(CPMVA)--的制备、结构和电催化性质。通过在这种盐的丙酮溶液中循环电位扫描,我们可以在HOPG电极表面制备稳定的CPMVA膜。我们利用XPS、STM和电化学多种手段来表征CPMVA膜的结构和性质。这些研究表明:在新剥离HOPG表面CPMVA膜的结构为自聚集的分子团,而在预阴极化HOPG表面CPMVA膜的结构为自有序单层。CPMVA膜在酸性和丙酮溶剂中部表现出可逆的氧化还原动力学行为,这说明这种新类型的膜甚至能在有机溶剂中用作催化剂。当溶液的pH值大于7.O时,CPMVA膜也能维持其稳定性,它对pH值的依赖程度明显小于其无机物形式的膜(H_4AsMo_(11)VO_(40))对pH值的依赖程度。CPMVA膜对Br0_3-的还原表现出很好的电催化活性,催化电流与BrO_3~-的浓度的平方成正比。这种有很高稳定性的新类型杂多酸膜在催化剂领域中将有很广阔的应用前景。2.电化学STM研究吸附在金属表面的表面活性剂聚集体由于电位诱导引起的结构变化表面活性剂在表面的吸附已广泛地被用于限制电极表面的活性和稳定溶液中的胶体和纳米粒子,但是人们对表面活性剂在电极表面的结构和由于电位变化所引起的结构改变并不清楚。在这个工作中我们利用现场STM观察了电位控制下表面活性剂十二烷基磺酸钠(SDS)在Au(111)表面的吸附。STM图像显示通过控制电位SDS在Au(111)表面有一从半圆柱胶束单层向致密双层膜过渡的构象变化。我们也建立了SDS聚集体在Au(111)表面电位诱导结构变化的模型。就我们所知,这是第一次系统地研究表面活性剂聚集体在金属表面的电位诱导结构变化。3.在固体表面构筑有序的聚苯胺分子导线我们提出了一种新的通过分子设计构筑有序聚苯胺分子导线的新方法。首先,根据Saveant的方法我们在HOPG表面修饰上有序的4-氨基苯单层,然后溶液中的苯胺分子通过阶跃的方法被层层电聚合在4-氨基苯单层修饰的HOPG表面,形成有序的聚苯胺分子导线。FTIR-ERS和XPS结果证实HOPG表面上形成了聚苯胺。SPM图显示在HOPG表面的聚苯胺平面结构为有序的3~(1/2) * 3~(1/2) R 30°。小角X-射线反射结果表明聚苯胺分子导线是垂直站立在HOPG表面。电化学测量进一步表明聚苯胺分子导线的形成有利于加速电子传递速率。这种先分子设计后电聚合的方法可能会成为一类在固体表面制备有序导电聚合物分子导线的新方法。依据上一个实验,我们在金表面通过自组装的方法构筑了绝缘分子导线。我们选择β-环糊精(β-CD)作为包络4-氨基硫酚的理想主体分子。β-CD和4-氨基硫酚形成的包络物首先被自组装到Au表面,然后也通过阶跃的方法被层层电聚合在自组装膜修饰的Au表面,形成有序的聚苯胺分子导线。FTIR-ERS和XPS结果证实Au表面上形成了聚苯胺。低电流STM(LC-STM)图像表明在Au(111)表面的聚苯胺分子线为六角的二维有序,分子与分子之间的最相邻距离为15.5±0.5 A。这种先进行CD超分子自组装后电聚合的方法可能会成为一类制备导电聚合物绝缘分子导线的新方法。4.SPM研究在HOPG表面电化学合成的纳米材料我们通过脉冲恒电位方法从稀的苯胺酸性溶液(1mM苯胺 + 1 M HClO_4)在HOPG表面制备聚苯胺纳米颗粒。我们利用FTIR-ERS、XPS、TM-AFM手段来表征聚苯胺纳米颗粒的组成和结构。FTIR-ERS和XPS结果表明制得的聚苯胺纳米颗粒主要以亚胺形式存在。TM-AFM图像显示分散于HOPG表面的聚苯胺纳米颗粒的表面覆盖度约为10~(10)cm~(-2)。这些纳米颗粒都为圆盘型,直径为200到600埃,高度为10到30埃。这些纳米颗粒的大小随聚合电量由5.7 μC/cm~2增加到19.3 μC/cm~2而增大。我们提出了一种通过分子设计在HOPG表面制备金属纳米粒子的新方法。第一步,根据Saveant的方法我们在HOPG表面修饰上一个4-氨基苯单层。第二步,通过配位相互作用Ag~+能在4-氨基功能化的HOPG表面形成单层。第三步,通过脉冲恒电位方法我们就能在4-氨基苯功能化的HOPG制备Ag纳米颗粒。电化学测量证明了在HOPG表面上Ag纳米颗粒的形成。STM图像显示通过这种方法制得的Ag纳米颗粒的大小十分均一且在HOPG表面上的分散度很高。这种新方法可被广泛地用来在碳表面制备各种金属纳米粒子。
