大环抗生素--毛细管电泳手性分离中一种新的手性选择剂

两种类型的大环抗生素对很多外消旋化合物具有显著的手性选择性且手性选择性相互补充:第一种类型含ansamycin (安沙霉素) 特别适合于阳离子外消旋化合物的分离;第二种类型含glycopeptide (糖肽)最适于阴离子的分离.介绍了大环抗生素的结构特征及手性识别机理,讨论了pH值、抗生素类型和浓度、电泳电解质浓度和化学性质、有机改性剂及胶束相等不同实验条件对分离的影响,还概述了几种大环抗生素作为手性选择剂,在毛细管电泳手性分离中的研究近况.     

碰撞能对O(1D)+HBr→OH+Br反应的极化分布的影响

运用准经典轨线法结合Peterson从头计算势能面,在碰撞能分别为20.9,41.80和66.88 kJ/mol时,对放热反应O(1D)+HBr(v=0,j=0)→OH+Br(△H=-252.89 kJ/m01)进行了细致的立体动力学性质研究.反映k与j'两矢量相关的函数P(θr)的分布表明产物分子的转动角动量j'在垂直于反应物相对速度矢量k的方向上有强烈的取向分布,且随碰撞能的变化比较明显;反映k,k'与j'三矢量相关的函数P(φr)的分布表明产物转动角动量j'不仅有沿着y轴的取向效应,还有沿着y轴正向的弱定向效应,且这种弱定向效应随碰撞能的增加有所减弱;描述产物转动角动量j'的空间分布函数P(θr,φr)在(90°,90°)和(90°,270°)两处有两个明显的分布,随着碰撞能的增加,这两个集中分布越来越密集,碰撞能对该分布有一定的影响.产物分子的极化主要集中在垂直于散射面的平面内.除此之外,极化微分反应截面(PDDCSs)给出了反应产物的散射方向.     

手性环境下的手性N-取代吡咯电化学聚合及其微结构

在 (S) (+) 樟脑磺酸 ((S) (+) CSA)或 (R) (- ) 樟脑磺酸 ((R) (- ) CSA)的存在下 ,电化学聚合了手性吡咯衍生物 (S) (+) (1H 吡咯基 )丙酸甲酯 (M(+)PyPr) .用电化学、红外、拉曼、X光电子能谱及圆二色谱 (CD)对聚合物进行了表征 ,并用电化学方法测试了聚合物膜的手性识别性质 .同时 ,恒电流及恒电位电解聚合制得了直立于电极表面的导电高聚物微米带     

螺〔1-溴-4-l-孟氧基-5-氧杂-6-氧代双环〔3.1.0〕己烷2,3’-(4’-甲氧基5’孟氧基丁内酯)〕的晶体结构

本文报道了利用新手性源合成的标题化合物C2 9H45 BrO7(Mr=5 85 .5 6 )的晶体结构 ,该晶体属正交晶系 ,空间群为P2 1 2 1 2 1 ,晶胞参数a =9.748(4) ,b =12 .5 37(5 ) ,c =2 5 .85 1(9) ,V =315 9(2 ) 3,Z =4,Dx=1.2 31g/cm3,μ =1.341mm- 1 ,F(0 0 0 ) =12 40 ,偏离因子R =0 .0 475 ,Rw=0 .0 6 0 9;分子中共有 5个环 ,12个手性中心 ,2个六元环呈椅式构象 ,2个五元内酯环呈信封式构象 ,并分别与环丙烷形成〔2 .4〕螺环和〔3 .1.0〕稠环 ,4个新生成的手性中心的绝对构型为C(13) (S) ,C(14 ) (S) ,C(15 ) (R) ,C(16 (R) ,无任何对称因素     

手性双核Salen配合物的谱学性质

合成了四个新型的手性双核(R,R)Salen配合物[(Cu)2L•H2O(2), (Ni)2L(3), (Zn)2L•H2O(4), (MnCl)2L•2H2O(5)], (其中L是由(R,R)环己二胺、 3,5-叔丁基水杨醛、 5,5’-亚甲基二水杨醛为原料合成的手性二聚Salen配体(1)).用元素分析、NMR、FT-IR、UV-Vis、CD光谱对配体和配合物进行了表征.在与单核的Salen配体和配合物比较的基础上，详细讨论了红外光谱、电子吸收光谱、圆二色光谱性质.发现双核配体和配合物的电子吸收光谱吸收峰的位置和形状与单核的配体和配合物基本一致，而吸收峰的强度有近似两倍的关系.另外， 用激子偶合理论解释了此类手性化合物圆二色谱的Cotton效应和Cotton分裂. Cotton分裂的方向依赖于环己二胺的构象.(R,R)环己二胺决定了Salen化合物的手征性为负， Cotton分裂的正负两部分分别处于高能区和低能区.     

