一种新的分子拓扑指数及其在QSPR/QSAR研究中的应用

通过引入量子数、键参数,认为分子的性质与其中各原子的电负性、价电子数、成键电子数、价层主量子数及各化学键的键长有关,提出了一种新的分子拓扑指数mAY.采用该拓扑指数对饱和烷烃、烷基苯、烷氧氯硅烷、卤代苯、含氮杂环化合物、碱金属卤化物及卤化锡的性质/活性进行了相关关系的研究.结果表明,mAY与有机物和无机物的性质/活性间具有良好的相关性.     

分子价连接性指数中杂原子价点价计算新方法及应用

对分子价连接性指数中杂原子点价δ^v~i的计算方法进行了改进,提出了一种计算杂原子价点价δ^h~i的新方法,认为分子中某一杂原子i的价点价δ^h~i值不仅与它的价层电子数Z~i、最高主量子数n~i以及结合的氢原子数目h~i有关,还与它所在的族烽N~i、陷氢图中连接的其他原子的数目m~i以及杂化方式L~p有关。杂原子i的δ^h~i值与原子i的Pauling电负性具有相近的物理意义。用由δ^h~i构成的分子价连接性指数^nχ^h(n=0,1,2)研究了取代芳烃和烃衍生物的物理化学性质和生物活性,结果表明,^1χ^h比^1χ^v有显著的改善,计算值与实验值接近的程度更高。     

卤代苯的沸点与分子结构的定量关系

原子点价是分子连接性指数的核心概念.本文提出了一个计算原子点价δiz'的新方法,其公式为: δiz'=mi(Zi-hi)Vi/Ei/ni2(1) 式中,ni,mi,Zi分别是原子i的核外电子层数、成键电子数和价电子数,hi是与原子i直接相连的氢原子数,Vi,Ei分别是分子图中原子i的顶点度和边度.     

新定义的价连接性指数与有机物理化活性的相关性研究

基于分子中成键原子i的结构特征和所处的化学环境,新定义了原子的价点价δYi,以价连接矩阵为基础构建了一个新的能表征含多重键、杂原子分子结构信息的价连接性指数mωY. mωY对有机化合物异构体具有很强的选择性和区分能力.用0ωY, 1ωY和分子中的含碳数NC研究了有机物的一系列理化活性,其相关性良好,并发现不同的性质,0ωY, 1ωY和NC所起的作用程度是有所不同的.新模型物理意义明确,计算简便,对不同类型有机物的不同理化活性具有良好的估算和预测能力,计算值与实验值的吻合程度均优于相应文献的结果.     

结构参数P与Abn型无机物总键能的关系

把量子数和价电子能级值引入原子点价,重新定义原子点价为iδP,并用iδP构建分子结构参数P.P与56种ABn型无机物的总键能ΔE呈现高度的相关性,其相关系数为0.988 2.与其他结构参数相比,本参数的计算更为准确.     

分子连接性指数mXz与烷基苯标准生成焓的定量关系

提出了计算有机物分子中成键原子点价δzi的新方法,以δzi为核心建构了一个新的分子连接性指数mXz(m=0,1),并探讨了mXz指数与烷基苯标准生成焓-△fH()m的相关性,结果表明,mXz指数对于烷基苯具有良好的结构选择性和性质相关性.以0Xz,1Xz和碳原子数Ⅳ为自变量的三元线性回归方程为-△fH()m=58.008 0Xz+27.075 1Xz+929.836N-1504.311,该方程对烷基苯标准生成焓的预测结果令人满意.     

单分子连接性指数mZh与取代芳烃急性毒性的定量关系

本文提出了一个计算有机物分子中成键原子点价δiz'的新方法,基于原子点价δiz'和分子图的邻接矩阵建构一种新的分子连接性指数mZh为:     

分子连接性指数(mZh)与烷基苯理化性质的相关性研究

定义有机物分子中成键原子点价δiz.基于δiz和分子图的邻接矩阵,建构一种新的分子连接性指数mZh(m=0,1),并研究了0Zh,1Zh与烷基苯的燃烧热、等张比容、沸点、汽化热、标准生成自由能、标准熵、摩尔体积、溶解度、正辛醇/水分配系数等10种物理化学性质的相关性.结果表明:0Zh,1Zh与烷基苯的物理化学性质具有优良的性质相关性,二元相关系数均在0.99以上;以0Zh,1Zh和分子中C原子数NC为自变量的三元线性回归方程对烷基苯理化性质的预测结果相当令人满意.     

