Refinements of transformation inequalities for zero-balanced hypergeometric functions

In the article, we present some refinements of three classes of transformation inequalities for zero-balanced hypergeometric functions by use of the updated monotonicity criterion for the quotient of power series.     

Interaction Between 1,2,3-Trichloropropane and Haloalkane Dehalogenase LinB

The haloalkane dehalogenase LinB from Sphingomonas paucimobills UT26 was found to transform the 1,2,3-trichloropropane(TCP) into inorganic halide ions and 2,3-dichloro-1-propanol although the catalytic activity is very low(Kcat=0.005 s-1).In this study,molecular dynamics simulation and docking studies were performed to investigate the binding of TCP to LinB.The docking results indicate that LinB does not restrict TCP to be bound productively in the active site and the water-mediated inhibition occurs in the...     

Supramolecular assembly of H‐bonded side‐chain polymers containing conjugated pyridyl H‐acceptor pendants and various low‐band‐gap H‐donor dyes bearing cyanoacrylic acid groups for organic solar cell applications

Novel supramolecular side‐chain polymers were constructed by complexation of proton acceptor (H‐acceptor) polymers, i.e., side‐chain conjugated polymers P1–P2 containing pyridyl pendants, with low‐band‐gap proton donor (H‐donor) dyes S1–S4 (bearing terminal cyanoacrylic acids) in a proper molar ratio. Besides unique mesomorphic properties confirmed by DSC and XRD results, the H‐bonds of supramolecular side‐chain structures formed by pyridyl H‐acceptors and cyanoacrylic acid H‐donors were also confirmed by FTIR measurements. H‐donor dyes S1–S4 in solid films exhibited broad absorption peaks located in the range of 471–490 nm with optical band‐gaps of 1.99–2.14 eV. Furthermore, H‐bonded polymer complexes P1/S1–P1/S4 and P2/S1–P2/S4 exhibited broad absorption peaks in the range of 440–462 nm with optical band‐gaps of 2.11–2.25 eV. Under 100 mW/cm² of AM 1.5 white‐light illumination, the bulk heterojunction polymer solar cell (PSC) devices containing an active layer of H‐bonded polymer complexes P1/S1–P1/S4 and P2/S1–P2/S4 (as electron donors) mixed with [6,6]‐phenyl C₆₁ butyric acid methyl ester (i.e., PCBM, as an electron acceptor) in the weight ratio of 1:1 were investigated. The PSC device containing H‐bonded polymer complex P1/S3 mixed with PCBM (1:1 w/w) gave the best preliminary result with an overall power conversion efficiency (PCE) of 0.50%, a short‐circuit current of 3.17 mA/cm², an open‐circuit voltage of 0.47 V, and a fill factor of 34%. © 2009 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 5998–6013, 2009     

Pfaffianization of the variable-coefficient KP equation

In this paper, we present a new integrable coupled variable-coefficient KP (vcKP) system, which is derived by extending the Pfaffianization procedure of Ohta and Hirota to the vcKP equation.     

电化学方法制备纳米NiO及反应机理初探

采用电化学法一步制备了镍醇盐配合物Ni(OEt) 2 (acac) 2 (acac为乙酰丙酮基 ) ,并以其作为前驱体 ,控制一定水解条件制得胶体 ,分别在 4 5 0℃ ,60 0℃煅烧均得到具有立方晶型的纳米NiO粉体 .通过红外光谱 (FT_IR)、核磁共振 (1HNMR)、拉曼光谱 (Ramanspectrum)、X_射线粉末衍射 (XRD)、透射电子显微镜 (TEM)等手段对前驱体和NiO粉体进行了表征 .结果表明 ,电解合成的最佳温度为 30～ 4 0℃ ,不溶性镍醇盐配合物升温到 4 0～ 5 0℃即可溶解 .电解法制备得到的纳米NiO层呈球形单分散结构 ,粒径在 10～ 15nm左右 .本文同时讨论了电合成纳米NiO的反应机理     

一种改进的弧长法及在结构后屈曲分析中的应用

基于一般的弧长法,提出了一种高效的改进弧长法.通过对增量弧长作了以考虑结构刚度变化为主的加权修正和利用已知平衡点信息的外插修正,而大大提高了求解效率;利用对累加弧长和期望弧长作近似展开的方法使求解能收敛到预定的载荷值,而拓宽了弧长法的应用范围.两个典型算例表明,采用改进的弧长法在板/壳结构后屈曲分析中,无论是追踪后屈曲的全程路径,还是求得指定载荷点的收敛解都有良好的适应性和较高的效率.     

反胶束体系制备负载型TiO2纳米光催化剂

在AOT/异辛烷反胶束体系中制备了粒径为2～5nm的单分散球形TiO₂纳米粒子,用TEM,DSC和XRD等手段对其进行了分析;用浸渍法以小孔分子筛HZSM-5为载体制备了负载型TiO₂纳米粒子,用FTIR,Langmuir及BET等手段进行了表征;用以上2种TiO₂粒子作光催化剂进行了简单模拟废水处理研究,用UV-Vis光谱分析其催化效果表明,负载型TiO₂纳米粒子比纯TiO₂纳米粒子的光催化活性更高.     

毛细管电泳电化学法监测甘露糖生产工艺

葡萄糖;葡萄糖酸钙;毛细管电泳电化学法监测甘露糖生产工艺;电化学检测     

硅酸锶中Pr~(3+)的4f5d态的光谱特性及Pr~(3+)→Gd~(3+)的能量传递

本文研究了室温下Pr3 + 在Sr2 SiO4 中的发射光谱和激发光谱 ,在激发光谱中 ,最低激发峰位置低于1S0能级位置 ,属于 5d态的吸收。发射光谱主要由 5d→ 4f的跃迁构成 ,未观测到Pr3 + 的3 P0 和1D2 的辐射跃迁。Pr3 + 的掺杂浓度在 0 0 1mol左右时 ,其发射强度接近最大。在Sr2 SiO4 ∶Pr3 + ,Gd3 + 体系中 ,Pr3 + 的 5d→3 H4 的跃迁与Gd3 + 的8S7/ 2 →6I能级的吸收跃迁相匹配 ,因此发生了Pr3 + →Gd3 的高效无辐射能量传递。固定Pr3 +的浓度时 ,随着体系中Gd3 + 离子浓度的增加 ,Gd3 + 的发射强度也随之增强 ,同时 ,Pr3 + 的发射强度则逐渐下降。