谷氨酸钠从其水溶液中的周期结晶现象

早在本世纪初物理化学家们就已观察到，某些物质从其熔融态或溶液中结晶出来时，在某些条件下可形成周期性的宏观结晶条纹［1，2］，这就是周期结晶现象，由于这种现象和晶体生长、材料物性以及成矿过程等重要问题紧密相关，很早就引起了人们的重视．近年来有关非平衡非线性系统中自发产生各种时空有序现象（自组织现象）的各种理论（如耗散结构理论）［3］的兴起，重新引起了人们对这类现象的兴趣．八十年代，Iwamoto等先后报道了甲基苄基氨基甲酸酯（MethylMesitylcarbamate）从氯仿溶液［4］和抗坏血酸（AscorbicAcid）从甲醇溶液［5］…     

3-硝基-1,2,4-三唑-5-酮的锰钴和镍配合物的分子轨道研究

用EHMO方法计算研究3－硝基－1，2，4－三唑－5－酮（NTO）的锰、钴和镍配合物［M（H2O）6］（NTO）2·2H2O（M＝Mn、Co和Ni）的电子结构，通过比较原子上净电荷、原子间重叠布居、前沿分子轨道能级和组成等电子结构参数，阐明了标题物的配位键特征和热解实验．     

[Ln(EO_2)_3](ClO_4)_3·3H_2O的晶体结构研究

合成了希土高氯酸盐开环冠醚二缩乙二醇（ＥＯ２）晶体，（Ｌｎ＝Ｎｄ，Ｈｏ），测定了结构，文内以Ｎｄ－Ｌ的数据为主要研究对象（方括号内是Ｈｏ－Ｌ的数据）。晶体属单斜晶系，Ｐ２１／ｎ空间群，化学式［Ｌｎ（ＥＯ２）３］（ＣｌＯ４）３·３Ｈ２Ｏ，晶胞参数为：ａ＝１４．１２４（１）［１４．０８７］，ｂ＝１３．９９０（１）［１４．０３９］，ｃ＝１５．２６５（１）［１５．０１４］；β＝９５．７８（１）［９５．６４］°；Ｖ＝３００１．１（６）［２９５５］３；Ｍｒ＝８１５．０１［８３５．７０］；Ｚ＝４；Ｄｃ＝１．８０４［１．８６５］ｇ／ｃｍ３；石墨单色器，μ（ＭｏＫα）＝２．０９［３．０７］ｍｍ－１，最终偏离因子Ｒ＝０．０５５［０．０７４］，ＲＷ＝０．０７１［０．１０９］。研究结果表明晶体具有相同的结构，配位多面体为九配位三帽三棱柱。发现ＥＯ２醚链有绕Ｃ－Ｃ键呈ＳＴＴＳ分布的规律。弱配体高氯酸根不参加配位。     

金刚石格点上自避行走尾形链的构象统计理论

研究了金刚石格点上自避随机行走（ＳＡＷ）尾形链，采用精确计数和ＭｏｎｔｅＣａｒｌｏ模拟方法求得该ＳＡＷ尾形链的构象数Ｃ（Ｄ）１（Ｎ）和均方末端距［ｈ（Ｄ）１（Ｎ）］２及其分量随链长Ｎ的变化关系．发现它们与自由ＳＡＷ链一样都服从标度律，从这些量的计算机实验数据拟合求出了金刚石格点上ＳＡＷ尾形链的临界指数和格点指数．计算结果还表明短链ＳＡＷ在壁的法向与ＮＲＷ尾形链一样有所伸展，均方末端距的法向分量几乎是平行分量的２倍；但随Ｎ→∞，链自回避效应对壁的作用有所屏蔽．这些都与简立方格子模型上得到的结果一致．     

镉－硫氰酸根与铵－苯并15－冠－5配合物的合成与结构研究

用凝胶法生长了标题配合物［ＮＨ_４（Ｂ１５Ｃ５）_２］［Ｃｄ（ＳＣＮ）_３］的晶体，并对其进行了红外光谱，元素分析等各项物理性质的测试。经Ｘ射线单晶结构分析得到了配合物的全部晶体学数据：Ｍ_ｒ＝８４１．３１，正交晶系，空间群Ｐ２_１２_１２_１，晶胞常数ａ＝１０．９７０（３），ｂ＝２１．８３４（３），ｃ＝１５．５６３（４），Ｖ＝３７２７（３），Ｚ＝４，Ｄ_ｘ＝１．５０ｇ／ｃｍ￣３，Ｆ（０００）＝１７３６，μ＝７．０９ｃｍ￣（－１），Ｒ＝０．０７０，Ｒ_ｗ＝０．０６３。结构分析结果表明，配阳离子［ＮＨ_４（Ｂ１５Ｃ５）_２］￣＋和配阴离子［Ｃｄ（ＳＣＮ）_３］￣－间靠静电力结合成配合物。     

