新型双核配合物的形成、与DNA的作用机制及荧光性质研究

利用紫外、荧光和粘度等方法研究了含不同配体的钌(II)配合物[Ru(phen)₂CImP]^2＋(CImP＝3,4-二羟基-咪唑并[4,5-i][1,10]邻菲咯啉)和[Ru(phen)₂TPPZ]^2＋(TPPZ＝四吡啶[3,2-a:2',3'-c:3',2'-h:2'',3''-j]吩嗪)与DNA的作用机制, 并研究了配合物与Zn^2＋配合后荧光性质变化. 结果表明[Ru(phen)₂TPPZ]^2＋与DNA以插入模式作用, 而[Ru(phen)₂CImP]^2＋与DNA则以沟面结合模式作用. 向配合物溶液中滴加Zn^2＋后, 配合物[Ru(phen)₂TPPZ]^2＋和[Ru(phen)₂CImP]^2＋均可以与Zn^2＋形成双核配合物[Ru(phen)₂(TPPZ)Zn]^4＋和[Ru(phen)₂(CImP)Zn]^4＋, 配合物的荧光减弱. 与DNA作用后, 配合物仍可以与Zn^2＋配位形成双核配合物, 但[Ru(phen)₂(TPPZ)Zn]^4＋保持插入模式与DNA作用, 配合物的荧光减弱. 而[Ru(phen)₂(CImP)Zn]^4＋与DNA则由沟面结合改为插入结合, 配合物的荧光增强.     

钌(Ⅱ)配合物[Ru(dpq)2L]4+的合成、晶体结构及与G-四链体DNA的相互作用

以cis-[Ru(dpq)₂Cl₂]·2H₂O(dpq=二吡啶[3,2-d:2',3'-f]二氮萘)为原料与5,5'-二(1-(三乙胺)甲基)-2,2'-联吡啶阳离子(L)合成钌(Ⅱ)配合物[Ru(dpq)₂L](PF₆)₄,并研究了该配合物与G-四链体DNA的作用:FRET实验表明,配合物对人端粒DNA h-telo具有选择性,其作用能力要强于同癌基因启动子区域的四链DNA,如c-myc和bcl2;CD光谱表明,在Na⁺和K⁺都不存在的情况下,配合物能诱导h-telo形成平行结构;此外,紫外和发射光谱都显示,配合物在K⁺溶液中与h-telo的作用力要大于在Na⁺溶液中的。     

一维链状3-碘苯甲酸铽配合物的合成、晶体结构和性质表征

溶液法合成了配合物{[Tb(3-IBA)₃(H₂O)₂]·0.5(4,4′-bipy)}_n(3-IBA=3-碘苯甲酸根;4,4′-bipy=4,4′-联吡啶),并通过X-射线衍射单晶结构分析、红外光谱、紫外光谱、荧光光谱以及热重分析对配合物进行了结构和性质表征。配合物晶体属三斜晶系,P1空间群。该配合物具有一维链状结构。Tb³⁺离子与8个O原子配位,其中6个O原子来自5个3-碘苯甲酸根,2个O原子来自水分子。相邻Tb³⁺离子通过2个双齿桥联的3-碘苯甲酸根联结成一维链状结构。未配位的4,4′-联吡啶分子与配位水分子之间形成氢键,并将相邻的一维链联结起来形成二维网状结构。沿a轴的分子堆积形成一维孔道,是由于相邻一维链的苯环之间部分重叠而形成的。在紫外光照射下,配合物发出很强的绿色荧光。配合物的荧光光谱中,4个峰位于490、544、583和619 nm,分别对应于Tb³⁺离子的⁵D₄→⁷F₆、⁵D₄→⁷F₅、⁵D₄→⁷F₄和⁵D₄→⁷F₃跃迁。     

