Observation of F = 2 Spinor Bose-Einstein Condensation in a Magnetic Field

Multiple-component Bose-Einstein condensation has been observed in a magnetic field generated by a controllable magnetic quadrupole-Ioffe-configuration trap. Different distributions of atoms in spinor Bose Einstein condensates are created by changing the time difference of switching-off current in quadrupole-Ioffe-configuration coils and bias coils of the magnetic trap. A simple analysis is carried out to explain some phenomena of the experiment.     

对钠与浓硫酸铜溶液反应发生着火原因的探究

正钠遇到浓的硫酸铜溶液时会迅速发生着火(并伴有爆炸),着火的原因主要有以下3个方面:(1)着火是由于硫酸铜溶液呈酸性引起的;(2)着火是由于浓的硫酸铜溶液黏度比较大引起的;(3)着火是由于生成的氢氧化铜沉淀引起的。那么究竟是什么呢?笔者进行了实验探究。1钠的着火是否是由酸性引起的硫酸铜溶液水解呈酸性,经测试常温下饱和硫酸铜溶液的pH约为3。为了研究钠的着火是否是由酸性引起的,我们选取了不产生沉淀且酸性更强的溶液进行实验。【实验1】向2个烧杯(规格125mL)中,分     

3,4,5-三甲氧基苯甲酸酯化壳聚糖的紫外吸收性能研究

将壳聚糖在甲磺酸中充分溶胀后,与3,4,5-三甲氧基苯甲酰氯反应,得到壳聚糖改性高分子紫外 线吸收剂。FTIR的表征表明:与壳聚糖相比,改性产物的红外谱图中1 720 cm-1处归属于C=O伸缩振动和 1 160 cm-1处归属于C-O-C对称伸缩振动的吸收峰显著增强,表明了酯化反应的发生。紫外光谱表明:产 物在220nm和274nm处具有较强的吸收峰。通过元素分析计算出不同投料比下所得改性产物的取代度,并 结合紫外光谱测试所得的数据,计算出了改性产物在273 nm处的摩尔消光系数e为8 205.9 L／(mol·cm)。     

黑体热辐射的光波长定义域研究

对黑体热辐射的光波长定义域进行了深入研究．结果表明,热辐射光波长定义域与温度和计算精度因子有关,温度越低,精度因子越大,长波长界越长;温度越高,精度因子越大,短波长界越短;由光波长定义域引起的热辐射功率计及误差与温度无关,且精度因子大于3时,该误差便小于万分之几．     

一维边发射有机半导体光子晶体激光器设计

基于有机共轭聚合物聚[2-甲氧基-5-(2-乙基己氧基)-1,4-苯乙炔](MEH-PPV)的脊形波导,利用光子晶体特殊的光调制特性,模拟设计了一维边发射有机光子晶体激光器。利用光子晶体的带隙结构和带边效应构建了由光子晶体全反镜和透反镜形成的谐振腔,在谐振腔内的脊形波导上引入一维缺陷型光子晶体,利用光子晶体缺陷模特性抑制了多纵模竞争,并在此基础上分析了复合结构所导致的边界模效应,得出此类非金属微腔激光器腔长设计的经验公式。模拟结果表明该一维边发射有机光子晶体激光器可实现中心波长为588nm、半峰全宽为0.131nm的单纵模激光输出。     

基于Julia分形的多涡卷忆阻混沌系统

忆阻器作为一种非线性电子元件,能用作混沌系统中的非线性项,从而提高系统的复杂度.分形与混沌是密切相连的,分别对两者的研究都已成熟,却鲜有将分形过程应用到混沌系统中,以产生丰富的混沌吸引子.为了探索将分形与混沌系统相结合的可能性,本文首先提出了一个新的忆阻混沌系统,并从对称性、耗散性、平衡点稳定性、功率谱、Lyapunov指数和分数维等方面探讨了系统的动力学特性;紧接着,把经典的Julia分形过程应用到该忆阻混沌系统中,产生了新的混沌吸引子,并将几种由Julia分形衍生的变形Julia分形过程应用于文中提出的忆阻混沌系统,获得了丰富的混沌吸引子;最后,讨论了分形过程中的复常数对系统的影响.从仿真结果可以看出,分形过程与混沌系统的结合能产生丰富的多涡卷混沌吸引子.这不仅为产生多涡卷混沌吸引子提供了一种新方法,还弥补了使用功能函数方法造成混沌系统不光滑的不足.     