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(1) Langmuir单分子膜对硫酸钡-硫酸铅混晶的影响:在不同的单分子膜下或单分子膜存在下掺杂铅离子时生长的晶体形貌不同。单分子膜对于电荷数相同、离子半径相近的成核离子有选择性。选择性取决于膜头基。(2)压缩单分子膜下氟化钙单晶的生长研究:二十二烷基羧酸单分子膜(BAM)诱导氟化钙晶体沿(110)晶面取向生长。晶体形状规则。但在无单分子膜或未压缩单分子膜下,生成的晶体无特定取向和规则的形貌。(3)氟化钡晶体在Langmuir单分子膜下的选择性结晶:无单分子膜存在时,混合摩尔比为1:2的氯化钡和氟化铵溶液有三种晶体生成。但是在铺展BAM时,可以获得(100)取向的氟化钡单晶。(4)不同单分子膜下氟化钡晶体的生长研究:通过研究不同单分子膜或亚相下氟化钡单晶薄膜。并且发现:亚相溶液的pH值、膜头基的电离程度以及膜头基的种类对于生成晶体的性质都有很大影响。(5)自组装单分子膜诱导氟化钡晶体生长的研究:把三氯锗丙酸组装的亲水的单晶硅片表面作为诱导模板。在自组装模板上得到(100)取向的氟化钡。
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本论文利用表面等离子体共振技术(sPR)进行了生物分子间相互作用的研究。主要包括可免疫识别、免疫分析、生物分子相互作用动力学以及层层组装生物分子功能膜等方面的研究。1.利用表面等离子体共振生物传感器对血清中HSA抗体的活性进行了检测。结果表明表面等离子体共振(SPR)生物传感器能快速实时检测anti-HSA抗体的活性,且传感片能够重复使用100次以上。2.应用表面等离子体共振生物传感器实现了对铁蛋白的实时免疫分析。实验中采用"三明治"放大法提高了分析的灵敏度和选择性。结果表明,在血清中分析铁蛋白的线性区间为30-200ng/ml,检测限为28ng/ml。应用pH2.0 glycine-HCl溶液进行再生,传感片可重复使用50次以上。3.通过溶液竞争法实现了S尸R技术对小分子化合物吗啡的检测。结果表明,溶液竞争法大大优于表面竞争法。同时求得了吗啡、mBSA与单抗及多抗之间相互作用的结合常数,并进行了比较。对实验现象给出了动力学上的合理解释。4.研究了通过静电吸附作用,DNA和PDDA交替组装多层膜。实时表面等离子体共振技术实时监测了DNA/PDDA多层膜的形成,研究了DNA在PDDA表面的吸附动力学。电化学阻抗谱和紫外可见光谱的研究结果也表明了这种层层组装多层膜的均一性。5.应用亲合素和生物素之间的强亲和作用,在金表面层层组装了由亲合素/生物素化抗体组成的蛋白质多层膜。使用实时BIA技术监测了多层膜的成膜过程,同时用电化学阻抗和傅立叶红外光谱对多层膜的成膜过程进行了表征。结果都表明了多层膜的均匀生长。同时,我们用亲和素生物素化抗体层层组装所制备的抗体多层膜对hlgG进行了灵敏检测。6.应用实时BIA技术研究了组蛋白与DNA之间的相互作用。发展了新的固定DNA传感片表面,消除了组蛋白与商品化传感片之间的非特异吸附。用Langmuir和Two State Reaction(Coormation change)模型对所得的动力学传感图进行了拟合,初步得到了动力学常数,直观的比较了组蛋白各亚组分与DNA相互作用之间的动力学差异。