Microscopic Theory of Blue Phases Ⅰ and Ⅱ of Liquid Crystal

The microscopic theory of the blue phases of chiral liquid crystal is proposed. Beginning with the potential between two molecules, by using the cell model of liquid, applying statistical physical method, the distribution function and the free energy of the system are obtained. By using variational approach and zero-order approximation, the differential equation that the order parameter tensor of the blue phase can satisfy is obtained. Then we change the differential equation to the eigenequation problem in quantum mechanics. Considering the symmetry of the blue phases,the order parameter tensors of blue phases Ⅰ and Ⅱ can be made up of the eigenvectors. Our results are the same as the results of Ginzberg-Landau‘s phenomenological theory. The parameters in the order parameter tensors that we calculate in the located system are close to the predecessors‘ results.     

Syntheses,crystal structures and blue emission of three zinc(II) coordination polymers with a 4,4′‐dicarboxybiphenyl sulfone ligand

Three novel zinc complexes [Zn(dbsf)(H₂O)₂] ( 1 ), [Zn(dbsf)(2,2′‐bpy)(H₂O)]·(i‐C₃H₇OH) ( 2 ) and [Zn(dbsf)(DMF)] ( 3 ) (H₂dbsf = 4,4′‐dicarboxybiphenyl sulfone, 2,2′‐bpy = 2,2′‐bipyridine, i‐C₃H₇OH = iso‐propanol, DMF = N,N‐dimethylformamide) were first obtained and characterized by single crystal X‐ray crystallography. Although the results show that all the complexes 1–3 have one‐dimensional chains formed via coordination bonds, unique three‐dimensional supramolecular structures are formed due to different coordination modes and configuration of the dbsf^2? ligand, hydrogen bonds and π–π interactions. Iso‐propanol molecules are in open channels of 2 while larger empty channels are formed in 3 . As compared with emission band of the free H₂dbsf ligand, emission peaks of the complexes 1–3 are red‐shifted, and they show blue emission, which originates from enlarging conjugation upon coordination. Copyright © 2006 John Wiley & Sons, Ltd.     

Simple dose rate measurements for a very high synchrotron X‐ray flux

Dose measurements based on methylene blue (MB) bleaching, widely used for ultraviolet light, can also be applied to X‐rays including very high flux levels. This method has been tested by using both MB bleaching and Fricke dosimetry for a conventional monochromatic X‐ray source and then for `white‐beam' synchrotron radiation. The results show that MB bleaching dosimetry can easily measure X‐ray doses up to at least 10⁵ Gy s^?1, as long as the MB concentration is sufficiently high. This condition can be verified from the deviations from linearity of the bleaching versus exposure time.     

Temperature Dependence of the Mössbauer Effect on Prussian Blue Nanowires

Highly ordered Prussian blue nanowires with diameter of about 50 nm and length up to 4 m have been fabricated by an electrodepositing technology with two-step anodizing anodic aluminum oxide films. The Mössbauer spectra taken between 15 and 300 K indicate that the hyperfine parameters decrease as the temperature increases. The temperature dependence of the quadrupole splitting, the isomer shift and the spectra area are discussed. A decrease of Debye temperature for Prussian blue nanowires was found with respect to that of Prussian blue bulk.     

Distinct magnetic properties of one novel type of nanoscale cobalt-iron Prussian blue analogues synthesized in microemulsion

One novel type of nanoscale cobalt-iron Prussian blue analogues (PBA) in the form of mixed nanorods and nanocubes were synthesized using cetyltrimethyl ammonium bromide (CTAB) as the surfactant in microemulsion at low temperature. The generated products were characterized by SQUID, XRD and IR techniques, etc. The effects of potassium contents, cobalt-to-iron ratios, reaction temperatures on the properties of the nanoscale cobalt-iron PBA were systematically explored. The results showed that the novel type of nanomaterials possessed distinct magnetic properties in that their coercivities were intensely dependent on cobalt-to-iron ratios and potassium contents. Furthermore, it was observed that low reaction temperature not only affected the morphologies of the products, but also had influence on their magnetic properties. Additionally, the cobalt-iron Prussian blue analogues were strongly influenced by CTAB around their surface, which led to higher Curie temperatures.     

