基于半刚性二羧酸配体的两个三维镉（Ⅱ）配位聚合物

通过引入2个不同的氮杂环配体,得到了2个Cd（Ⅱ）配位聚合物[Cd（m-phda）（btbb）_0.5]_n（1）和[Cd（m-phda）（hbmb）_0.5]_n（2）（m-H₂phda=间苯二乙酸）,并对它们的结构进行了表征。结构分析表明配合物1是一个6-连接的pcu拓扑网络,拓扑符号为4¹²·6³。配合物2是一个5-连接的sqp拓扑网络,拓扑符号为（4⁴·6⁶）。另外,配合物1和2表现出较好的热稳定性和不同的荧光行为。     

金属有机骨架薄膜材料的三阶非线性光学性能研究进展

金属有机骨架(MOFs)材料因其可设计的结构以及灵活可控的配位模式,在三阶非线性光学(NLO)领域引起了广泛的关注。与液体分散状态相比,MOFs在固体状态下的三阶NLO性能更为重要,这不仅可以深入了解MOFs本身所固有的光学性能,还有助于实现MOFs在光学器件中的实际应用。然而,由于散射的存在和透光率的限制,单独的MOFs材料难以直接实现固体状态下的三阶NLO性能研究,将MOFs制备成具有较好光学透过性的薄膜是研究其NLO性能最为可行的一种策略。MOFs薄膜不仅很好地继承了MOFs所固有的三阶NLO性能,而且还结合了薄膜的高透光率以及灵活的机械性能。基于此,本文分析总结了MOFs薄膜的制备方法及其NLO性能研究方面的相关工作,并根据目前MOFs薄膜在三阶NLO性能方面的研究现状对其未来发展予以了展望。     

1,3-二(4-吡啶)丙烷-Cd(II)手性配合物的合成与晶体结构

利用室温挥发方法合成了手性化合物[Cd(bbp)2(H2O)2]·bbp·2NO3·H2O(bpp=1,3-二(4-吡啶基)丙烷);利用X射线单晶衍射分析了产物的分子结构,并测定了其荧光光谱和固体圆二色光谱.结果表明,合成产物具有含一维手性链[Cd(bbp)2(H2O)2]n的手性超分子结构;其在室温下表现出中等强度的倍频效应,其二阶非线性极化率为尿素的0.4倍,是潜在的二阶非线性光学材料.此外,合成的手性化合物呈现弱的荧光,其固体圆二色光谱则呈现正的Cotton效应.     

两种含大吸电子取代基的SnR_2Cl_2化合物的合成和晶体结构

以SnCl4和2,4,6-(CF3)3C6H2Li、2,6-(CF3)2C6H3Li为原料合成了两种含大吸电子取代基的化合物Sn[2,4,6-(CF3)3C6H2]2Cl2(缩写为SnAr2Cl2)和Sn[2,6-(CF3)2C6H3]2Cl2(缩写为Sn Ar′2Cl2),利用X射线衍射仪和核磁共振谱仪(19F NMR)表征了产物SnAr2Cl2和SnAr′2Cl2的晶体结构.     

不稳定的二甲基氨基甲基二茂铁的ESI-HRMS分析条件研究

研究并优化了化合物N,N-二甲基氨基甲基二茂铁的电喷雾离子化-高分辨质谱(ESI-HRMS)分析方法。重复测定样品,目标分子离子计数的相对标准偏差(RSD,n=10)为2.4%,表明仪器重复性良好。通过对目标分子的一级质谱图与二级质谱图分析,一级质谱图中母离子的丰度低于最强子离子丰度的10%,表明目标分子在源内发生了裂解。研究了一级质谱中目标分子离子及其最强碎片离子的离子计数与干燥气温度、毛细管出口电压的变化规律,并拟合得到相应的数学方程;确定了目标分子质谱分析的最佳条件。     

(1R,4S,5S)-6-环己基-4-[(1R,2S,5R)-5-甲基-2-异丙基环己氧基]-3-氧杂-6-氮杂双环[3.1.0]-2-己酮的合成及结构表征

环已胺与差向异构体5-[(1R,2S,5R)-5-甲基-2-异丙基环己氧基]-3-溴-2(5H)-呋喃酮发生不对称Mi-chael加成-分子内亲核取代反应,并经柱层析分离,得到一对手性氮杂环丙烷-丁内酯衍生物,其中的标题化合物为首次得到的新手性化合物,产率17%,其结构经IR、1H NMR、13C NMR和HRMS进行了表征。     