稀土钠钨青铜化合物NaxLayWO3结构与导电性的理论研究

使用密度泛函理论研究了稀土钠钨青铜化合物的结构和导电性质. 在实验晶体结构数据的基础上构建Na_xWO₃和Na_xLa_yWO₃的模型分子, 优化其几何结构, 并与实验值比较. 在此基础上计算了化合物的能带结构和电子能态密度. 通过这些研究探讨当La^3＋取代Na_xWO₃的中心Na^＋后对结构和导电性的影响. 计算结果表明La^3＋的取代并没有改变结构的空间对称性, 但却使晶格参数和体积略有增大; 取代使电子结构发生了变化, 在费米面附近, 能带相互交叠更加密集, 电子出现的几率增加, 从而增加了其导电性. 这可能是掺杂后La^3＋的4f和5d电子的贡献使电子轨道杂化作用增强, 电子云密度分布重排的结果.     

钌(Ⅱ)配合物[Ru(dpq)2L]4+的合成、晶体结构及与G-四链体DNA的相互作用

以cis-[Ru(dpq)₂Cl₂]·2H₂O(dpq=二吡啶[3,2-d:2',3'-f]二氮萘)为原料与5,5'-二(1-(三乙胺)甲基)-2,2'-联吡啶阳离子(L)合成钌(Ⅱ)配合物[Ru(dpq)₂L](PF₆)₄,并研究了该配合物与G-四链体DNA的作用:FRET实验表明,配合物对人端粒DNAh-telo具有选择性,其作用能力要强于同癌基因启动子区域的四链DNA,如c-myc和bcl2;CD光谱表明,在Na⁺和K⁺都不存在的情况下,配合物能诱导h-telo形成平行结构;此外,紫外和发射光谱都显示,配合物在K⁺溶液中与h-telo的作用力要大于在Na⁺溶液中的。     

配合物稳定性和配体酸碱强度之间的直线自由能关系──铜(Ⅱ)、锌(Ⅱ)-芬布芬-α-氨基酸三元配合物体系

在25±0.1℃,I=0.1mol·dm^-3KNO₃条件下,80%(v/v)DMSO-H₂O混合溶剂中,应用pH法测定了甘氨酸,L一缬氨酸,L-异亮氨酸,L-脯氨酸,L-丝氨酸,DL-苯丙氨酸等六种α-氨基酸(缩写为α-AA,记为B配体)的酸离解常数,铜(Ⅱ)-α-氨基酸。锌(Ⅱ)-α-氨基酸二元配合物的稳定常数及铜(Ⅱ)-芬布芬-α-氨基酸(芬布芬缩写为Fen,记为A配体)和锌(Ⅱ)-芬布芬-α-氨基酸三元配合物的稳定常数。实验发现,在下面三对参数之间,即logβ₁₀₂与pK₂^B,lOgβ₁₁₁;与pK₂^B及10gβ₁₁₁与logβ₁₀₂,均存在良好的直线自由能关系。用△logK_M和△logβ₁₁₁两个参量描述了三元配合物相对于母体二元配合物的稳定性。讨论了溶剂的性质,配合物分子内配体之间的疏水作用,芳环之间的堆积作用对配合物稳定性的影响。     

三(羟甲基)甲基甘氨酸合镍(II)配合物的结构及其与生物分子的作用研究

合成了配合物[Ni(tricine)₂]•6H₂O单晶, 其中, tricine为三(羟甲基)甲基甘氨酸. 配合物属于单斜晶系, P2(1)/n空间群, 配体以一个氮原子和二个氧原子与中心Ni^2＋离子配位, 生成八面体构型配合物. 配合物分子之间靠丰富氢键形成稳定的二维结构. 用紫外光谱方法测定了该配合物与鱼精DNA、腺苷三磷酸和腺嘌呤的作用情况, 并就相互作用机理进行了初步分析.     