含间位聚醚酮醚酮酮的合成与结晶

聚芳醚酮类聚合物因其综合性能优异而在高技术领域得到广泛应用．这些高聚物的主链大都为全对位连接,使其熔点较高以至加工难度增大．如果在聚合物主链中引入间位结构,则可在对玻璃化转变温度影响较小的情况下降低熔点来改善加工条件［１］．含间位聚醚酮醚酮酮（ＰＥＫＥＫｍＫ）也是其中一种．本文主要研究ＰＥＫＥＫｍＫ的合成、基本物性与结晶行为．样品的合成与制备：单体４,４′双（对苯氧基）二苯甲酮按文献［２］方法合成．聚合物参照文献［３］合成．将粉末样品在油压机上熔融后快速取出投入冰水中淬火得无定形样品,或将熔融…     

等电子系列XO-3及BF3的定量价键阐述

等电子系的理论和实验研究，可以揭示体系内部电子运动与其外在宏观性质之间的关系．由于等电子体BO33-、CO32-和NO3-均可稳定存在，可以推测该系列的下一个物种OO3也会短暂存在，尽管实验仅发现O4以O2双聚体，即vanderWaals分子（O2）2形式存在．最近Roeggen等［1］和Hotakka等［2］同时对OO3（D3h点群）进行了理论上的研究，前者采用EXGEM方法和（9s5p1d）／［6s4p1d］基组进行计算，表明OO3是一亚稳结构，且Ro－o＝1．330A；后者对BO33-、CO32-、NO3-及OO3系列进行了对比研究，发现采用6－31G基组作HF计算得到的键长和振…     

C60接枝聚(N-乙烯基咔唑)的合成、表征及光电导性能

自从Ｃ６０被发现和被制备出来以后,其特殊的结构和独特的物理和化学性质受到各研究领域学者的广泛青睐．聚（Ｎ－乙烯基咔唑）（ＰＶＫ）体系经 Ｃ６０掺杂后光电导性能有很大幅度提高．但掺杂体系不稳定,因而限制了对该类材料的应用．为了克服这种缺点,我们尝试用各种简单的方法把Ｃ６０化学键合到高分子链中,制备具有光电导性能的Ｃ６０高分子衍生物． 最近,唐本忠［１］和 Ｐａｔｉｌ［２］等分别用常规的自由基聚合方法,将Ｃ６０接枝到聚合物分子主链上,我们已研究了不含导电高分子的Ｃ６０共聚物的光电导性能［３］,本文采用…     

淀粉／聚乙烯共混物的降解

淀粉和聚乙烯二者极性差别很大，如何提高淀粉／聚乙烯共混物降解塑料中两相的相容性是此项研究的技术关键．采用添加增容剂［１］，或进行淀粉疏水改性［２］，或对聚乙烯进行亲水改性［３］的办法均取得了一定的进展．本文在提高相容性研究的基础上，又添加油酸和有机铁...     

多核钴铁羰基簇结构与催化性能研究

本文以ＣｌＣＣｏ_３（ＣＯ）_９，Ｅｔ_４Ｎ［ＦｅＣｏ_３（ＣＯ）_（１２）］，Ｍｅ_４Ｎ［Ｆｅ_６Ｃ（ＣＯ）_（１６）］诸羰基簇为研究对象，采用激光等离子体源飞行时间质谱及量化计算相结合，对上述羰基簇合物结构及稳定性进行了研究，并将所得结果用于推论ＣｌＣＣｏ_３（ＣＯ）_９及Ｅｔ_４Ｎ［ＦｅＣｏ_３（ＣＯ）_（１２）］的烯烃氢甲酰化反应活性中间体和α－Ａｌ_２Ｏ_３担载的相应簇合物的ＣＯ加氢活性物种。     

