基于干涉条纹跟踪实现纳米级位移测量的方法研究

设计了一套干涉条纹图像实时采集处理系统。在分析迈克尔逊干涉条纹特征表象的基础上 ,给出了通过跟踪干涉条纹的移动量测量被测对象纳米级位移量的理论公式 ;提出了干涉条纹特征点的提取与跟踪算法 :分段线性变换、方形窗口中值滤波和门限化边缘提取 ,给出了基于统计学原理的通过计算多条干涉条纹移动量获得被测对象纳米级位移量的计算公式。实验结果表明了该方法的有效性和实用性     

用于准相位匹配的LD泵浦Nd:YAG946nm连续激光光源

本文为泵浦质子交换准相位匹配波导器LiNbO₃提供了激光光源,用808nm半导体激光器泵浦Nd:YAG晶体,在室温下获得946nm激光连续输出大于120mW,斜率效率9.8%,并且在国内首次实现了LD泵浦Nd:YAG/KNbO₃473nm蓝色激光器的连续运转,报道了初步的实验结果并对此进行了详细的分析,提出了改进方案.     

锕系双原子分子的从头算研究

用相对论有效原子实势（RECP）和密度泛函方法（B3LYP）,采用U和Pu原子的紧缩价基集合[5s4p3d4f]/[3s3p2d2f],优化了U2和Pu2分子的平衡结构,得到它们的键长（LBL）和短键长（SBL）分别为：U2分子是0．38965和0．29927nm,Pu2分子是0．45375和0．35202nm;导出了基态和最低激发态的势能函数,计算出它们的力常数、光谱数据和离解能。     

用于较大泵浦尺寸半导体泵浦固体激光器的一种特殊腔型

提出一种泵浦固体激光器的特殊腔型,解决了当功率较大时泵浦尺寸较大使得泵浦光斑与激光光斑不匹配的问题,并从激光腔理论和速率方程理论两方面通过数值计算验证了该腔型的优越性.同时对LD泵浦固体激光器以及倍频的设计提出了几条普适原则.     

CALCULATION OF THE FINE STRUCTURE OF OXYGEN-LIKE IONS USING THE POLARIZATION POTENTIAL FUNCTION

We have calculated the forbidden transition energies and magnetic dipole transition probabilities of 2s²2p⁴(³P₁－³P₂) and 2s²2p⁴ (³P₀－³P₁) of oxygen-like isoelectronic sequences (Z=10－32) by a method of polarization potential correction. The transition energies show good agreement with experiment and are much better than the calculations in the literature. These results also illustrate that it is feasible to use the dipole expansion of the polarization potential to deal with some dynamic and non-dynamic effects in the central field approach. The relation of polarizability and cut-off radius with atomic number is discussed. We also give the fitted formula between the polarizability α₁ and atomic number Z as α₁=0.73429-9.56644×10^-4Z+7.43016×10^-5Z^{2-2.53298×10-6Z3+2.08306×10-8Z4.}     

β-环糊精与CTAB微乳液协同增敏荧光法测定微量铋研究

β-环糊精与CTAB微乳液协同增敏荧光法测定微量铋研究;铋（Ⅲ）;β-环糊精;微乳液;增敏;荧光分析法     

薄层色谱扫描法测定塑料食品袋中酞酸酯的含量

建立了采用薄层色谱扫描测定塑料食品袋中4种酞酸酯(酞酸二甲酯(DMP)、酞酸二乙酯(DEP)、酞酸二丁酯(DBP)和酞酸二(2-乙基己基)酯(DEHP))的方法。经粉碎的样品先用乙醇浸泡24 h,然后超声提取,经0.45 μm滤膜过滤。点样在以丙酮处理过的硅胶G板上,以乙酸乙酯-无水乙醚-异辛烷(体积比为1∶4∶15)为展开剂展开,以双波长反射吸收飞点扫描测定(λS=275 nm,λR=340 nm),外标法定量。该法的线性关系较好,DMP、DEP、DBP和DEHP的检出限分别为2.1,2.4,3.4和4.0 ng,混合标准品在同一薄层板上的峰面积的相对标准偏差（RSD）为2.8%～3.5%,4种酞酸酯的样品加标回收率为78.58%～111.04%。该方法样品用量少,前处理简单,分离效果好,可用于塑料袋中4种酞酸酯的同时测定。经与气相色谱法的分析结果比较,两种方法对实际样品的分析结果接近。     

SOFC阳极阻挡层La0.3Ce0.7O2-δ薄膜的制备

镓酸镧基SOFC存在的关键问题是在阳极/电解质界面发生固相反应生成绝缘相,一个根本的解决办法是在阳极与电解质之间制备一层薄且致密的阻挡层La0.3Ce0.7O2-δ(LDC30).本文采用共沉淀法制备了LDC30的前驱体,高温煅烧后,通过XRD分析和粒度分布测试,表明La2O3成功地掺杂到CeO2晶格中,制得了粒径较小的纯相LDC30粉体,并确定了最佳的煅烧条件是在1000℃下煅烧2h.采用丝网印刷法将阻挡层浆料涂覆在电解质表面并高温烧结,通过烧结收缩曲线及微观形貌观测,发现在1400℃时烧结2h可以成功的制备一层厚约10μm的致密的阻挡层薄膜,将电池的放电性能提高了44;.     

The splitting of low-lying states for hydroxyl molecule under spin--orbit coupling

The splitting of potential energy curves for the states $X^{2}\Pi _{3/2}$, $^{2}\Pi _{1/2}$ and $A^{2}\Sigma ^{ +}$ of hydroxyl OH under spin--orbit coupling (SOC) has been calculated by using the SO multi-configuration quasi-degenerate perturbation theory (SO-MCQDPT). Their Murrell--Sorbie (M--S) potential functions have been derived, then, the spectroscopic constants for $X^{2}\Pi _{3/2}$,$^{ 2}\Pi _{1/2}$ and $A^{2}\Sigma ^{ + }$ have been derived from the M--S function. The calculated dissociation energies for the three states are $D_{0}$[OH($X^{2}\Pi _{3/2})$]=34966.632cm$^{-1}$, $D_{0}$[OH($^{2}\Pi _{1/2})$]=34922.802cm$^{-1}$, and $D_{0}$[OH($A^{2}\Sigma ^{ + })$]=17469.794cm$^{-1}$, respectively. The vertical excitation energy $\nu [ {{ }^2\Pi _{1/2} ( {\nu = 0} ) \to {X}{ }^2\Pi _{3/2} ( {\nu = 0} )} ] = 139.6{\rm cm}^{-{\rm 1}}$. All the spectroscopic data for the $X^{2}\Pi _{3/2}$ and $^{2}\Pi _{1/2 }$ are given for the first time except the dissociation energy of $X^{2}\Pi _{3/2}$.     

Variation of dielectronic satellite intensity factors with n for dielectronic recombination processes in selected lithium—like ions

Satellite intensity factors F^*₂(s→f) have been calculated for the 1s²2s+εl→(1s²3l′nl″)^*→1s²2sml''+hν dielectronic recombination processes of lithium-like V, Cu, Se, Ag and Ba ions. The relevant atomic parameters have been calculated explicitly for all intermediate resonance states |s〉≡|1s²3l′nl″SLJ〉 with n=3－9 in the intermediate coupling scheme. The 1/n³ scaling, which has often been used in extrapolating F^*(s→f) for n≥4, is tested against these values of F^*₂(s→f).