高Al组分In1-xAlx Sb/InSb的MBE生长研究

高Al(10%~15%)组分的In1-xAlx Sb层可作为势垒层以抑制隧穿暗电流、提高器件工作温度而显得很重要。采用分子束外延的方法对InSb(100)衬底高Al组分的In1-xAlx Sb/InSb外延生长进行了实验探索,确定出了Al组分(约12.5%)并讨论了Al组分梯度递变的In1-xAlx Sb缓冲层和生长温度对外延薄膜质量的影响。     

MOCVD生长不同Al组分AlGaN薄膜

本文研究了利用金属有机物化学汽相淀积系统（MOCVD）生长高质量不同Al组分AlxGa1-xN薄膜（0．13〈x〈0．8）。扫面电子显微镜（SEM）照片表明生长的AlN插入层有效地调节了AlGaN层与GaN支撑层的应力，使AlGaN表面平整无裂纹，原子力显微镜（AFM）测量得到所有AlGaN薄膜粗糙度均小于1nm。通过原位干涉谱发现，AlGaN薄膜生长速率主要由Ga流量大小控制，随Al组分升高逐渐降低。利用X射线衍射和卢瑟福背散射（RBS）两种方法确定AlGaN薄膜的Al组分，发现Al组分与摩尔比TMAl／（TMGa＋TMAl）关系为线性，说明在优化的生长条件下，Al原子与NH3的寄生反应得到了有效的抑制。     

MOCVD生长不同Al组分AlGaN薄膜

本文研究了利用金属有机物化学汽相淀积系统(MOCVD)生长高质量不同Al组分AlxGa1-xN薄膜(0.13＜x＜0.8).扫面电子显微镜(SEM)照片表明生长的AlN插入层有效地调节了AlGaN层与GaN支撑层的应力,使AlGaN表面平整无裂纹,原子力显微镜(AFM)测量得到所有AlGaN薄膜粗糙度均小于1 nm.通过原位干涉谱发现,AlGaN薄膜生长速率主要由Ga流量大小控制,随Al组分升高逐渐降低.利用X射线衍射和卢瑟福背散射(RBS)两种方法确定AlGaN薄膜的Al组分,发现Al组分与摩尔比TMAl/(TMGa+TMAl)关系为线性,说明在优化的生长条件下,Al原子与NH3的寄生反应得到了有效的抑制.     

MOCVD生长不同Al组分AlGaN薄膜

本文研究了利用金属有机物化学汽相淀积系统(MOCVD)生长高质量不同Al组分AlxGa1-xN薄膜(0.13相似文献   

高温工作InAlSb的MBE生长及器件性能研究

接近室温的更高工作温度是第三代红外探测器发展的重要方向。本文论述了用MBE在InSb(100)衬底上外延生长制备P-i-N型三元In1-xAlxSb薄膜合金材料,并通过制备单元器件进行了验证。采用RHEED振荡和X射线双晶衍射对In1-xAlxSb薄膜的Al组分进行了调控和检测。5.3 μm厚薄膜的FWHM≈50 arcsec,Al组分约1.9%。10 μm×10 μm原子力表面粗糙度RMS≈0.6 nm。制备的单元器件获得了预期的理想效果,为下一步面阵焦平面的制备奠定了基础。     

高质量InSb薄膜的MBE同质和异质外延生长

InSb是3~5 μm中波红外波段具有重要研究意义的材料。本文以单位内部生产的InSb(100)衬底为基础,通过摸索InSb(100)衬底的脱氧、生长温度和V/III束流比,获得了高质量的InSb同质外延样品,1.5 μm样品的表面粗糙度RMS≈0.3 nm(10 μm×10 μm),FWHM≈7 arcsec;采用相同的生长温度和V/III束流比并采用原子层外延缓冲层的方法在GaAs(100)衬底上异质外延生长本征InSb层,获得了较高质量的异质外延InSb样品,1.5 μm样品的室温电子迁移率高达6.06×104cm2 V-1s-1,3 μm的样品最好的FWHM低至126 arcsec。InSb材料的同质和异质外延优化生长可为高温工作掺Al的InSb器件结构的优化生长提供重要参考依据。     

