609 resultados para PSEUDOMORPHIC INGAAS HEMT


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利用数值计算的方法研究了InP基高电子迁移率晶体管(HEMT)中沟道厚度对沟道中二维电子气(2DEG)性质的影响,并对产生这种影响的原因进行了深入探讨.计算结果表明,当沟道层厚度从10nm增加到40nm时,沟道中2DEG的密度几乎没有变化,但激发态和基态上的电子密度之比(R)先增加后减小.当沟道层厚度在20-25nm之间时,R达到最大.此结果可作为优化器件结构设计的依据.

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平面型雪崩光电二极管(APD)在结弯曲处具有高的电场,导致在结边缘的提前击穿。运用FEMLAB软件对不同工艺流程制备的三种不同结构平面型InP/InGaAsAPD的电场分布进行了二维有限元模拟,在表面电荷密度为5×10^11cm^-2时分析了吸收层厚度、保护环掺杂浓度、保护环和中央结纵向及横向间距等因素对边缘提前击穿特性的抑制程度。比较了这三种结构的InP/InGaAsAPD在边缘提前击穿的抑制特性的优劣。通过理论研究对平面InP/InGaAsAPD进行了优化。

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AlGaN/AlN/GaN high electron mobility transistor (HEMT) structures with a high-mobility GaN thin layer as a channel are grown on high resistive 6H-SiC substrates by metalorganic chemical vapor deposition. The HEMT structure exhibits a typical two-dimensional electron gas (2DEG) mobility of 1944cm2/(V · s) at room temperature and 11588cm2/(V· s) at 80K with almost equal 2DEG concentrations of about 1.03 × 1013 cm-2 High crystal quality of the HEMT structures is confirmed by triple-crystal X-ray diffraction analysis. Atomic force microscopy measurements reveal a smooth AlGaN surface with a root-mean-square roughness of 0. 27nm for a scan area of 10μm × 10μm. HEMT devices with 0.8μm gate length and 1.2mm gate width are fabricated using the structures. A maximum drain current density of 957mA/mm and an extrinsic transconductance of 267mS/mm are obtained.

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采用低压金属有机化合物气相沉积法(LP-MOCVD)生长并制作了1.6—1.7μm大应变InGaAs/InGaAsP分布反馈激光器.采用应变缓冲层技术,得到质量良好的大应变InGaAs/InP体材料.器件采用了4个大应变的量子阱,加入了载流子阻挡层改善器件的温度特性.1.66μm和1.74μm未镀膜的3μm脊型波导器件阈值电流低(小于15mA),输出功率高(100mA时大于14mW).从10—40℃,1.74μm激光器的特征温度T0=57K,和1.55μm InGaAsP分布反馈激光器的特征温度相当.

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研究了双子带占据的In0.52Al0.48As/In0.53Ga0.47As单量子阱中磁电阻的Shubnikov-de Haas(SdH)振荡效应和霍耳效应,获得了不同子带电子的浓度、迁移率、有效质量和能级位置.低磁感应强度(B〈1.5T)下由迁移率谱和多载流子拟合相结合的方法得到的各子带电子浓度与通过SdH振荡得到的结果一致.在d^2ρ/dB^2-1/B的快速傅里叶变换谱中,观察到除了通常强烈依赖温度的对应于各子带的频率f1和f2以及f1的倍频(2f1)外,还观察到对温度不敏感的频率f1-f2.这是由于量子阱中不同子带的电子具有相近的有效质量,两个子带之间发生了强烈的磁致子带间散射.

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The growth of multi-layer InGaAs/InAs/GaAs self-assembled quantum dots (QDs) by molecular beam epitaxy (MBE) is investigated,and a QD laser diode lasing at 1.33μm in continuous operation mode at room temperature is reported. The full width at half maximum of the band edge emitting peaks of the photoluminescence (PL) spectra at room temperature is less than 35meV for most of the multi-layer QD samples,revealing good,reproducible MBE growth conditions. Moreover,atomic force microscopy images show that the QD surface density can be controlled in the range from 1×10^10 to 7 ×10^10 cm^-2 . The best PL properties are obtained at a QD surface density of about 4×10^10cm^-2. Edge emitting lasers containing 3 and 5 stacked QD layers as the active layer lasing at room temperature in continuous wave operation mode are reported.

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用固态分子束外延技术生长了高应变.In0.45Ga0.55As/GaAs量子阱材料.研究了快速热退火对高应变InGaAs/GaAs量子阱材料光学性质的影响.本文采用假设InGaAs/GaAs量子阱中的In—Ga原子扩散为误差函数扩散并解任意形状量子阱的薛定谔方程的方法,对不同退火温度下InGaAs/GaAs量子阱室温光致发光峰值波长拟合,得到了In原子在高应变InGaAs/GaAs量子阱中的扩散系数以及扩散激活能(O.88ev).