含四元环的多环芳香化合物的研究进展

含四元环的多环芳香化合物通常能够表现出独特的光物理和化学性质,在很多领域具有潜在应用价值.分别针对线型、角型、螺旋型和环型含四元环多环芳香化合物的合成方法、分子堆积方式、光电性质及载流子迁移率等方面进行归纳总结.研究表明,表面合成法更利于制得规则形貌的多环芳香化合物;线型类分子表现出了较高的载流子迁移率;角型分子通常显示出更高的反芳香性;螺旋型分子具有好的旋光性及更大的光学带隙,且该类材料中四元环的个数及其所在分子中的位置对材料的光电性质有着决定性的影响.     

丙卡特罗在三种刷型手性固定相上的直接拆分

以正己烷-异丙醇二元混合溶剂体系为流动相,在Whelk-O1、 DNB-PG和DNB-Leucine 3种刷型手性固定相上将药物丙卡特罗直接拆分为(R,R/S)和(S,R/S)对映体,分离系数α值达1.4 ～1.8.考察了流动相组成及固定相分子结构对对映体分离效果的影响,同时对丙卡特罗与3种固定相的手性识别机理进行了探讨.结果表明,当流动相中异丙醇的体积分数(φB)为2% ～30%时,lnk′与lnφB之间呈现较好的线性关系.因此,在一定范围内可以根据所需色谱分离系数或保留时间估计流动相的组成.以后出峰对映体所表征的3种手性柱的色谱分离效能分别为:n(Whelk-O1)=10 816/m,n(DNB-PG)=4 532/m,n(DNB-Leucine)=12 844/m.DNB-PG柱柱效相对较低,谱峰展宽较大,且有轻微拖尾,需改善柱子装填和预处理技术以提高色谱分离柱效.     

手性SalenCOⅡ配合物与氨基酸酯类客体的分子识别研究

用紫外-可见分光光度法研究了手性SalenCoⅡ配合物对4对对映异构的手性氨基酸酯类客体在CH2Cl2中的分子识别,发现手性SalenCoⅡ配合物与此类客体的配位数为1.各客体缔合常数均为KD＞KL,且按K(LeuOMe)＞K(AlaOMe)＞K(SerOMe)＞K(TyrOMe)的顺序依次减小,测定了识别过程的△rGmθ,△rHθm,△rSmθ,发现该反应是放热、熵减少的过程.采用分子力学的方法考察了主客体的最佳优势构象,对该优势构象进行量子化学计算,较好地解释了实验事实.     

手性SalenCOⅡ配合物与氨基酸酯类客体的分子识别研究

用紫外-可见分光光度法研究了手性SalenCoⅡ配合物对4对对映异构的手性氨基酸酯类客体在CH2Cl2中的分子识别,发现手性SalenCoⅡ配合物与此类客体的配位数为1.各客体缔合常数均为KD＞KL,且按K(LeuOMe)＞K(AlaOMe)＞K(SerOMe)＞K(TyrOMe)的顺序依次减小,测定了识别过程的△rGmθ,△rHθm,△rSmθ,发现该反应是放热、熵减少的过程.采用分子力学的方法考察了主客体的最佳优势构象,对该优势构象进行量子化学计算,较好地解释了实验事实.     

1,1'-螺二氢茚-7,7'-二酚(SPINOL)及类似物中螺环骨架的构建方法

1,1'-螺二氢茚骨架是在21世纪初发展起来的一类新型手性配体或催化剂的骨架,具有C2对称性,以及刚性强、稳定性高、易于修饰等特点.周其林等将手性1,1'-螺二氢茚-7,7'-二酚(SPINOL)发展为一系列螺环配体及催化剂,在催化不对称合成领域获得了巨大的成功.1,1'-螺二氢茚骨架的配体及催化剂被认为是为数不多的"优势手性配体和催化剂".尽管催化的不对称合成已经出现,目前方法得到的SPINOL及类似物多为外消旋体,需要进行费力的手性拆分.合成和拆分步骤繁琐的局限性对其大规模生产形成了阻碍.因此,如何从廉价易得的原料出发,发展相应手性螺环骨架配体的高效、不对称催化合成新方法,是非常迫切而且具有挑战性的课题.总结了最近20年SPINOL及螺环骨架类似化合物的合成方法,包括含杂原子的螺环骨架,希望能对配体或催化剂用途的螺环骨架的构建有所启发.     