Density functional embedding approach to the Mn impurities in NaBr crystals

We have performed density functional calculations for three 19‐atom clusters, two 25‐atom clusters, and one 18‐atom cluster, each embedded in a Madelung potential that takes into account the long‐range electrostatic interactions of the ion lattice of a NaBr crystal. One of the three 19‐atom and one of the two 25‐atom clusters model bulk crystalline NaBr; the others model a Mn²⁺ impurity trapped in a cubically symmetric crystalline electric field (CEF) site of the NaBr host. One of the latter has the NaBr bulk interatomic distance, while in the others relaxation of the Br atoms around the metallic impurity has been considered. The 18‐atom cluster models a relaxed Mn impurity Na vacancy system. All of our calculated clusters have a Na site at the center, and they all include at least first and second nearest‐neighbor host atoms. In the center of the doped clusters the Mn impurity replaces the missing Na ion. The electronic structure of the embedded impurity ion in its local environment was computed self‐consistently by means of all‐electron density functional theory (DFT) techniques. We have examined the lattice relaxation around the impurity and calculated the hyperfine coupling constants (HFCC). The results for the Mn electronic structure and for the HFCC are in agreement with experimental results using electron paramagnetic resonance measurements. © 2000 John Wiley & Sons, Inc. Int J Quant Chem 79: 34–46, 2000     

Local structure and local compressibilities around Co2+ impurity in ZnSiF6.6H2O crystal determined from electron paramagnetic resonance data.

The perturbation formulas of g-factors gparallel, gperpendicular and hyperfine structure constants Aparallel, Aperpendicular for 3d7 ion in trigonal octahedral crystal field are established on the basis of a cluster approach. These formulas consist of the contributions from configuration interaction and covalency effect and the parameters related to both effects can be estimated from the optical spectra and the structural data of the system under study. According to these formulas, the local trigonal distortion angle beta at pressure P = 0 and the local compressibilities d ln beta/dP in two pressure regions around Co2+ impurity in ZnSiF6.6H2O crystal are estimated by fitting the calculated electron paramagnetic resonance parameters gi, Ai and their pressure coefficients to the observed values. The results show that these local values are different from those of the host crystal because of the influence of impurity.     

Quasi-one-dimensional systems and localized defects: Some results of the Green's matrix formalism

The application of the self-consistent field (SCF ) local-impurity formalism to quasi-one-dimensional systems is discussed. We describe a general procedure for an accurate numerical determination of the Green's function matrix elements of the unperturbed system. An application to a local impurity in a model chain with two orbitals per unit cell is reported. The changes in the charge-bond-order matrix and in local and total density of states due to the impurity are discussed with special emphasis on the changes at the critical points (van Hove singularities) at the band edges. The Green's matrix approach is used to reexamine long-range Friedel oscillations caused by an impurity in a strictly one-dimensional metal. The extent of the long-range tail of the perturbed charge density is in an inverse relation to the localization length of the impurity state: the stronger the perturbation the more localized is the bound state and the more extended are the oscillations in the charge distribution. The results for the model chain with two orbitals per unit cell indicate that the impurity-induced change in charge distribution may be locally screened by redistribution of the population of the on-site orbitals, therefore damping possible oscillations and leading to a faster decay than in strictly one-dimensional systems.     

Studies of the spin Hamiltonian parameters and local structure for ZnO:Cu2+

The spin Hamiltonian parameters (the g factors and the hyperfine structure constants) and local structure for ZnO:Cu2+ are theoretically studied from the perturbation formulas of these parameters for a 3d9 ion under trigonally distorted tetrahedra. The ligand orbital and spin-orbit coupling contributions are taken into account from the cluster approach due to the significant covalency of the [CuO4](6-) cluster. According to the investigations, the impurity Cu2+ is suggested not to locate on the ideal Zn2+ site in ZnO but to undergo a slight outward displacement (approximately 0.01 angstroms) away from the ligand triangle along C3 axis. The calculated spin Hamiltonian parameters are in good agreement with the observed values. The validity of the above impurity displacement is also discussed.     

Quantum bits with polyacetylene

The dynamics of a polyacetylene single chain as a system for possible physical implementations of quantum bits is determined. This novel proposition is studied by varying intensity and duration of application of an electric field as well as the intensity, number, and position in the polymer chain of impurity molecules. The behavior of soliton pairs, whose associated energy levels form the quantum bit, is analyzed. The chain is modeled by a modified Pariser-Parr-Pople Hamiltonian extended to include the effects of an external electric field and the parameters of the impurity molecules. The effect of the variation of the field and impurities on the separation of the energy levels associated with soliton pairs is analyzed by numerical integration of the equations of motion. Two different approaches for controlling the separation of levels are presented, and their features compared. First, the use of changes in the electric field to control the distance (and ultimately coupling) between two solitons moving freely on the chain or captured by the potential generated by the impurity molecules. Second, the change in the intensity of the impurities alone, with no application of an external field. We have found that the effect of the use of the field on the separation of levels is much smaller than the one obtained by changes in the parameters of the impurity molecules, which eventually led us to achieve quantum bit behavior in a polyacetylene chain. The influence of the field and impurity parameters in the energy levels is determined, as well as their role in the coupling of the two solitons on the chain. Critical values for distance between solitons, intensity of field, and impurities that determine whether a pair of solitons can work as a quantum bit are obtained.     

