分布反馈式光纤激光器的光热调谐方法

针对现有光纤激光器调谐方法通常不能兼顾调谐幅度和调谐速率的问题,提出了一种基于光热效应的调谐方法,有效兼顾了调谐幅度和调谐速率的要求。分析了光纤激光器的输出波长随泵浦功率变化而改变的实验现象,并以980 nm泵浦源自身调谐为例,进行了静态和动态实验,结果表明:基于光热效应的分布反馈式光纤激光器静态调谐幅度达392 MHz/100 mA,动态调谐速率超过2 kHz,验证了光纤激光器光热调谐方案的可行性。     

孔雀绿与磷钒钼杂多酸显色反应的研究

在稀H2SO4介质中,磷酸盐与钼酸盐和偏钒酸盐反应形成磷钒钼杂多酸,杂多酸再与孔雀绿缔合形成四元有色络合物,能稳定存在于含聚乙烯醇的水溶液中。缔合物的最大吸收位于590nm波长处,摩尔吸收系数ε=1.7×105L·mol-1·cm-1,P(V)的质量浓度在0～0.12μg mL范围内与吸光度成正比。研究了显色反应的适宜条件、共存离子的影响和缔合物的组成。方法已用于合成试样中磷的测定。     

2′-(2-噻吩亚甲基)-2-羟基苯甲酰腙钴(Ⅲ)配合物的合成、表征及晶体结构

In ethanol, a mononuclear cobalt(Ⅱ) complex incorporating 2′-(2-Thienylidene)-2-Hydroxybenzoylhydra-zide has been synthesized and characterized by IR, UV-Vis, elemental analysis and X-ray crystal structure analysis. The crystal belongs to triclinic system, space group P1 with cell constant, a=1.230 69(10) nm, b=1.329 18(11) nm, c=1.330 56(11) nm, α=113.702(2)°, β=91.590(2)°, γ=100.846(2)°, V=1.944 4(3) nm³, Z=2, μ=0.662 mm^-1, D_c=1.482 g·cm^-3, F(000)=896, R_int=0.048 7. The crystal structure shows an anionic didentate ligand O and N donors in this work. The cobalt(Ⅲ) atom is hexacoordinated with oxygen atom from keto group and nitrogen atom from amide to form a cobalt atom for the core octahedral structure. CCDC: 748882.     

金纳米粒子的共振散射光谱

采用Frens 法制备了粒径为10～95 nm的金纳米粒子.它们均在580 nm处产生一个共振散射峰.从液相纳米粒子的波动观点出发,解释了金纳米粒子共振散射光谱的产生原因.用超分子界面能带理论解释了金纳米粒子的颜色与粒径的关系.根据最大吸收波长与粒径的关系,建立了一种测量金纳米粒子粒径的光度标尺.     

ZrO2前体的制备方法对WOX-/ZrO2

考察了ZrO2前体的制备方法对WOX-/ZrO2的性质及其正庚烷临氢异构化反应性能的影响,同时采用BET、XRD、Py-IR等手段对其进行了表征.结果表明,ZrO2前体的制备方法会明显影响ZrO2前体的比表面积及WOX-/ZrO2催化剂中四方ZrO2和单斜ZrO2晶型的比例,同时WO3的分散程度也有差异.单斜ZrO2太多及WO3晶型的出现会降低正庚烷临氢异构化反应活性;而ZrO2全部为四方晶型时,虽然有利于提高低温反应活性,但缺点是裂解选择性太高;而当单斜ZrO2和四方ZrO2共存,但以四方ZrO2为主,且没有WO3晶型出现时,既可保持较高的反应活性,同时又具有极高的异构化选择性.     

三维虚拟层合板壳单元及其应用

层合结构已广泛应用于各类工程领域。文中介绍的三维虚拟层合板壳单元,其主要特点是它允许同一单元由不同材料构成,有限元网格划分时可以把整体节点定义在结构的外部。这就使得该单元不仅可以应用于一般的层合结构计算,而且还可以应用于结构的形状优化设计。文中的经典算例说明了该单元的有效性。     

双材料单伸臂叠合梁的界面滑移与自振特性分析

将叠合梁划分为接触区和分离区,接触区界面间的摩擦作用会对叠合梁的滑移、刚度和自振频率产生影响。本文给出了单伸臂叠合梁在均布荷载和集中力作用下,考虑叠合界面摩擦作用的滑移应变和滑移分布的表达式;推导了考虑叠合界面间摩擦力及摩擦力产生的抵抗弯矩共同作用下的截面刚度。假设梁按等波长和等刚度两种形式自由振动,运用传递矩阵法推导出了单伸臂叠合梁自振频率的计算公式。最后,基于一个钢-混凝土组合与叠合试验梁的算例分析了滑移沿梁长的分布及自振频率。结果表明:随界面间摩擦系数的增大,接触区界面的滑移值逐渐减小;摩擦效应对叠合梁自振频率的影响随阶次的升高越来越明显。     

室温固相反应制备Keggin结构K_3PW_(12)O_(40)·10H_2O纳米粒子

采用室温固相反应制备 Keggin结构钨磷酸钾纳米粒子 ,并通过元素分析、红外光谱、X射线衍射、电镜等进行了表征     

Application of multi-pulse optical imaging to measure evolution of laser-produced counter-streaming flows

A counter-streaming flow system is a test-bed to investigate the astrophysical collisionless shock(CS) formation in the laboratory. Electrostatic/electromagnetic instabilities, competitively growing in the system and exciting the CS formation, are sensitive to the flows parameters. One of the most important parameters is the velocity, determining what kind of instability contributes to the shock formation. Here we successfully measure the evolution of the counter-streaming flows within one shot using a multi-pulses imaging diagnostic technique. With the technique, the average velocity of the high-density-part(ne ≥ 8–9 × 10~(19)cm~(-3)) of the flow is directly measured to be of ～ 10~6cm/s between 7 ns and 17 ns.Meanwhile, the average velocity of the low-density-part(ne ≤ 2 × 10~(19)cm~(-3)) can be estimated as ～ 10~7cm/s. The experimental results show that a collisionless shock is formed during the low-density-part of the flow interacting with each other.     

Bow shocks formed by a high-speed laser-driven plasma cloud interacting with a cylinder obstacle

A bow shock is formed in the interaction of a high-speed laser-driven plasma cloud with a cylinder obstacle. Its temporal and spatial structures are observed by shadowgraphy and interferometry. The width of the shock transition region is ～ 50 μm, comparable to the ion–ion collision mean free path, which indicates that collision is dominated in the shock probably. The Mach-number of the ablating plasma cloud is ～ 15 at first, and decreases with time resulting in a changing shock structure. A two-dimension hydrodynamics code, USim, is used to simulate the interaction process. The simulated shocks can well reproduce the observed.