Optical and vibrational properties of toroidal carbon nanotubes

Toroidal carbon nanotubes (TCNTs), which have been evaluated for their potential applications in terahertz communication systems, provide a challenge of some magnitude from a purely scientific perspective. A design approach to TCNTs, as well as a classification scheme, is presented based on the definition of the six hollow sections that comprise the TCNT, slicing each of them to produce a (possibly creased) planar entity, and projecting that entity onto a graphene lattice. As a consequence of this folding approach, it is necessary to introduce five- and seven-membered rings as defect sites to allow the fusing together of the six segments into final symmetric TCNTs. This analysis permits the definition of a number of TCNT geometry families containing from 108 carbons up to much larger entities. Based on density functional theory (DFT) calculations, the energies of these structural candidates have been investigated and compared with [60]fullerene. The structures with the larger tube diameters are computed to be more stable than C(60) , whereas the smaller diameter ones are less stable, but may still be within synthetic reach. Computational studies reveal that, on account of the stiffness of the structures, the vibrational frequencies of characteristic low-frequency modes decrease more slowly with increasing ring diameter than do the lowest optical excitation energies. It was found that this particular trend is true for the "breathing mode" vibrations when the diameter of the tubes is small, but not for more flexible toroidal nanotubes with larger diameters.     

新型手性双核Salen Zn(II)配合物的分子识别研究

采用新型Salen中间体合成了新型Salen Zn(II)配合物. 用紫外-可见光谱滴定法研究了主体双核Salen Zn(II)与咪唑、二胺类等含氮小分子的分子识别行为, 测定了它们的缔合常数. 对咪唑类客体的缔合常数顺序为K^θ(Im)＞K^θ(2-MeIm)＞K^θ(EMeIm); 对二胺类客体缔合常数顺序为K^θ(DAP)＞K^θ(DAE). 主体与咪唑类和二胺类客体的配位数分别是2和1. 主体与这些客体的识别过程为放热、熵减的焓驱动反应. 利用圆二色光谱研究了识别过程的Cotton效应. 用分子力学方法研究了主客体体系的最低能量构型, 通过量化计算对实验事实做了进一步解释.     

氯分子束与InP(100)表面反应散射的角分布研究

采用角分辨分子束散射技术研究了Cl_2与InP(100)表面热反应和激光诱导反应产物的角分布. 对于热反应, 由调制分子束和可转动四极质谱仪测得产物离子InCl~+、InCl_2~+、PCl~+、PCl_2~+和P_4~+的角分布, 都可用cos~(1.5)θ函数报合. 对于紫外(355 nm)激光诱导反应, 由飞行时间质谱法测得主要产物离子的角分布明显地偏离Knudsen定律. 其中In~+, InCl~+和InCl_2~+的角分布可用α·cosθ+(1-α)cos~nθ函数拟合, 其中α和n为拟合参数, 对于不同的产物离子有不同的数值. 由实验测得的脱附粒子的通量和能量在表面法线方向有明显地聚集现象, 可以认为产物从表面上脱附的机理, 除了热脱附之外, 还有非热脱附以及在表面附近脱附粒子的碰撞效应.     

手性不对称Salen Ni对咪唑类和二胺类客体的分子识别研究

用紫外-可见光谱滴定法研究了新型手性不对称Salen Ni主体(1和2)与咪唑类和二胺类客体的分子识别行为. 结果表明, 二胺类客体的缔合常数顺序为Kθ(乙二胺)>Kθ(丙二胺); 咪唑类客体的缔合常数顺序为Kθ(Im)>Kθ(N-MeIm)>Kθ(2-MeIm)>Kθ(2-Et-4-MeIm), 除主体2对2-乙基-4-甲基咪唑的配位数为1外, 其它体系的配位数均为2. 通过测定识别过程的热力学函数ΔrHθm和ΔrSθm发现, 反应为放热、熵减少过程; 利用圆二色光谱研究了识别过程中的主-客体结合能力的强弱; 用分子力学方法研究了主客体体系的最低能量构象, 并通过量化计算对实验事实做了进一步解释.     

Different experimental results for the influence of immersion angle on the resonant frequency of a quartz crystal microbalance in a liquid phase: with a comment