基于环形微腔的多频段三角晶格光子晶体耦合腔波导光学传输特性

本文理论研究了近红外波段硅基三角晶格光子晶体环形微腔的光场局域特性,通过将微腔在空间周期性排列组成耦合腔光波导,研究了多个导带区域内光束传输时的群速度,最大和最小值分别为0.0028c和0.00028c.将环形微腔在垂直于光传输方向上进行交错排列,通过改变相邻微腔之间的耦合区域,可以大幅降低多频段范围内光束在耦合腔波导中传输时群速度之间的差异,并提高部分频段的透过率数值.在不改变介质柱半径条件下,通过去掉三角晶格光子晶体中距中心介质柱距离分别为2a和√3a的六个介质柱构成了两种微腔,研究了两种微腔所支持的谐振波长之间的差异,在此基础上构造了两种耦合腔波导,进而将这两种耦合腔光波导与W1型输入/输出波导相连,最终实现了在多个不同频率范围内降低群速度的同时实现频段选择和频段分束功能,其导模群速度可降低到0.00047c.     

The quantum spectral analysis of the two-dimensional annular billiard system

Based on the extended closed-orbit theory together with spectral analysis, this paper studies the correspondence between quantum mechanics and the classical counterpart in a two-dimensional annular billiard. The results demonstrate that the Fourier-transformed quantum spectra are in very good accordance with the lengths of the classical ballistic trajectories, whereas spectral strength is intimately associated with the shapes of possible open orbits connecting arbitrary two points in the annular cavity. This approach facilitates an intuitive understanding of basic quantum features such as quantum interference, locations of the wavefunctions, and allows quantitative calculations in the range of high energies, where full quantum calculations may become impractical in general. This treatment provides a thread to explore the properties of microjunction transport and even quantum chaos under the much more general system.     

温度对SiO2表面上磁控溅射制备Ge纳米点的生长模式和尺寸的影响

采用磁控溅射技术在SiO2/Si(100)表面上制备了一系列不同生长温度的Ge纳米点样品.原子力显微镜(AFM)的实验结果表明:不同衬底温度下Ge纳米点在SiO2薄膜上的生长模式和尺寸分布有所不同.当衬底生长温度达到500 ℃时,SiO2开始与Ge原子发生化学反应,并形成"Ge纳米点的Si窗口".在此温度条件下,外延生长实验可获得尺寸均匀且密度高达3.2×1010 cm-2的Ge纳米点.     

Engineering the light propagating features through the two-dimensional coupled-cavity photonic crystal waveguides

This paper studies the propagating characteristics of the electromagnetic waves through the coupled-resonator optical waveguides based on the two-dimensional square-lattice photonic crystals by the finite-difference time-domain method.When the traditional circular rods adjacent to the centre of the cavities are replaced by the oval rods,the simulated results show that the waveguide mode region can be adjusted only by the alteration of the oval rods’ obliquity.When the obliquity of the oval rods around one cavity is different from the obliquity of that around the adjacent cavities,the group velocities of the waveguide modes can be greatly reduced and the information of different frequencies can be shared and chosen at the same time by the waveguide branches with different structures.If the obliquities of the oval rods around two adjacent cavities are equal and they alternate between two values,the group velocities can be further reduced and a maximum value of 0.0008c(c is the light velocity in vacuum) can be acquired.