Localized impurity states in the Hartree-Fock,LCAO approximation. I.

One-electron energies and wave functions for deep trap impurity electrons in a crystal are calculated by the Hartree-Fock, single determinant method. The interactions arising from a many-electron single determinant crystal wave function, with automatic inclusion of exchange effects, are those which determine the one-electron functions and energies. The crystal plus impurity system has no translational symmetry and hence the Bloch theorem is not applicable for the solution of the essentially infinite Hartree-Fock eigenvalue matrix. Thus we develop a technique in which the Hamiltonian and overlap matrices are written in terms of bordered matrices, with the interaction of the impurity functions with the rest of the crystal environment contained in the bordering rows and columns. The resulting secular equation explicitly includes the effects of orthogonalization of the entire basis set, including the impurity functions. This technique could be used in an iterative calculation of the electronic structure of a small number of electrons, assuming that the rest of the electrons in the environment are fixed according to an initial estimate.     

LiF-KF熔盐溶液局部结构的计算机模拟研究

本文用Monte Carlo法对同离子系LiF-KF熔盐溶液的局部结构进行了计算机模拟,介绍了计算方法和模型。计算了LiF, KF及Lif-KF混合前后正-正离子, 正-负离子, 负-负离子间位能变化, 各类离子的近邻离子排布规律, 以及各种形式离子团的组成比例。本文还讨论了在熔盐瞬时结构中存在的静电场的微区涨落。     

Theoretical studies of lattice distortions around the impurity ions in V2+ doped CdCl2, CdI2 and PbI2

The lattice distortions around the impurity ions in V(2+) doped CdCl(2), CdI(2) and PbI(2) are theoretically studied from the perturbation formulas of the spin Hamiltonian (SH) parameters zero-field splitting, g factors and the hyperfine structure constants for a 3d(3) ion in trigonal symmetry based on the cluster approach. In these formulas, the contributions from the s-orbitals of the ligands are taken into account. Based on the studies, it is found that the local angles beta (between the impurity-ligand bonding lengths and the C(3) axis) in the impurity centers are smaller than the angles beta(H) in the hosts. The calculated SH parameters based on the above local angles beta show better agreement than those on neglecting of the ligand s-orbital contributions (and those on the host angles beta(H)) with the experimental data.     

Influence of single impurity atoms on the structure, electronic, and magnetic properties of Ni5 clusters

With a gradient-corrected density functional method, we have studied computationally the influence of single impurity atoms on the structure, electronic, and magnetic properties of Ni5 clusters. The square-pyramidal isomer of bare Ni5 with six unpaired electrons was calculated 23 kJ/mol more stable than the trigonal bipyramid in its lowest-energy electronic configuration with four unpaired electrons. In a previous study on the cluster Ni4, we had obtained only one stable isomer with an O or an H impurity, but we located six minima for ONi5 and five minima for HNi5. In the most stable structures of HNi5, the H atom bridges a Ni-Ni edge at the base or the side of the square pyramid, similarly to the coordination of an H atom at the tetrahedral cluster Ni4. The most stable ONi5 isomers exhibit a trigonal bipyramidal structure of the Ni5 moiety, with the impurity coordinated at a facet, (micro3-O)Ni5, or at an apex edge, (micro-O)Ni5. We located four stable structures for a C impurity at a Ni5 cluster. As for CNi4, the most stable structure of the corresponding Ni5 complex comprises a four-coordinated C atom, (micro4-C)Ni5, and can be considered as insertion of the impurity into a Ni-Ni bond of the bare cluster. All structures with C and five with O impurity have four unpaired electrons, while the number of unpaired electrons in the clusters HNi5 varies between 3 and 7. As a rough trend, the ionization potentials and electron affinities of the clusters with impurity atoms decrease with the coordination number of the impurity. However, the position of the impurity and the shape of the metal moiety also affect the results. Coordination of an impurity atom leads to a partial oxidation of the metal atoms.