1.3μm InGaAs/InAs/GaAs Self-Assembled Quantum Dot Laser Diode Grown by Molecular Beam Epitaxy

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.

Er离子在Inp、GaAs和Si中的1.54μm特征发光峰

分别在InP、GaAs和Si中以7×10＜′14＞和1×10＜′15＞cm＜′－2＞的剂量进行Er离子注入, 并采用闭管、快速和炉退火等热处理。低温光致发光（PL）、反射式高等电子衍射和卢瑟福背散射实验研究表明, 上述样品中Er＜′3＋＞离子特征发光的中心波长均出现在1．5μm处, 其中InP的发光峰最强, 而注入损伤的恢复是影响Er＜′3＋＞发光的重要因素之一。卢瑟福背散射分析进一步证实退火后Er原子在Si中向表面迁移, 而在InP中的外扩散较小, 并比较了Er在InP和Si晶格中的占位情况。图7参12

Homogeneous Epitaxial Growth of N,N '-di(n-butyl)quinacridone Thin Films on Ag(110)

The structural evolution of the ordered N-N' dibutyl-substituted quinacridone (QA4C) multilayers (3 MLs) has been monitored in situ and in real time at various substrate temperatures using low energy electron diffraction (LEED) during organic molecular beam epitaxy (MBE). Experimental results of LEED patterns clearly reveal that the structure of the multilayer strongly depends on the substrate temperature. Multilayer growth can be achieved at the substrate temperatures below 300 K, while at the higher temperatures we can only get one ordered monolayer of QA4C. Two kinds of structures, the commensurate and incommensurate one, often coexist in the QA4C multilayer. With a method of the two-step substrate temperatures, the incommensurate one can be suppressed, and the commensurate, on the other hand, more similar to the (001) plane of the QA4C bulk crystal, prevails with the layer of QA4C increasing to 3 MLs. The two structures in the multilayers are compressed slightly in comparison to the original ones in the first monolayer.

Fabrication of Novel Superhydrophobic Surfaces and Water Droplet Bouncing Behavior - Part 1: Stable ZnO-PDMS Superhydrophobic Surface with Low Hysteresis Constructed Using ZnO Nanoparticles

A superhydrophobic surface has many advantages in micro/nanomechanical applications, such as low adhesion, low friction and high restitution coefficient, etc. In this paper, we introduce a novel and simple route to fabricate superhydrophobic surfaces using ZnO nanocrystals. First, tetrapod-like ZnO nanocrystals were prepared via a one-step, direct chemical vapor deposition (CVD) approach. The nanostructured ZnO material was characterized by scanning electron microscope (SEM) and X-ray diffraction (XRD) and the surface functionalized by aminopropyltriethoxysilane (APS) was found to be hydrophobic. Then the superhydrophobic surface was constructed by depositing uniformly ZnO hydrophobic nanoparticles (HNPs) on the Poly(dimethylsiloxane) (PDMS) film substrate. Water wettability study revealed a contact angle of 155.4 +/- 2 degrees for the superhydrophobic surface while about 110 degrees for pure smooth PDMS films. The hysteresis was quite low, only 3.1 +/- 0.3 degrees. Microscopic observations showed that the surface was covered by micro- and nano-scale ZnO particles. Compared to other approaches, this method is rather convenient and can be used to obtain a large area superhydrophobic surface. The high contact angle and low hysteresis could be attributed to the micro/nano structures of ZnO material; besides, the superhydrophobic property of the as-constructed ZnO-PDMS surface could be maintained for at least 6 months. (C) Koninklijke Brill NV, Leiden, 2010

高电荷态离子~(207)Pb~(q+)(24≤q≤36)与Si(110)固体表面作用的电子发射研究

报道了利用兰州重离子加速器国家实验室ECR源引出的高电荷态离子207Pbq+(24≤q≤36)入射到Si(110)表面产生的电子发射的实验测量结果.结果表明,高电荷态离子与固体表面相互作用产生的电子发射产额Y与入射离子的电荷态q、入射角度ψ和入射能量E都有很强的关联.首次发现,电子发射产额Y与入射角度ψ间有接近1/tanψ的关系.理论分析认为,这些过程与基于经典过垒模型的势能电子发射过程密切相关.

Electron emission induced by the interaction of highly charged ions Pb-207(q+) (24 <= q <= 36) with solid surface of Si(110)

The electron emission induced by highly charged ions Pb-207(q+) (24 <= q <= 36) interacting with Si(110) surface is reported. The result shows that the electron emission yield Y has a strong dependence on the projectile charge state q, incidence angle psi and impact energy E. In fitting the experimental data we found a nearly 1/tan psi dependence of Y. Theoretical analysis shows that these processes are closely related to the process of potential electron emission based on the classical over-the-barrier model.