喹哪啶蓝与核酸作用的光谱研究及分析

外部堆积结合;分光光度法;喹哪啶蓝与核酸作用的光谱研究及分析     

溶剂热法制备Ag/TiO2纳米材料及其光催化性能

以乙醇为溶剂, 钛酸四丁酯为前驱体, 用溶剂热法制备了Ag表面修饰的负载型纳米二氧化钛光催化剂. 利用X射线衍射(XRD)、N₂吸附-脱附(BET)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)、紫外-可见(UV-Vis)光谱等技术对其进行了系统的表征, 以亚甲基蓝(MB)溶液的脱色降解为模型反应, 考察了不同Ag含量样品的光催化性能. 结果表明: 用溶剂热法制备的样品中TiO₂皆为锐钛矿相, 金属Ag颗粒沉积在TiO₂表面, 粒径为2 nm左右, 比表面积较溶胶凝胶法制备的样品大大增加, 最高可达151.44 m²·g^-1; UV-Vis光谱和光催化实验表明: Ag修饰使TiO₂对光的吸收能力大大增强, 吸收带边红移至可见光区, 亚甲基蓝在该复合材料上的光催化降解反应遵循一级反应动力学模型; 溶剂热法制备样品的光催化性能明显好于溶胶凝胶法制备的样品, 在紫外光和可见光下, Ag摩尔分数为5%的样品表现出最佳的光催化活性.     

果胶改性硅胶复合材料的制备及其对亚甲基蓝的吸附性能

以废弃柚子皮中提取的果胶改性硅胶表面,制备出新型的果胶改性硅胶复合材料——P-硅胶,研究了P-硅胶对水中亚甲基蓝染料的吸附性能。利用红外光谱对材料进行表征,并通过分光光度法考察了用量、pH值、吸附时间、温度及实际水样对P-硅胶吸附亚甲基蓝性能的影响。硅胶经果胶改性后,其对亚甲基蓝的吸附容量由31.6mg?g-1增至41.7mg?g-1,吸附性能明显提高;P-硅胶对亚甲基蓝的吸附容量随着pH值、温度的升高而增大,碱性条件有利于吸附。结果显示：当pH7.0,P-硅胶用量为5mg,吸附时间为2h,吸附温度为50℃时,制备出的P-硅胶对亚甲基蓝染料溶液的吸附容量最大可达59.2mg?g-1。动力学研究显示,P-硅胶对亚甲基蓝的吸附能够在120min内迅速达平衡,吸附行为符合准二级动力学方程,表明该吸附过程以化学吸附为主。吸附等温线研究表明,与Freundlich模型相比,实验数据拟合更符合Langmuir吸附等温模型。P-硅胶对环境水样中亚甲基蓝的去除率可达90%以上。     

蓝绿光敏感的非水溶性光致聚合物特性研究

报导了一种新型蓝绿光敏感的非水溶性光致聚合物材料,这种材料以聚醋酸乙烯酯为成膜物,9-乙烯基咔唑(NVC),甲基丙烯酸2-苯氧乙脂(POEA)和双季戊四醇五丙烯酸酯为单体,Dye3和Dye4为光敏剂,邻氯代六芳基双咪唑(O-CL-HABI)为共引发剂.本材料能同时对蓝光和绿光敏感,用蓝光和绿光分别或同时对该材料曝光,可得到清晰图像.测得的两种衍射效率分别不低于80%.     

基于GaAs膜的GaInP/AlGaInP无杂质空位扩散诱导量子阱混杂的研究

在红光半导体激光器芯片上采用GaAs介质膜进行无杂质空位扩散诱导量子阱混杂研究。激光器芯片的有源区由一个9nm厚的GaInP量子阱和两个350nm厚的AlGaInP量子垒构成,利用MOCVD方法在芯片表面生长GaAs介质膜。在950℃的情况下进行不同时长不同GaAs层厚度的高温快速热退火诱发量子阱混杂。通过光致发光光谱分析样品混杂之后的波长蓝移情况和光谱半峰全宽变化规律。当退火时间达到120s时,样品获得53.4nm的最大波长蓝移;在1min退火时间下获得18nm的最小光谱半峰全宽。