Gd3+对Ca0.8Zn0.2TiO3:Pr3+红色发光材料的敏化作用

采用溶胶-凝胶法在较低温度下合成了红色发光材料Ca0.8Zn0.2TiO3:0.002Pr3 ,xGd3 .金属离子预先溶解含有柠檬酸的乙二醇溶液中.XRD表明在800℃灼烧2h形成了钛酸盐的晶体.荧光检测结果表明所合成样品的特征激发峰为330nm、特征发射峰为614nm,分别对应于O(2p)→Ti(3d)带间跃迁和Pr3 的1D2→3H4的特征发射.样品的发光强度随x的不同而不同,发光强度增强了29%-69%.当x＝0.0005时,即nPr3 :nGd3 ＝4∶1时样品的红色发光强度最强,发光强度增强了69%.     

A New Type of Terahertz Waveguides

A new type of THz waveguides, which employs a solid polyethylene rod as the core and polyethylene tubes in a periodic array of square lattice as the cladding, is proposed. Optical properties of this new THz waveguide, especially in dispersion, confinement loss and single mode property, are investigated in detail with the plane wave expansion method and the beam propagation method. Numerical results demonstrate that the new THz waveguide can reach not only low dispersion but also low confinement loss at single mode propagation. Therefore, the square lattice structure is a better candidate as THz waveguides than the triangular ones.     

正确认识分运动的相互关系及其对合运动的贡献——再谈运动的合成和分解

当我们将一个较为复杂的运动视为物体同时参与的几个分运动进行讨论时，应该明确，这些分运动既具有相对的独立性，又具有相互联系的运动等时性．它们无主从之分，共同决定着合运动的性质、效果．     

Langevin Simulation of Non-Uniform Granular Gases

We present and study a fractal model of a non-uniform granular system for the first time, based on which wenumerically solve the dynamics actions in the system successfully in one-dimensional case. The multi-mixture is composed of N different particles, whose granularity distribution has the fractal characteristic. The particles are subject to inelastic mutual collisions and obey to Langevin equation between collisions. Far from the equilibrium,i.e. the given typical relaxation time τ of the driving Brownian process is much larger than the mean collision time τc, the results of simulation indicate that the degree of inhomogeneity in the granularity distribution signed by the fractal dimension D of size distribution has great influence on the dynamics actions of the system. The velocity distribution deviates obviously from the Gaussian distribution and the particles cluster more pronouncedly with the larger value of D in the system. The velocity distribution and spatial clnsterization change with D are presented.     

N-1,1''''-(3,3''''-二羧基-4,4''''-联苯撑)-双-(3-N-羟基-3-N-苯基三氮烯)的合成、结构表征及对钼(Ⅵ)的显色反应

1引言 近年来,利用构效关系寻找特效试剂已成为国内外研究的热门课题.改变物质的组成和结构是寻找高灵敏度、高选择性试剂的重要途径.N-1,1'-(3,3'-二羧基-4,4'-联苯撑)-双-(3-N-羟基-3-N-苯基三氮烯),是目前报道的对镍、铜灵敏度最高的显色剂,常用于镍、铜离子的定性检测.由于该物质的水溶性不好,不能在光度分析上应用.本文介绍在联苯苯环对应的3C位置中分别引入羧基双偶氮化后,再与苯基羟胺反应,合成NCPHPA.由于在一分子中增加两个羧基,不仅使试剂的溶解性有很大的提高,且对钼表现出很强的选择性和很高的显色灵敏度.本文介绍NCPHPA的合成方法,并用紫外吸收光谱、红外吸收光谱、核磁共振波谱、质谱等方法论证了产物的结构.简述了NCPHPA在光度分析中性能.将NCPHPA应用于光度法测定痕量钼,E4566达3.52×106 L·mol-1·cm-1,较文献报道钼的高灵敏显色反应,εmax提高了15倍,重现性亦较满意,用于痕量钼的测定,结果与AAS法一致.     

141Nd激发态的在束γ谱学研究

通过130Te(16O,5nγ)141Nd反应布居了141Nd的高自旋态能级. 对反应产生的在束γ射线进行了γ射线单谱和γ-γ符合测量. 建立了激发能达7614.5keV的141Nd能级纲图,新发现了12条γ射线和15个能级. 基于实验测量的γ跃迁各向异性,建议了141Nd部分能级的自旋值. 用一个h11/2价中子空穴与142Nd核芯晕态的耦合可以定性地解释141Nd的能级结构.     

利用α关联衰变链鉴别新同位素265107Bh

主要介绍了合成和鉴别107号元素的新同位素265Bh的实验装置、实验方法以及实验结果.目标核265Bh是由能量为135MeV的26Mg离子轰击243Am靶,通过融合蒸发反应而产生. 反应产物首先由He-jet系统传输到装有数个探测器对的转轮收集测量系统，然后依靠母子核遗传关系通过观察新同位素和它们已知子核261Db和257Lr之间的a衰变的关联，来实现对新核素的鉴别. 实验测得265Bh的a衰变能量为(9.24±0.05)MeV, 半衰期为0.94＋0.70 -0.31s. 从该实验得出的265Bh的a衰变能量和半寿命能够与理论预言一致.     

真彩色全息图的制造新方法

提出采用特殊制作的色编码板，结合空间分离取样技术及彩色荧光屏发光混合原理和方法，仅用单束光，制造一般二维物体的真彩色全息图，文中还叙述对掩膜的制作方法，及高质量色编码板的参数选取和制备方法。最后给出了实验结果。     

一种新型固体Q开关Cr4＋∶YAG的实验研究

对一种适用于Ｎｄ３＋∶ＹＡＧ激光系统的新型被动Ｑ开关掺铬钇铝石镏石（Ｃｒ４＋∶ＹＡＧ）进行了实验研究，得到单脉冲能量为１４５ｍＪ、脉宽为３０～４０ｎｓ、效率接近１％、动静比达４０％以上的结果。     

MASS TRANSPORT IN SOLID TUMORS(Ⅱ)──DRUG DELIVERY

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