阴离子调控的含反式-双(苯甲酰丙酮)-1,4-环己二胺银配位聚合物的合成、晶体结构及其荧光性质

将配体反式-双(苯甲酰丙酮)-1,4-环己二胺(L)与AgX(X=NO₃^-,BF₄^-,SbF₆^-,ClO₄^-)进行反应得到4个配合物{[Ag(L)]NO₃}_n(1),{[Ag(L)(H₂O)]BF₄}_n(2),{[Ag₂(L)₃](SbF₆)₂}_n(3),{[Ag(L)]ClO₄}_n(4),并用元素分析,红外和X-射线单晶衍射表征了4个配合物的结构。在固体状态下,配合物1和2都形成2D网状结构的配位聚合物,都有2个不同配位类型的配体,不同的是,配合物1中桥连配体的1,4-环己二胺1,4位的C-N键在直立键上,而配合物2中桥连配体的1,4-环己二胺中1,4位的C-N键在平伏键上;配合物3也有2种不同配位类型的配体,但是与配合物1和2不同,配合物3形成1D配位聚合物;配合物4中的配体只有一种配位类型,配合物4形成2D网状结构。4个配合物中,配合物2,3的阴离子未参与Ag(Ⅰ)配位,配合物1和1的阴离子与Ag(Ⅰ)配位。同时,研究了配体和配合物在室温下的固态荧光性质。     

由4-甲基-1，2，3-噻二唑-5-甲酸构筑的过渡金属配合物的合成、晶体结构及与DNA作用

以4-甲基-1,2,3-噻二唑-5-甲酸（C₄H₄N₂O₂S, HL）分别与硫酸钴（CoSO₄·7H₂O）、氯化铜（CuCl₂·2H₂O）、硝酸银（AgNO₃）反应合成了3个配合物[Co（L）₂（H₂O）₄] ·2H₂O （1）、[CuNa（L）₃] _n （2）和[AgL] _n （3）,用元素分析、红外光谱、热重分析进行表征,用单晶X射线衍射测定了产物的结构。配合物1属于三斜晶系,空间群P1,Co²⁺的配位数为6,形成一个略为拉长的CoN₂O₄八面体,与理想的正八面体非常接近。配合物2属于三斜晶系,空间群P1。Cu²⁺离子的配位数为4,构成变形的平面四边形结构,Na⁺离子的配位数为6,构成一个略微变形的八面体结构,最终形成三维网状结构。配合物3属于单斜晶系,空间群P2₁/c,银离子为三配位,构成变形的平面三角形构型,具有二维网状结构。用溴化乙锭荧光探针法测定了配体和配合物与DNA作用的荧光光谱。     

第一过渡系金属-镝单分子磁体研究进展与展望

第一过渡系中的顺磁性离子Cr^Ⅲ、Mn^Ⅱ/Mn^Ⅲ、Fe^Ⅱ/Fe^Ⅲ、Co^Ⅱ、Ni^Ⅱ和Cu^Ⅱ及抗磁性离子Co^Ⅲ和Zn^Ⅱ均可与Dy^Ⅲ在多齿螯合配体配位下形成单分子磁体配合物。在本文中,我们阐述或汇总了几乎所有的第一过渡系金属-镝单分子磁体。对于由顺磁性第一过渡金属离子和Dy^Ⅲ离子形成的配合物,有2个有趣的现象需要引起人们的注意：一是一些Cr-Dy配合物具有较高的阻塞温度和较大的矫顽场,这可归功于配合物内Cr^Ⅲ离子和Dy^Ⅲ离子之间较强的磁耦合作用（|J|>10 cm^-1）。二是报道的Fe^Ⅱ₂-Dy配合物的能垒可达到319 cm^-1（459 K）,这在第一过渡系金属-镝单分子磁体中也是比较高的。这可能与Fe^Ⅱ₂-Dy中Dy^Ⅲ具有较高的轴向对称性（D_5h）有关,且从头计算表明该配合物中Dy的第一激发态也具有较高的轴向对称性。除了部分Cr-Dy和Fe^Ⅱ-Dy配合物外,其他顺磁性第一过渡金属-Dy的能垒较低,这可能由配合物内顺磁离子间弱的磁耦合造成的。为了消除磁耦合对磁弛豫行为影响,近年来人们关注于使用抗磁性第一过渡金属离子与Dy^Ⅲ构建单分子磁体配合物。相比其他核数的Zn-Dy配合物,三核Zn₂Dy配合物被报道的数目最多且研究得最为深入,这可能与较易调控Zn₂Dy中Dy配位几何对称性有关。最后,我们提出了几点关于进一步提升第一过渡系金属-镝单分子磁体的磁性能的建议,其中最为重要的是控制Dy配位几何的轴向对称性及Dy的基态m_J的电荷分布。对于第一过渡系金属-镝单分子磁体中的Dy^Ⅲ离子,Dy^Ⅲ基态m_J的电荷与配体的电荷之间的静电排斥应该降到最低。     