0.4-1.2A GeV能区重离子碰撞中的直接流系统性研究

直接流是研究重离子碰撞动力学演变和压缩形成的高密核物质性质很好的探针，本论文系统地研究了0.4、0.8和1.16A GeV的Ni+Ni和Pb+Pb碰撞中的直接流。实验是在德国重离子研究中心(GSI)的FOPI探测装置上完成的。论文中，简单总结了中高能区重离子碰撞的现状和描述集体流的主要理论模型，介绍了FOPI探测系统，给出了详细的实验数据分析过程，对所得到的物理结果进行了讨论。本论文工作的重点如下：基于FOPI系统的实验数据，发展了一套质量相关(Z=1离子)的直接流的提取方法。提取了各碰撞系统出射P、D和T粒子在不同碰撞中心度下的微分直接流和积分直接流。研究了P、D和T的直接流对碰撞中心度、系统尺寸和碰撞能量的依赖性，以及对核物质状态方程的敏感性。结果表明：直接流敏感地依赖于碰撞中心度，近中心碰撞具有更强直接流信号；对于轻重两种系统，用常用的AP1/3+AT1/3系数对积分直接流进行了标度，观察到一定的标度性，但不能完全标度；通过研究直接流对碰撞能量的依赖性发现，在0.4－1.2A GeV能区内，随能量升高，直接流在已经达到了饱和，并开始下降，并且P、D和T的变化趋势相同。实验数据与输运模型IQMD计算比较发现，直接流的变化趋势和最大密度变化趋势相同，说明直接流是核物质压缩程度的一个良好探针。计算得到的P、D和T微分和积分的V1值表明，与质量相关的直接流，无论是微分值还是积分值都敏感依赖于模型中EoS参数。比较发现，不同碰撞能量下，重的Pb+Pb系统的数据和软的EoS符合很好，说明核物质不可压缩系数在210 MeV附近，这与文献中的结果相吻合，说明与质量相关的直接流是EoS的敏感探针。对于轻Ni＋Ni系统，目前的IQMD还不能重现数据，但其趋向于硬的EoS，需要发展描述碰撞过程更为精细的理论模型。数据整体趋势表明，随者系统变重，中子比例的增加，EoS变软，难以给出同一组IQMD参数来同时解释全部的实验数据。对于所研究的碰撞系统，比较中心快度区斜率行为时发现，P、D和T的直接流与出射粒子质量数呈线性关系，并且出射粒子的积分直接流可以很好的用常数(A+1)/2进行标度。如果出射粒子的直接流用IQMD计算的核阻止进行归一，归一后的直接流与碰撞能量成正比。这证明核阻止与直接流有线性关联，反映了核阻止对于碰撞中核物质达到的最高密度起决定性的作用。论文工作的另一部分是完成了FOPI探测装置中飞行时间探测器的升级工作。研制了新型的玻璃MMRPC，完成了性能的批量测试，并研究了该探测器的高计数率行为。测量结果显示，在实验计数率(0.1 kHz/cm2)条件下，MMRPC时间分辨达到75 ps，探测效率达到98％。当计数率达到3－5 kHz/cm2时，时间分辨和探测效率降至约110 ps和75％。高计数率探测效率变差的幅度可以用DC模型进行解释，然而时间分辨的变化幅度用DC模型难以解释

Novel < 110 >-oriented organic-inorganic perovskite compound stabilized by N-(3-aminopropyl) imidazole with improved optical properties

In the organic-inorganic perovskites family, the < 100 >-oriented type has been extensively investigated as a result of its unique magnetic, optical, and electrical properties, and only one type of < 110 >-oriented hybrid perovskite stabilized by methylammonium and iodoformamidinium cations or the latter themselves has been known so far. In this paper, another novel < 110 >-oriented organic-inorganic perovskite (C6H13N3)-PbBr4 (compound 1) has been prepared by reacting N-(3-aminopropyl)imidazole (API) with PbBr2 in hydrobromic acid. The crystal structure is determined, which indicates that the perovskite is stabilized by API. The introduction of the optically active organic ligand API into the hybrid perovskite results in a red shift and a great enhancement of photoluminescence in the perovskite with respect to organic ligand API itself. These results have been explained according to calculation based on density-functional theory. Moreover, the excellent film processing ability for the perovskite (C6H13N3)PbBr4 together with the improved optical properties makes it have potential application in optoelectronic devices.