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The compressively strained InGaAs/InGaAsP quantum well distributed feedback laser with ridge-wave- guide is fabricated at 1.74μm. It is grown by low-pressure metal organic chemical vapor deposition(MOCVD). A strain buffer layer is used to avoid indium segregation. The threshold current of the device uncoated with length of 300μm is 11.5mA. The maximum output power is 14mW at 100mA. A side mode suppression ratio of 35.5dB is obtained.

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A novel unselective regrowth buried heterostructure long-wavelength superluminescent diode (SLD) with a graded composition bulk InGaAs active region is developed by metalorganic vapor phase epitaxy (MOVPE). At a 150mA injection current, the full width at half maximum of the emission spectrum of the SLD is about 72nm, ranging from 1602 to 1674nm. The emission spectrum is smooth and flat. The ripple of the spectrum is less than 0.3dB at any wavelength from 1550 to 1700nm. An output power of 4.3mW is obtained at a 200mA injection current under continuous-wave operation at room temperature. This device is suitable for the applications of light sources for gas detectors and L-band optical fiber communications.

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A Si doped AlGaN/GaN HEMT structure with high Al content (x= 44%) in the barrier layer is grown on sapphire substrate by RF-MBE. The structural and electrical properties of the heterostructure are investigated by the triple axis X-ray diffraction and Van der Pauw-Hall measurement, respectively. The observed prominent Bragg peaks of the GaN and AlGaN and the Hall results show that the structure is of high quality with smooth interface.fabricated and characterized. Better DC characteristics, maximum drain current of 1.0A/mm and extrinsic transconductance of 218mS/mm are obtained when compared with HEMTs fabricated using structures with lower Al mole fraction in the AlGaN barrier layer. The results suggest that the high Al content in the AlGaN barrier layer is promising in improving material electrical properties and device performance.

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利用动态掩膜湿法腐蚀技术,研究了HCl/HF/CrO3溶液对与InP衬底晶格匹配的InxGa1-xAs1-yPy(y=0,0.2,0.4,0.6)材料的腐蚀特性.对于HCl(36wt%)/HF(40wt%)/CrO3(10wt%)的体积比为x∶0.5∶1的溶液,随着x由0增加到1.25,相应的腐蚀液对In0.53Ga0.47As/In0.72Ga0 28As06P0.4的选择性由42.4降到1.4;通过调节腐蚀液的选择性,在In072Ga0.28As06P0.4外延层上制备出了倾角从1.35°到35.9°的各种楔形结构;当x为0.025和1.25时,相应的In0.72Ga0.28As0.6P0.4腐蚀表面的均方根粗糙度分别为1.1nm和1.6nm.还研究了溶液的组分与InxGa1-xAs1-yPy(y=0,0.2,0.4)的腐蚀速率间的关系,并对腐蚀机理进行了分析.

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采用压应变InGaAs量子阱和张应变InGaAs准体材料交替混合的有源结构,研制了宽带偏振不灵敏的半导体光放大器.此放大器在100~250mA的工作电流范围内,获得了大于70nm的3dB光带宽;在0~250mA工作电流和3dB光带宽波长范围内,偏振灵敏度小于1dB.对于1.55μm的信号光,在200mA的注入电流下获得了15.6dB的光纤到光纤的增益、小于0.7dB的偏振灵敏度和4.2dBm的饱和输出功率.

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简要回顾了AlGaN/GaN HEMT器件电流崩塌效应研究的进展,着重阐述了虚栅模型、应力模型等几种解释电流崩塌效应形成机理的模型和器件钝化、生长盖帽层等减小电流崩塌效应的措施.

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A kind of novel broad-band superluminescent diodes (SLDs) using graded tensile-strained bulk InGaAs is developed. The graded tensile-strained bulk InGaAs is obtained by changing only group-III trimethyl-gallium source flow during low-pressure metal organic vapor-phase epitaxy. At the injection current of 200 mA, the fabricated SLDs with such structure demonstrate full-width at half-maximum spectral width of 106 nm and the output light power of 13.6 mW, respectively.

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在GaAs基In x Ga1-xAs( x =0.15)应变层上生长了InAs 量子点(QD)层,通过分析各层之间的应力状况和位错的演变过程,配合生长过程中对反射式高能电子衍射仪(RHEED)实时监测,并观察生长后的表面形貌,发现可以通过控制应变层厚度来控制应变层表面布纹结构的宽度,而且在应变层厚度低于位错增殖的临界厚度时布纹宽度较窄.如果同时控制QD层在刚刚出点,则QD主要沿着较窄的布纹结构排列,从而得到有序排列的QD.