Molecular dynamics simulation of thermomechanical properties of montmorillonite crystal. 3. montmorillonite crystals with PEO oligomer intercalates

We present the results of molecular dynamics (MD) simulation of the structure and thermomechanical behavior of Wyoming-type Na+-montmorillonite (MMT) with poly(ethylene oxide) (PEO) oligomer intercalates. Periodic boundary conditions in all three directions and simulation cells containing two MMT lamellae [Si248Al8][Al112Mg16]O640[OH]128 oriented parallel to the XY-plane were used. The interlamellar space, or gallery, between neighboring MMT lamellae was populated by 24 Na+ counterions and PEO macromolecules of different lengths, ranging from 2 up to 240 repeat units. We considered three different loadings of PEO within the gallery: 80, 160, and 240 repeat units, corresponding to 13, 23, and 31 wt % PEO based on total mass of the nanocomposite, respectively. In the cases of 13 and 23 wt %, the polymer chains formed one or two well-defined amorphous layers with interlayer distances of 1.35 and 1.8 nm, respectively. We have observed also formation of a wider monolayer gallery with interlayer distances of 1.6 nm. Three-layer PEO films formed in the case of 31 wt % loading. The thermal properties were analyzed over the range 300-400 K, and the isothermal linear compressibility, transversal moduli, and shear moduli were calculated at 300 K. These properties are compared with the results of our simulation of thermal and mechanical properties of MMT crystal with galleries filled by one or two water layers as well as with those of an isolated clay nanoplate.     

Saturation ratio of poly(ethylene oxide) to silicate in melt intercalated nanocomposites

Melt intercalation has been found to be a very successful approach for preparation of polymer-clay nanocomposites. An aspect of this area that has been little investigated is the amount of polymer required to fill the interlayer galleries of the clay. This paper reports experiments which determine the amount of poly(ethylene oxide) (PEO) required to saturate the spacing between montmorillonite (MMT) or organically-modified bentonite (B34) layers. Differential scanning calorimetry (DSC), X-ray diffraction (XRD) and thermogravimetric analysis (TGA) were used to determine the saturation ratios of PEO to silicates, which are then compared to theoretical calculations. The deduced saturation ratio of PEO to MMT is 28:72, and PEO to B34 15:85 by XRD and DSC, whilst ratios of PEO to MMT of 21:79 and PEO to B34 10:90 were obtained via TGA. The density of intercalated PEO in the silicate galleries is estimated to be 0.82 g/cm³, which suggests that PEO in the silicate galleries is far less efficiently packed than in the amorphous region of the bulk polymer.     

Grafting of poly(ethylene oxide) on poly(methyl methacrylate) by transesterification

The grafting of the potassium alkoxide derivative of poly(ethylene oxide) on poly(methyl methacrylate) in homogeneous solution in toluene was studied. The alkoxide was prepared by reaction with potassium metal with methanolic potassium methoxide, or with potassium naphthalene. The last was the most suitable for the systematic investigation of the grafting process. Soluble graft polymers were formed, and essentially the initial poly(ethylene oxide) (PEO) and poly(methyl methacrylate) (PMMA) participated in the production of graft polymer. The composition of the graft polymers and the frequency of grafting of the side chains were determined by NMR. The solubility of the graft polymers in methanol and water increased with increasing PEO contents, while the melting ranges decreased. Fractionation of the crude graft polymers showed that the grafting reaction was random, and graft polymers containing one PEO side chain per about 10–170 MMA units were obtained.     