Nd_nSrFe_nO_(3n+1)(n=1,2,3,∞)的合成、结构、电性质和磁性研究

合成了NdnSrFenO3n+1(n=1,2 ,3,∞ ) 系列复合氧化物 ,其中Nd3SrFe3O10 是首次合成 ,并研究了其晶体结构 ,IR谱以及 30 0～ 110 0K之间的电性质和磁性质。相对于NdSrFeO4 ,Nd2 SrFe2 O7中ab平面上的Fe O键较短而c轴方向的Fe O键较长 ;而NdFeO3中只有一种Fe O键 ,在 30 0～110 0K之间 ,NdSrFeO4 ,显反铁磁性行为 ,Nd2 SrFe2 O7表现为亚铁磁性 ,而Nd3SrFe3O10 和NdFeO3为顺磁性。随着n值的增大 ,该系列氧化物电阻率增大 ,这可能是系统四价Fe离子浓度减小的结果。

方差-范围函数法求低密度聚乙烯/乙烯-丙烯-辛烯-1共聚物的共混体系次晶结构

将方差-范围函数法应用于共混体系中,求得了LDPE/EPO共混体系的(110)和(200)晶面的微晶大小和点阵畸变参数.微晶大小和点阵畸变参数值随EPO组份含量的增加基本呈下降趋势.

STRUCTURE OF 1,10-DIAMINODECANE TETRACHLOROZINCATE

[NH3(CH2)10NH3][ZnCl4], M(r) = 381.51, triclinic, P1BAR, a = 7.296 (1), b = 10.110 (3), c = 12.814 (4) angstrom, alpha = 90.84 (2), beta = 101.17 (2), gamma = 92.52 (2)-degrees, V = 926.13 angstrom 3, Z = 2, D(x) = 1.37 Mg m-3, lambda(Mo K-alpha) = 0.71073 angstrom, mu = 1.925 mm-1, F(000) = 396, T = 298 K, final R = 0.070 for 1237 unique reflections [I > 3-sigma(I)]. The structure is characterized by layers of inorganic ions sandwiched between layers formed by the paraffinic chains.

STRUCTURE OF CIS-DIAQUABIS(1,10-PHENANTHROLINE)ZINC SULFATE HEXAHYDRATE

[Zn(C12H8N2)2(H2O)2]SO4.6H2O, M(r) = 665.98, triclinic, P1BAR, a = 10.070 (4), b = 12.280 (3), c = 13.358 (2) angstrom, alpha = 109.12 (2), beta = 92.58 (2), gamma = 110.85 (2)-degrees, V = 1433.9 (7) angstrom 3, Z = 2, D(x) = 1.54 g cm-3, lambda(Mo K-alpha) = 0.71069 angstrom, mu = 10.1 cm-1, F(000) = 692, T = 293 K, R = 0.044 for 3985 observed reflections. The Zn atom is coordinated in a distorted octahedral geometry by four N atoms from two 1,10-phenanthroline (phen) ligands and two water molecules. The intermolecular ring-stacking interactions between the phen ligands occur in two forms: infinite chains and discrete dimers. Hydrogen bonds further stabilize the structure.

Coadsorption of nitric oxide and oxygen on the Ag(110) surface

The coadsorption of NO and O-2 on Ag(110) surface has been studied by X-ray photoelectron spectroscopy (XPS), ultraviolet photoelectron spectroscopy (UPS) and in situ Raman spectroscopy. The existence of oxygen enhances the adsorption of NO by forming the NOx species, that is, NO2 and NO3, and the NO in turn as a promotor facilitates the cleavage of the dioxygen bond, forming the surface atomic oxygen species having the same spectral characteristics as those produced using oxygen at high pressure. The oxygen species generated by the interaction is composed of two parts. One is produced directly by the decomposition of surface NO-O-2 complex at ca 625 K, which raised an O 1s feature at 530.5 eV and is absent at ca 800 K, while the another with an O 1s binding energy of 529.2 eV emerges at higher temperatures and shows similar properties as the reported gamma-state oxygen which bound tightly on restructured silver surface. The exposure to NO and O-2 causes noticeable changes in the morphology of the Ag(110) surface and the flat terraces superseded by small (ca 0.1 mu m) pits, and particles with typical diameters of a few micrometres were formed at elevated temperatures. (C) 1999 Elsevier Science B.V. All rights reserved.