GENERATION OF ENTANGLED FOCK STATES OF TWO NONLOCAL CAVITY MODES WITH DIFFERENT FREQUENCIES

We present a method to generate entangled Fock states of two nonlocal cavity modes with different frequencies. We send an atom with three levels g,e, and f across two cavities. The atomic transition frequency between level g and e is resonant with the first cavity frequency, while the atomic transition frequency between level g and f is resonant with the second cavity frequency. The detection of the atomic state leaves the pure field in an entangled Fock state.     

四元Heisenberg群上次拉普拉斯算子的m幂次的基本解

本文研究了四元Heisenberg群上次拉普拉斯算子的m幂次的基本解，该结论是Heisenberg群上结果的推广.本文利用了四元Heisenberg群上的Fourier变换理论构造了该群上次拉普拉斯算子的m幂次的基本解，并且给出了基本解的积分表示.     

New efficient reaction media for SET‐LRP produced from binary mixtures of organic solvents and H2O

SET‐LRP is mediated by a combination of solvent and ligand that promotes disproportionation of Cu(I)X into Cu(0) and Cu(II)X₂. Therefore, the diversity of solvents suitable for SET‐LRP is limited. SET‐LRP of MA in a library of solvents with different equilibrium constants for disproportionation of Cu(I)X such as DMSO, DMF, DMAC, EC, PC, EtOH, MeOH, methoxyethanol, NMP, acetone and in their binary mixtures with H₂O was examined. H₂O exhibits the highest equilibrium constant for disproportionation of Cu(I)X. The apparent rate constant of the polymerization exhibits a linear increase with the addition of H₂O. This is consistent with higher equilibrium constants for disproportionation generated by addition of H₂O to organic solvents. Furthermore, with the exception of alcohols and carbonates, the rate constant of polymerization in binary mixtures could be correlated with the Dimroth‐Reichardt solvent polarity parameter. This is consistent with the single‐electron transfer mechanism proposed for SET‐LRP that involves a polar transition state. These experiments demonstrate that the use of binary mixtures of solvents with H₂O provides a new, simple and efficient method for the elaboration of a large diversity of reaction media that are suitable for SET‐LRP even when one of the two solvents does not mediate disproportionation of Cu(I)X. © 2009 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 5577–5590, 2009     

Ce-Pt-Pd/不锈钢丝网催化剂的制备与催化性能

采用阳极氧化技术在不锈钢丝网上自生长了一层结构致密的阳极氧化膜,并以此为载体,制备出一种高活性、高稳定性的负载型Ce-Pt-Pd催化剂.考察了该系列催化剂对甲苯、丙酮和乙酸乙酯的氧化活性,并用扫描电镜、X射线光电子能谱和程序升温氧化技术对催化剂进行了表征.结果表明,不锈钢丝网载体表面自生长的氧化物膜十分有利于活性组分的负载,制得的催化剂具有较高的催化燃烧有机化合物的活性和稳定性.     

2008年南方冰灾输电塔损毁原因调查与分析

以2008年受冰灾较为严重的湖南省郴州市为例,基于实地调查所取得的大量资料,剖析了2008年1月以来由于冰覆引起的大量输电塔倒塌的主要原因.研究表明：严重覆冰所引起的输电塔超载、输电塔布局不合理所引起的不平衡力等是造成冰雪灾害中大量输电塔倒塌的主因;同时提出了输电塔设计改进的建议,为最大限度减少类似灾害造成输电塔损失提供参考.     

非晶态金属Al中微团簇多面体结构及其演变规律的模拟研究

对50 000个金属Al原子从液态急冷形成非晶态结构的过程进行了分子动力学模拟研究.采用原子键型和原子团簇类型指数法,发现在其微观结构的转变过程中,与不断增加的1551键型密切相关的二十面体及其缺陷结构的形成起了非常突出的作用.通过各种键型原子团簇的计算,获得团簇多面体结构的分布数据.在可视化的显示下,得到一幅十分清晰的关于团簇多面体结构的特征及其演变的图景.建立了一种简单而有效的团簇多面体结构研究方法.同时也对模拟计算结果的微观机理给出了相应的讨论,这对于深入理解非晶态结构的形成机制及其微观过程,将有重     

二维组装纳米银粒子上对巯基苯胺的表面增强拉曼光谱研究

采用表面自组装方法在聚赖氨酸修饰ITO电极表面和对巯基苯胺修饰光滑银表面组装了纳米银粒子的二维结构。FT -SERS光谱结果表明 ,巯基苯胺的吸附取向垂直于金属银表面 ,其中电磁增强机理起主导作用 ,但同时也存在化学增强的贡献。纳米银粒子的“体积效应”使其与吸附分子间的电荷转移更为有利。耦联于纳米银和光滑银表面间的巯基苯胺的拉曼散射增强则与纳米银粒子和光滑银表面的耦合而导致的局部电磁场增强直接相关。     

煤燃烧过程中汞、砷、硒反应机理研究

本文以三种典型煤为对象,测定了煤及灰中汞,砷,硒的浓度,了解了元素的挥发性。对钱家营褐煤进行了不同温度的燃烧实验。测定了在不同温度下燃烧灰中汞,砷,硒的含量变化。将所得实验结果与化学热力平衡分析工具F~*A~*C~*T2.1模拟系统结果相比较。推测了其中可能发生的反应。     

自组织InAs/GaAs量子点垂直排列生长研究

利用自组织生长InAs/GaAs量子点的垂直相关排列机制，生长了上下两层用6.5nm GaAs间隔的InAs结构.下层InAs已经成岛，由于应力传递效应，上层InAs由二维生长向三维成岛生长的转变提前发生，临界厚度从1.7ML变成小于1.5ML.透射电子显微镜截面象显示形成上下两层高度差别很大的InAs量子点，但是由于两层量子点之间存在强烈的电子耦合，光致发光谱中只有与包含大量子点的InAs层相对应的一个发光峰.     

Efficient Scheme for the Generation of Atomic Schrodinger Cat States in an Optical Cavity

An efficient scheme is proposed for the generation of atomic Schrodinger cat states in an optical cavity. Inthe scheme N three-level atoms are loaded in the optical cavity. Raman coupling of two ground states is achieved via alaser field and the cavity mode. The cavity mode is always in the vacuum state and the atoms have no probability ofbeing populated in the excited state. Thus, the scheme is insensitive to both the cavity decay and spontaneous emission.