Functions of Acyclic Poly(ethylene Oxide) Homologs: Acceleration of Nucleophilic Reactions and Selective Ion Transport through Membranes

The acceleration effect of poly(ethylene oxide) on nucleophilic reactions was investigated. The enhancement of the reaction rate was interpreted by the cooperative solvation of alkali metal ions with ethereal oxygens of PEO resulting in active nucleophilic anions. In relation to the complex formation of alkali metal ions with PEO, the oligo(ethylene oxide) derivatives were prepared as the synthetic ionophores, which were able to transport alkali metal ions selectively through a liquid membrane against the alkali metal ion concentration.     

Investigation of the micropolarity in reverse micelles of nonionic poly(ethylene oxide) surfactants using 4-nitropyridine-N-oxide as absorption probe

The micropolarities of the reverse micelle (RM) interior of nonionic poly(ethylene oxide) surfactants of the alkyl ether type (poly(ethylene oxide)[4] lauryl ether (C12E4, Brij 30)), alkyl-aryl ethers (poly(ethylene oxide)[4] nonylphenyl ether (C9PhiE4), poly(ethylene oxide)[5] nonylphenyl ether (C9PhiE5), and poly(ethylene oxide)[5] octylphenyl ether (C8PhiE5)), and poly(ethylene oxide)-poly(propylene oxide)-poly(ethylene oxide) (PEO-PPO-PEO) triblock copolymers (Pluronics P123, F127) were investigated as a function of the water content by applying the absorption probe technique, using 4-nitropyridine-N-oxide (NP) as a probe. The change in the micellar aggregate micropolarity in different solvents (cyclohexane, decane, n-butanol, and n-butyl acetate) at various water contents has been investigated. The research was focused on the determination of the effects of surfactant structure and solvent type on the hydration degrees of the PEO chains in the region at the core limit, where the NP probe was located. All results regarding the polarities in RM and PEO/water calibration mixtures have been expressed in terms of Kosower's Z values, using the linear dependence of E(NP) on Kosower's Z. The PPO/butanol mixtures have also been used for RM in butanol as a reference system. The data revealed that local polarity in RM is dependent on the surfactant type, block copolymer composition, solvent nature, and water content. At the same water content, the results clearly indicate a lower hydration degree of triblock copolymers, as compared to the surfactants of the alkyl ether and alkyl-aryl ether type, but for P123 and F127 Pluronics in n-butanol the hydration is higher owing to the behavior of butanol as cosurfactant and to its hydration.     

Dielectric relaxation processes and ionic conduction behaviour in poly(ethylene oxide)–montmorillonite clay nanocomposite aqueous colloidal suspensions

The relative complex dielectric function, electric modulus, alternating current (ac) electrical conductivity and complex impedance spectra of poly(ethylene oxide) (PEO)–montmorillonite (MMT) clay aqueous colloidal suspension (hydrocolloids) were investigated over the frequency range 20 Hz to 1 MHz at 27 °C. The relaxation time corresponding to electrode polarisation and Maxwell–Wagner polarisation processes (ionic conduction) were determined from these plots. The direct current (dc) electrical conductivity is evaluated from the fitting of real part ac conductivity data to the Jonscher power law. A correlation of increase in dc conductivity and decrease of ionic conduction relaxation time with increase of clay concentration is discussed considering intercalation of PEO chains and its dynamics and exfoliation of MMT clay nanoplatelets in these complex fluids. The formation of PEO–MMT clay supramolecular lamellar nanostructures with increase in continuity of lamellae arrangements were explored for the structural conformation of these nanocomposite novel materials.     

