软X射线多层膜色散元件

介绍研制软Ｘ射线多层膜色散元件的初步结果，结合Ｍ０／Ｓ１、Ｓ／Ｓ１色散元件的研制实例，讨论了包括设计、性能模拟计算、镀膜工艺、检测等在内的制备过程，这些元件将在Ｘ射线光学和Ｘ射线光谱学的有关研究工作中得到应用。     

An Experimental Study of In-Situ Phase Fraction in Jet Pump Using Electrical Resistance Tomography Technique

We perform the experiments to investigate in-situ phase fraction in a jet pump using the electrical resistance tomography （ERT） technique. A new jet pump with ERT sensors is designed to measure in-situ phase fraction and flow regime. The study is based on laboratory experiments that are carried out on a 50-mm vertical flow rig for various gas and liquid phase superficial velocities. The different flow patterns of gas liquid in the jet pump and vertical pipe are studied using the ERT technique. The results suggest that the ERT system can be used to successfully produce images of gas-liquid flow patterns with frames rates of 58 fps and the in-situ phase fraction with frame rates of 5 fps can be obtained. The visualizations of a rapid mixing process in the throat of a jet pump obtained in this work provide a reliable basis for theoretical study and optimal design of jet pumps.     

Electron Transport Property of CdTe under High Pressure and Moderate Temperature by In-Situ Resistivity Measurement in Diamond Anvil Cell

In situ resistivity measurement has been performed to investigate the electron transport property of powered CdTe under high pressure and moderate temperature in a designed diamond anvil cell. Several abnormal resistivity changes can be found at room temperature when the pressure increases from ambient to 33 GPa. The abnormal resistivity changes at about 3.8 GPa and 10 GPa are caused by the structural phase transitions to the rock-salt phase and to the Cmcm phase, respectively. The other abnormal resistivity changes at about 6.5 GPa, 15.5 GPa, 22.2 GPa and about 30 GPa never observed before are due to the electronic phase transitions of CdTe. The origin of the abnormal change occurred at about 6.5 GPa is discussed. The temperature dependence of the resistivity of CdTe shows its semiconducting behaviour at least before 11.3 GPa.     

La－Th－O系催化剂的结构与甲烷氧化偶联催化性能的关系

研究了Ｌａ－Ｔｈ－Ｏ二元氧化物的组成、结构及其对甲烷氧化偶联反应催化性能的影响；用ＸＲＤ、ＩＲ、ＸＰＳ、ＳＥＭ等方法对催化剂进行表征。Ｌａ－Ｔｈ－Ｏ系列催化剂随Ｌａ／Ｔｈ原子比的变化，可生成Ｌａ＿ｘＴｈ＿（１－ｘ）Ｏ＿（２－δ）固溶体。具有萤石结构的Ｌａ＿ｘＴｈ＿（１－ｘ）Ｏ＿（２－δ）是甲烷氢化偶联反应的主要活性相。     

甲烷氧化偶联含锂多元复合氧化物催化剂的失活机理

对甲烷氧化偶联反应活性较高的多元复合氧化物催化剂（Ｌｉ－Ｔｉ－Ｌａ，Ｌｉ－Ｍｎ－Ｌａ，Ｌｉ－Ｎｉ－Ｌａ）的稳定性和失活机理进行了初步探讨，利用ＸＲＤ，ＩＲ，ＸＰＳ和Ｏ２－ＴＰＤ等方面对催化剂进行了表征，结果表明，催化剂在高温及反应气氛的作用下，表面锂的流失，使体相晶格中的锂向表面扩散，导致含锂活性相结构的分解（或部分分解），从而减少了体相相氧空位和生氧种的数量，降低了晶格氧的活动性，致使催化剂活必     

共缩聚聚酰胺胶囊的制备及其性质的研究

界面缩聚法是制备微胶囊的常用办法之一,在医药、农药、生物工程等各个领域得到了广泛的研究与应用.此法制备聚酰胺胶囊具有制备方法简单、缩聚速度快、囊壁孔隙大等优点.在制备胶囊时,一般以一种二元胺或多元胺作为水溶性单体,制备的微胶囊存在很大的缺陷.当用二元胺作为水溶性单体时,得到具有线型结构的聚酰胺胶囊,囊壁的机械强度差.采用多元胺作为水溶性单体时,反应深度小,制备的胶囊囊壁薄、孔隙小.我们采用二元胺和多元胺的混合物作为水溶性单体,得到了不规则缩聚的共缩聚胶囊.改变二元胺与多元胺的比例,改善囊壁的机械强度和对KCl 的渗透系数,从而制备出具有较高机械强度和较大渗透系数的胶囊,以适应实际应用中对芯材控制释放的要求.     

Bi-Mo-Nb复台氧化物的结构与对丙烯氧化的催化活性

本文用XRD,IR,Raman,SEM和ESR等方法研究了系列氧化物Bi_2Mo_(3-3x)Nb_(2x)O_(12-4x)(X=0.00,0.02,0.05,0.10,0.15,0.20,0.25)的结构和对丙烯氧化的催化活性,结果表明,在X≤0.25范围内,催化剂基本保持典型的α-Bi_2Mo_3O_(12)结构,少量Nb~(5+)的掺杂,可取代晶格中的Mo~(6+),产生氧空位,无序分布的氧空位的浓度先随X值的增加而增加,当X=0.15时达最大值,催化剂对丙烯氧化的催化活性与这种氧空位的浓度成正比,反应遵循Redox机理.     

5-巯基-1, 3, 4-噻二唑-2-硫酮微溶剂团簇的光谱和理论计算研究

微溶剂作用(即溶剂化过程)广泛存在于所有物理、 化学和生命过程中. 在液相化学反应体系中, 几乎是一切化学反应的基础. 通过傅里叶变换拉曼光谱(FT-Raman)并结合密度泛函理论(DFT), 表征了固态5-巯基- 1, 3, 4-噻二唑-2-硫酮(MTT)的结构, 并进一步确认了MTT在乙腈、 甲醇和水中微溶剂团簇的大小和氢键位点. 通过探究MTT在不同溶剂及pH条件下的紫外-可见吸收光谱(UV-Vis), 结合含时密度泛函理论(TD-DFT)计算, 揭示了溶剂和pH对MTT电子跃迁带的影响, 进一步解释了其光谱位移. 结合能量计算可以得出, MTT分别与1个乙腈、 2个甲醇和2个水分子形成MTT(CH₃CN), MTT(CH₃OH)₂ 和MTT(H₂O)₂团簇.