MBE生长的InAs薄膜Hall器件

利用ＧａＡｓ衬底上的ＩｎＡｓ薄膜制备的Ｈａｌｌ器件,具有灵敏度高（在相同的电子浓度、室温附近灵敏度是ＧａＡｓＨａｌｌ器件的１．５倍）,不等位电压温漂小等优点．可用于电流传感器、无刷电机等磁敏传感器中,具有广阔的应用前景     

高Al组分AlGaN的MBE生长及表面活性机理

采用分子束外延(MBE)方法制备了高质量的高Al组分AlGaN薄膜,在室温下获得了266 nm波长的深紫外发光。利用原位监控系统,结合原子力显微镜(AFM)和变温光致发光(PL)谱研究了生长前端的Ga原子的表面活性作用对AlGaN薄膜的生长模式、表面形貌和光学性质的影响,并通过二次离子质谱仪(SIMS)探究了生长温度与p型AlGaN Mg掺杂浓度的变化关系及内在机理。结果显示,Ga原子不仅参与AlGaN的结晶,而且在薄膜生长和Mg掺杂中发挥着表面活性剂的作用,能够促进Al原子的迁移与并入。Ga原子作为表面活性剂有利于AlGaN薄膜进行二维层状生长,改善AlGaN薄膜的表面形貌和光学特性;它还能够提高Al原子的并入效率,使AlGaN薄膜具有更短的发光波长。此外,适当降低p型AlGaN薄膜的生长温度,能减少Mg原子脱吸附并增强Ga原子的表面活性剂作用,从而提高Mg的掺杂浓度。     

MBE生长的InSb和InASxSb1—x的载流子浓度剖面分布

在(111)InSb 和(100)GaAs 衬底上,用分子束外延技术生长了 InSb 和 InAs_xSb_(1-x)外延层。用自动电化学 C—V 法测量了外延层的载流子浓度剖面分布。结果表明:(1)外延层呈 P 型;(2)InSb/GaAs 异质外延层的载流子浓度为(1～2)×10~(16)cm~(-3),比相应的同质外延层 InSb/InSb 的(1～2)×10~(17)cm~(-3)小一个数量级;(3)生长层的载流子浓度剖面分布和质量取决于衬底表面的制备。讨论了有关问题。     

高Al组分AlxGa1-xN薄膜的弹性-塑性力学性质

采用纳米压痕方法,研究了AlN/sphire模板上的高Al组分AlxGa1-xN薄膜的力学性质,特别是弹性-塑性转变行为.研究表明,AlxGa1-xN薄膜的杨氏模量E随着Al组分的增加而增大,薄膜中产生塑性形变所必要的剪切应力也随着Al组分的增加而增大.在AlxGa1-xN薄膜纳米压痕实验中,观察到位移不连续的跳断("pop-in")行为,并且发现"pop-in"行为强烈依赖于Al组分,Al组分的增加导致这种行为的减少.我们认为随着Al组分的增加,AlxGa1-xN中键能的增强和由于AlxGa1-xN与AlN/sapphire模板之间晶格失配减少这两个因素增加了AlxGa1-xN中新位错形成的阻力,从而导致了AlxGa1-xN薄膜中的"pop-in"行为随Al组分增加而减少.     

Al薄膜对(002)ZnO/Al/Si结构基片中ZnO薄膜特性影响的实验研究

采用射频磁控溅射法沉积制备了(002)ZnO/A l/Si复合结构。研究了Al薄膜对(002) ZnO/Al/Si复合结构的声表面波器件(SAWD)基片性能影响以及当ZnO 薄膜厚度一定时的Al膜最佳厚度。采用X射线衍射(XRD)对Al和ZnO薄膜进行了结构表征 ,采用 扫描电镜(SEM)对ZnO薄膜进行表面形貌表征,并从薄膜生长机理角度进行了分析。结果 表明,加Al薄膜有利于ZnO薄膜按(002)择优取向生长,并且ZnO 薄膜的结晶性能提高;与(002)ZnO/Si结构基片相比,当Al薄膜 厚为100nm时,(002)ZnO/Al/Si结构中ZnO薄 膜的机电耦合系数提高 了65%。     