This paper presents different experimental results of the influence of an immersion angle (θ, the angle between the surface of a quartz crystal resonator and the horizon) on the resonant frequency of a quartz crystal microbalance (QCM) sensor exposed one side of its sensing surfaces to liquid. The experimental results show that the immersion angle is an added factor that may influence the frequency of the QCM sensor. This type of influence is caused by variation of the reflection conditions of the longitudinal wave between the QCM sensor and the walls of the detection cell. The frequency shifts, measured by varying θ, are related to the QCM sensor used. When a QCM sensor with a weak longitudinal wave is used, its resonant frequency is nearly independent of θ. But, if a QCM sensor with a strong longitudinal wave is employed, the immersion angle is a potential error source for the measurements performed on the QCM sensor. When the reflection conditions of the longitudinal wave are reduced, the influence of θ on the resonant frequency of the QCM sensor is negligible. The slope of the plot of frequency shifts (ΔF) versus (ρη)^1/2, the square root of the product of solution density (ρ) and viscosity (η), may be influenced by θ in a single experiment for the QCM sensor with a strong longitudinal wave in low viscous liquids, which can however, be effectively weakened by using the averaged values of reduplicated experiments. In solutions with a large (ρη)^1/2 region (0-55 wt% sucrose solution as an example, with ρ value from 1.00 to 1.26 g cm⁻³ and η value from 0.01 to 0.22 g cm⁻¹ s⁻¹, respectively), the slope of the plot of ΔF versus (ρη)^1/2 is independent of θ even for the QCM sensor with a strong longitudinal wave in a single experiment. The influence of θ on the resonant frequency of the QCM sensor should be taken into consideration in its applications in liquid phase.     

Quasi-Classical Trajectory Study on O++DH (v=0, j=0)→OD++H Reaction at Different Collision Energy

The quasi-classical trajectory calculations O⁺+DH (v=0, j=0)→OD⁺+H reactions on the RODRIGO potential energy surface have been carried out to study the isotope effect onstereo-dynamics at the collision energies of 1.0, 1.5, 2.0, and 2.5 eV. The distributions of dihedral angle P(φr) and the distributions of P(θr) are discussed. Furthermore, the angular distributions of the product rotational vectors in the form of polar plot in θr and φr are calculated. The differential cross section shows interesting phenomenon that the reaction is dominated by the direct reaction mechanism. Reaction probability and reaction cross section are also calculated. The calculations indicate that the stereo-dynamics properties of the title reactions are sensitive to the collision energy.     

激光小角光散射测定高聚物的分子量

本工作建议了一种比较方便可行的、用已知瑞利因子的溶剂标定激光小角散射光度计的方法。纯溶剂的瑞利值R_θ与其散射强度比(G_θ/G_0)有如下关系:R_θ/n=φ[(G_θ/G_0)-δ],式中n为溶剂折光指数;φ为仪器常数;δ为与背景有关的参数。以已知瑞利值的甲苯、苯、环己烷、氯仿及四氯化碳的R_θ/n对测定的(G_θ/G_0)值作图,得到了较好的线性关系,从直线斜率可定φ值。以此方法标定的仪器测定了十个聚苯乙烯窄分布试样均得到了满意的结果。     

Advancing and receding wetting behavior of a droplet on a narrow rectangular plane

The contact angle (CA) measurements are generally performed on a large planar surface of a specific substrate with the width larger than the droplet size. In this study, the contact angle hysteresis on a narrow rectangular plane with a width smaller than the droplet size is experimentally studied through the inflation–deflation process by the needle–syringe method. The inflation process by stepwise addition of the liquid to the droplet leads to the contact line advancing outwardly along the major axis with advancing angle (θ_a). Although the droplet width is constrained by the edge of the plane, the CA along the minor axis (θ_w) increases and its value is greater than θ_a (θ_w > θ_a). Deflation process by stepwise withdrawal of liquid from the droplet results in the contact line retracting inwardly along the major axis as the CA reduces to receding angle (θ_r). In the meantime, the CA along the minor axis decreases as well. Both advancing and receding angles acquired from the narrow rectangular plane are confirmed with those obtained form the typical large surface of acrylic glass. On the basis of free energy minimization and liquid-induced defects model, Surface Evolver simulations are performed to reproduce the behavior of droplet on the narrow rectangular plane during the inflation–deflation process. The results of experiment and simulation agree with each other very well.     

Chiral Naphthalenediimides with High-Efficiency Fluorescence and Circularly Polarized Luminescence in the Solid State for the Application in Organic Optoelectronics

Naphthalenediimides (NDIs) have been extensively studied due to their tunable luminescent properties. However, generally, the monomers or aggregates of non-core substituted NDIs exhibit low fluorescence quantum yields (Φ_FL<10 %) in the solid state, which limit their applications as light-emitting materials and render their chiral species unsuitable for circularly polarized luminescence (CPL). Herein, a series of non-core substituted chiral NDIs that exhibit high luminous efficiencies (Φ_FL up to 56.8 % for racemate and 36.5 % for enantiomer) and a strong CPL behavior in the solid state is reported. These significant improvements are attributed to the unique molecular conformation of the chiral NDIs and the formation of distinctive discrete dimers. The structures of the NDIs were significantly simpler and more accessible than those of other NDIs. The findings evidence that non-core substituted NDIs can exhibit strong fluorescence in the solid state and provide a new pathway to improve photophysical properties of NDIs.