The effect of poly(ethylene oxide) on the characteristics of Triton X-100/1-butanol/ n-octane/water reverse micelles

 Nonionic poly(oxyethylene) surfactant with about ten ethylene oxide units and 1-butanol have been studied in reverse micelles with one nonpolar solvent(n-octane) at different water contents in the presence and in the absence of poly (ethylene oxide) (PEO) using two absorption probes, methyl orange and methyl blue MB and one spin probe, 5-doxylstearic acid. The study has focused attention on the effect of the addition of PEO on the phase behavior of the system, the state of water in the reverse micelles, and the locus of PEO solubilized in reverse micelles. In the presence of PEO, some PEO segments may penetrate into the interface close to the palisade layer of the reverse micelles and then replace some water molecules, which results in a less close arrangement between the chains of surfactants as well as between alcohol molecules. Received: 13 April 1999/Accepted in revised form: 5 November 1999     

聚氧乙烯-高氯酸锂-水复合物体系的固体核磁共振研究

运用13C和7Li固体高分辨核磁共振(NMR)技术对一系列以水作溶剂制备的不同配比聚氧乙烯(PEO)-高氯酸锂(LiClO4)复合物样品的相态结构进行了研究.发现在样品中有一定量水存在的条件下,随着LiClO4含量的增加,复合物体系经历了PEO的结晶逐渐被破坏,PEO与LiClO4形成的新的晶型逐渐增加的过程,当PEO单体与LiClO4的摩尔比在6/1与8/1之间时,样品完全非晶,水的存在对PEO与Li+的相互作用起到了明显的阻碍作用.     

Selective adsorption of poly(ethylene oxide) onto a charged surface mediated by alkali metal ions

Using a surface force balance, we have measured normal and shear interactions between mica surfaces across pure water and across 0.1 M aqueous solutions of LiNO3, NaNO3, KNO3, and CsNO3, both prior to adding polymer and following addition of 1.5 x 10(-4) w/w poly(ethylene oxide) (PEO, Mw = 170 kD) and overnight incubation. Our results reveal that while the PEO adsorbs strongly from the KNO3 and CsNO3 solutions, unexpectedly it does not adsorb at all from the LiNO3 and NaNO3 salt solutions. We attribute this to the different nature of the hydration layers about the alkali metal ions: these favor liganding to the negatively charged mica surface of the etheric -O- group on the ethylene oxide monomer for the case of the more weakly hydrated K+ and Cs+, but not for the case of Na+ or Li+ with their more strongly bound water. A simple model relating the electrostatic energy changes occurring upon such liganding to the experimentally measured hydration energies of the different alkali metal ions supports this attribution.     

Dielectric and conductivity studies of 90 MeV O7+ ion irradiated poly(ethylene oxide)/montmorillonite based ion conductor

In the present work effect of 90 MeV O⁷⁺ ions with five different fluences on poly(ethylene oxide) (PEO)/Na⁺-montmorillonite (MMT) nanocomposites has been investigated. PEO/MMT nanocomposites were synthesized by solution intercalation technique. With the increase in irradiation fluence, gallery spacing of MMT increases in the composite and an exfoliated nanostructure is obtained at the fluence of 5?×?10¹² ions/cm² as revealed by X-ray diffraction results. Highest room temperature ionic conductivity of 4.2?×?10^?6?S?cm^?1 was found for the fluence 5?×?10¹² ions/cm², while the conductivity for unirradiated polymer electrolyte was found to be 7.5?×?10^-8?S?cm^?1. The increase in intercalation of PEO chains inside the galleries of MMT results in the increase in interaction between Na⁺ cation and oxygen heteroatom leading to the increase in ionic conductivity of the composites. Surface morphology and interactions among the various constituents in the nanocomposites at different fluence have been examined by scanning electron microscopy and Fourier transform infrared spectroscopy, respectively. The appearance of peak for each fluence in the loss tangent suggests the presence of relaxing dipoles in the polymer nanocomposite electrolyte films. With the increase in ion fluence the peak shifts towards higher frequency side, suggesting decrease in the relaxation time.