Hollow Multilayer Microcapsules for pH‐/Thermally Responsive Drug Delivery using Aliphatic Poly(urethane‐amine) as Smart Component

Hollow multilayer microcapsules made of aliphatic poly(urethane‐amine) (PUA) and sodium poly(styrene sulfonate) (PSS), templated on PSS‐doped CaCO₃ particles, are prepared for pH‐/thermally responsive drug delivery. The electrostatic interaction and hydrogen bonding under weak‐acid conditions between aliphatic PUA and PSS contribute to the formation of multilayer microcapsules. Scanning electron microscopy (SEM) results demonstrate an obvious variation of the hollow multilayer microcapsules in response to changes in temperature and pH value. Drug‐release behaviors using DOX as a model drug demonstrate that the drug release increases on decreasing the pH value because of the interaction weakness between aliphatic PUA and PSS in acidic conditions. Moreover, the drug release is higher at 55 °C than that at 37 °C for the sake of the shrinkage of aliphatic PUA above its lower critical solution temperature (LCST).

     

SPE–HPLC–MS/MS method for the trace analysis of tobacco‐specific N‐nitrosamines and 4‐(methylnitrosamino)‐1‐(3‐pyridyl)‐1‐butanol in rabbit plasma using tetraazacalix[2]arene[2]triazine‐modified silica as a sorbent

Tobacco‐specific N‐nitrosamines (TSNAs), including N′‐nitrosonornicotine, 4‐(methylnitrosamino)‐1‐(3‐pyridyl)‐1‐butanone, N′‐nitrosoanatabine, and N′‐nitrosoanabasine, have been implicated as a source of carcinogenicity in tobacco and cigarette smoke. We present a rapid and effective method comprising SPE based on tetraazacalix[2]arene[2]triazine‐modified silica as sorbent and analysis with HPLC–MS/MS for the determination of TSNAs and 4‐(methylnitrosamino)‐1‐(3‐pyridyl)‐1‐butanol (NNAL), a metabolite of 4‐(methylnitrosamino)‐1‐(3‐pyridyl)‐1‐butanone, in rabbit plasma. The linear dynamic ranges were 10–2000 pg/mL for NNAL and 4–2000 pg/mL for the four TSNAs with good correlation coefficients (>0.9965). The LODs were in the range of 0.9–3.7 pg/mL, and the LOQs were between 2.9 and 12.3 pg/mL. The accuracies of the method were also evaluated and found to be in the range of 90.1–113.3%. This method is promising to be applied to the preconcentration and determination of TSNAs and NNAL in smoke and human body fluids.     

Ion Pairing Kinetics Does not Necessarily Follow the Eigen-Tamm Mechanism

The most recognized and employed model of the solvation equilibration in the ionic solutions was proposed by Eigen and Tamm, in which there are four major states for an ion pair in the solution： the completely solvated state, 2SIP （double solvent separate ion pair）, SIP （single solvent separate ion pair）, and CIP （contact ion pair）. Eigen and Tamm suggested that the transition from SIP to CIP is always the slowest step during the whole pairing process, due to a high free energy barrier between these two states. We carried out a series of potential of mean force calculations to study the pairing free energy profiles of two sets of model mono- atomic 1：1 ion pairs 2.0：x and x：2.0. For 2.0：x pairs the free energy barrier between the SIP and CIP states is largely reduced due to the salvation shell water structure. For these pairs the SIP to CIP transition is thus not the slowest step in the ion pair formation course. This is a deviation from the Eigen-Tamm model.     

A theoretical study on the red- and blue-shift hydrogen bonds of cis-trans formic acid dimer in excited states

The excited states of cis-trans formic acid dimer and its monomers have been investigated by time-dependent density functional theory (TDDFT) method. The formation of intermolecular hydrogen bonds O₁-H₁...O₂=C₂ and C₂-H₂...O₄=C₁ induces bond length lengthening of the groups related to the hydrogen bond, while that of the C₂-H₂ group is shortened. It is demonstrated that the red-shift hydrogen bond O₁-H₁...O₂=C₂ and blue-shift hydrogen bond C₂-H₂...O₄=C₁ are both weakened when excited to the S₁ state. Moreover, it is found that the groups related to the formation of red-shift hydrogen bond O₁-H₁...O₂=C₂ are both strengthened in the S1 state, while the groups related to the blue-shift hydrogen bond C₂-H₂...O₄=C₁ are both weakened. This will provide information for the photochemistry and photophysical study of red- and blue-shift hydrogen bond.