高质量单晶In2Ge2O7纳米带的合成和生长机制探究

采用CVD法成功合成了高质量单晶In2 Ge2 O7纳米带,采用高分辨透射电子显微镜(HRTEM)图像以及X射线衍射(XRD),能谱元素分布图像等对产物进行了表征.结果表明,生长的纳米带长几十微米、厚度50 nm,几乎没有缺陷且In,Ge,O元素分布均匀.此外,基于热力学原理对单晶纳米带的生长机制进行了讨论.     

Growth of hexagonal and cubic InN nanowires using MOCVD with different growth temperatures

We have performed a detailed investigation of the metal-organic chemical vapor deposition (MOCVD) growth and characterization of InN nanowires formed on Si(1 1 1) substrates under nitrogen rich conditions. The growth of InN nanowires has been demonstrated by using an ion beam sputtered (∼10 nm) Au seeding layer prior to the initiation of growth. We tried to vary the growth temperature and pressure in order to obtain an optimum growth condition for InN nanowires. The InN nanowires were grown on the Au+In solid solution droplets caused by annealing in a nitrogen ambient at 700 °C. By applying this technique, we have achieved the formation of InN nanowires that are relatively free of dislocations and stacking faults. Scanning electron microscopy (SEM) showed wires with diameters of 90–200 nm and lengths varying between 3 and 5 μm. Hexagonal and cubic structure is verified by high resolution X-ray diffraction (HR-XRD) spectrum. Raman measurements show that these wurtzite InN nanowires have sharp peaks E₂ (high) at 491 cm⁻¹ and A₁ (LO) at 591 cm⁻¹.     

Growth and optical properties of high-density InN nanodots

High density InN/GaN nanodots were grown by pulsed mode (PM) metal–organic chemical vapor deposition (MOCVD). InN nanodots density of up to ∼5×10¹⁰ cm⁻² at a growth temperature of 550 °C was achieved. The high diffusion activation energy of 2.65 eV due to high NH₃ flow rate generated more reactive nitrogen adatoms on the growth surface, and is believed to be the main reason for the growth of high density InN nanodots. In addition, an anomalous temperature dependence of the PL peak energy was observed for high density InN nanodots. The high carrier concentration, due to high In vacancy (V_In) in the InN nanodots, thermally agitated to the conduction band. As the measurement temperature increased, the increase of Fermi energy resulted in blue-shifted PL peak energy. From the Arrhenius plot of integrated PL intensity, the thermal activation energy for the PM grown InN nanodots was estimated to be E_a∼51 meV, indicating strong localization of carriers in the high density InN nanodots.     

以乙醇为氧源生长ZnO薄膜中温度对光谱影响的研究

本文探索了以乙醇为氧源通过MOCVD方法生长ZnO薄膜的方法,着重研究了该实验中生长温度对薄膜发光光谱的影响.我们分别在350℃、370℃、380℃、400℃和420℃温度下生长了ZnO薄膜,并对其发光光谱进行了研究.结果表明适当地提高生长温度可以使近带边发光峰蓝移,但温度过高,使得峰位红移并展宽.在380℃的生长条件下得到了较好的光谱.370℃条件下还出现了474nm的发光峰,经退火后此峰消失.     

MOCVD生长温度对氧化锌薄膜结构及发光性能的影响

利用甲醇做氧源,采用金属有机物化学气相沉积(MOCVD)工艺在硅(111)衬底上生长了一系列的氧化锌薄膜,生长温度为400～600 ℃.薄膜的表面形貌及晶体质量分别利用场发射扫描电镜及X射线衍射仪进行了测量.研究表明:随着生长温度的降低,在X射线衍射图谱中氧化锌(101)峰取代了(002)峰成为了主峰.这可能是由于温度过低使得甲醇未完全分解,而甲醇分子抑制了氧化锌沿c轴极性过快的生长所致.室温光致发光光谱结果表明在较高生长温度下获得的样品具有良好的光学性质,发光强度随着温度的降低而降低.     

MOCVD生长低阈值电流GaInP/AlGaInP650nm激光器

通过MOCVD外延实现了限制层高铝组分及高掺杂,制作出低阈值电流密度的压应变多量子阱激光器材料,后工艺制备了低阈值电流基横模弱折射率脊形波导激光器.该激光器阈值电流最低达到6.2mA,这是我们所见报道的650nm AlGaInP红光激光器的最低阈值电流. 在25mA 工作电流下,基横模连续输出功率达到18mW.     

径向三重流MOCVD反应器生长GaN的数值模拟

采用计算流体力学方法对生长半导体材料GaN的重要设备三重进口行星式MOCVD (金属有机物化学气相沉积) 反应室中的输运过程进行了二维数值模拟.从浓度场的角度分析反应器内衬底上方NH3和TMGa的浓度影响因素.根据对模拟结果的分析,发现较均匀的流场对应衬底上方的反应物浓度较高,降低反应器内压强,也可获得衬底上方较高的反应物浓度,由于MOCVD反应器内有较大的温差,因此热扩散效应不能忽视.     

MOCVD法在(220)CaF2衬底上生长ZnO薄膜及其性能研究

采用金属有机化学汽相沉积(MOCVD)法在(220)CaF2衬底上外延生长ZnO薄膜.利用X射线衍射(XRD)、紫外-可见光谱和光致发光谱(PL)对ZnO薄膜的结构和光学性能进行了分析.XRD结果表明,所制备的ZnO薄膜结晶性能良好,具有高度的(002)的择优取向,002衍射峰的半高宽(FMHM)为0.115°.所制备的ZnO薄膜透明,透过率超过85;.在常温的(He-Cd激光器)PL谱中,只有378.5 nm的带边发射.用同步辐射光源测试的真空紫外光谱中,在低温20K时,出现218 nm、368 nm、418 nm、554 nm发光峰,其中368 nm峰强度随着温度的升高强度逐渐下降,到常温时几乎消失.     

GaAs衬底温度对液滴外延法生长In液滴的影响

采用液滴外延法在GaAs(001)衬底上生长In液滴,利用原子力显微镜(AFM)对不同衬底温度下生长的样品进行表征,观察其表面形貌.研究表明In液滴的生长对衬底温度十分敏感,随着衬底温度的升高,液滴密度逐渐减小,液滴尺寸逐渐增大.分析了In液滴在不同衬底温度形成过程的物理机制,解释了该实验现象的原因.根据成核理论中最大...     

Growth and annealing effect of high-quality ZnSe:N/ZnSe by MOCVD

The ZnSe : N epitaxial layers were grown on (1 1 0) ZnSe substrates in a low-pressure metalorganic chemical vapor deposition (MOCVD) system using hydrogen as a carrier gas, and using ammonia as a dopant source. In order to obtain highly doped ZnSe : N epitaxial layers, the optimum growth and doping conditions were determined by studying the photoluminescence (PL) spectra from the ZnSe epitaxial layers grown at different ammonia flux and VI/II flux ratio. Furthermore, in order to enhance the concentration of active nitrogen in ZnSe epitaxial layer, a rapid thermal anneal technique was used for post-heat-treating. The results show that the annealing temperature of over 1023 K is necessary. Beside, a novel treatment method to obtain a smooth substrate surface for growing high quality ZnSe epitaxial layers is also described.