InP基MOCVD及MBE外延生长HBT的制备与分析

设计并研制了用于光电集成(OEIC)的InP基异质结双极晶体管(HBT),介绍了工艺流程及器件结构。分别采用金属有机化学气相沉积(MOCVD)及分子束外延(MBE)生长的外延片,并在外延结构、工艺流程相同的条件下,对两种生长机制的HBT直流及高频参数进行和分析。结果表明,采用MOCVD生长的InP基HBT,直流增益为30倍,截止频率约为38GHz;MBE生长的HBT,直流增益达到100倍,截止频率约为40GHz。这表明,MBE生长的HBT外延层质量更高,在相同光刻条件下,所对应的HBT器件的性能更好。     

Observation of prevalence of quasi-equilibrium in the MBE growth of Hg1−xCdxTe

MBE growth of Hg_1−xCd_xTe has been carried out at 185°C. Parameters of growth have systematically varied. The resulting compositional changes and the electrical characteristics have been explained on the basis of the prevalence of quasi-equilibrium at the growth temperature.     

Kinetics of hillock growth in Al and Al-alloys

Hillock growth kinetics and size distribution were investigated in Al, Al:Si 1% and Al:Si1%:Cu 0.5% layers. Metallization surface was examined by optical, SEM and TEM microscopy, stylus profiling and an automatic method of hillock recognition from a microscope image. The method allowed for counting hillocks in a desired range of their diameter d. Surface density of hillocks was measured as a function of time of furnace annealing at 400°C and as a function of temperature of RTP annealing. A maximum hillock size was found to increase linearly with metallization layer thickness and with logarithm of annealing time. A total area occupied by hillocks was evaluated. Hillock density decreased versus 1/T with an activation energy of 0.28 eV for Al and 0.31 eV for Al:Si. It was found, that a normalized hillock density N may be expressed by a formula N=N₀ exp(−cd). Values for N₀ and c are given together with a short discussion.     

MBE growth of tensile-strained Ge quantum wells and quantum dots

Germanium (Ge) has gained much interest due to the potential of becoming a direct band gap material and an efficient light source for the future complementary metal-oxide-semiconductor (CMOS) compatibl...     

A low voltage and small hysteresis C_(60) thin film transistor

Organic thin film transistors with C_(60) as an n-type semiconductor have been fabricated.A tantalum pentoxide(Ta_2O_5)/poly-methylmethacrylate(PMMA) double-layer structured gate dielectric was used.The Ta_2O_5 layer was prepared by using a simple solution-based and economical anodization technique.Our results demonstrate that double gate insulators can combine the advantage of Ta_2O_5 with high dielectric constant and polymer insulator for a better interface with the organic semiconductor.The performanc...     

Self-limiting MBE growth and characterization of three-dimensionally confined nanostructures on patterned GaAs (311)A substrates

The formation of triangular-shaped dot-like (TD) structures grown by molecular beam epitaxy on GaAs (311)A substrates patterned with square- and triangular-shaped holes is compared. On substrates patterned with square-shaped holes, TD structures are formed via the pinch-off of two symmetrically arranged {111} planes which develop freely in the regions between the holes on the original substrate surface, while the (111)A sidewalls of the as-etched holes develop a rough morphology during growth. The evolution of the rough (111)A sidewalls is eliminated on substrates patterned with triangular shaped holes resulting in similar TD structures with highly improved uniformity over the entire pattern. Spectrally and spatially resolved cathodoluminescence spectroscopy reveals the lateral variation of the quantum-well confinement energy in the TD structures generating distinct lateral energy barriers between the top portion and the nearby smooth regions with efficient radiative recombination. Formation of TD structures provides a new approach to fabricate three-dimensionally confined nanostructures in a controlled manner.