一个新的连接性指数用于脂肪醇QSPR/QSAR研究

本文提出了一个计算分子中成键原子点价δzi的新方法,其公式为:δzi=Zi(Zi-hi)Vi/Ei/n2i式中,ni,Zi分别为原子i的核外电子层数和价电子数,hi为与原子i直接相连的氢原子数,Vi,Ei分别为分子图中原子i的顶点度和边度.     

主族金属元素电子脱出功与拓扑指数~mP的相关性

利用Pauling电负性xpi、原子的价电子数mi和原子的价电子层数ni构建了点价iδ.由点价iδ构建了拓扑指数mP.利用其0阶指数0P与23种金属元素电子脱出功关联,拟合成3个线性回归方程.相关系数为0.9803,0.9870和0.9878,均优于文献值.预测取得了较好的结果.     

Novel topological index for research on structure-property relationships of complex organic compounds

Based on bonding parameters such as Yang's Electronegative Force Gauge Y(i), electronic number of valence layer Z(i), number of combined hydrogen atoms h(i), number of bonding electron b(i), and quantum number such as the highest main quantum number of valence layer n(i), a novel atomic valence delta(i) (Y) is defined and a novel topological index (1)chi(Y) is derived from the atomic valence. The atomic valence is defined as delta(i) (Y) = (Z(i) - h(i))b(i)/n(i) (2)Y(i), while the topological index is expressed as (1)chi(Y) summation operator (i,j=1) (m) (delta(i) (Y)delta(j) (Y))(-1/2). Subsequently, the index (1)chi(Y) is utilized to study the structure-property relationships of complex organic compounds. The results of correlativity showed that the index is highly and extensively correlated with such properties as solubility of phenyl chlorides, gas chromatographic retention index of alkoxyl silanes, and toxicity of heterocyclic nitrogen-containing compounds. Moreover, predicted values are quite consistent with experimental ones when the index is employed to predict the partition coefficient (log P) of fatty alcohols, phenyl chlorides, and barbitals. Compared to the topological indices reported in the literature, the universality and reliability of (1)chi(Y) to the properties of complex organic compounds have been distinctively improved, and its calculating process is simple and convenient.     

碱金属卤化物的F心能带、晶格能、标准熵的拓扑研究

基于Kier的点价(δiv)及量子数(如ni)定义新的原子点价(δit), 并在邻接矩阵基础上建构连接性指数(mF)。用其中1F分别与20种碱金属卤化物的F心能带[E(F)]、晶格能(U)、标准熵(Smθ)关联,它们的相关系数(R)依次为0.9922、0.9972、0.9918。符合Mihalic等人提出的建模要求(R>0.99)。结果表明,mF将在化合物的QSPR/QSAR研究中成为具有广泛、良好相关性的结构参数。     

一个新的拓扑指数用于有机化合物的QSPR/QSAR研究

在分子图的邻接矩阵和距离矩阵的基础上提出了一个新的拓扑指数Xu,该拓扑指数易于计算,对C~2-C~1~6饱和烷烃有较高的结构区分能力,通过适当的处理可方便地推广到含多重键杂原子体系。该指数与饱和烷烃的正常沸点等理化性质,不饱和链烃类化合物的热容以及某些脂肪醇的毒性和疏水性参数均具有较好的性质相关性。绝大多数理化性质与Xu指数均能建立简单线性模型,且相关系数均大于0.99,表明该指数有望在QSPR/QSAR研究中作为一个新的参数而获得推广应用。     

Toward a physical understanding of electron-sharing two-center bonds. I. General aspects

In 1916, Lewis and Kossel laid the empirical ground for the electronic theory of valence, whose quantum theoretical foundation was uncovered only slowly. We can now base the classification of the various traditional chemical bond types in a threefold manner on the one- and two-electron terms of the quantum-physical Hamiltonian (kinetic, atomic core attraction, electron repulsion). Bond formation is explained by splitting up the real process into two physical steps: (i) interaction of undeformed atoms and (ii) relaxation of this nonstationary system. We aim at a flexible bond energy partitioning scheme that can avoid cancellation of large terms of opposite sign. The driving force of covalent bonding is a lowering of the quantum kinetic energy density by sharing. The driving force of heteropolar bonding is a lowering of potential energy density by charge rearrangement in the valence shell. Although both mechanisms are quantum mechanical in nature, we can easily visualize them, since they are of one-electron type. They are however tempered by two-electron correlations. The richness of chemistry, owing to the diversity of atomic cores and valence shells, becomes intuitively understandable with the help of effective core pseudopotentials for the valence shells. Common conceptual difficulties in understanding chemical bonds arise from quantum kinematic aspects as well as from paradoxical though classical relaxation phenomena. On this conceptual basis, a dozen different bond types in diatomic molecules will be analyzed in the following article. We can therefore examine common features as well as specific differences of various bonding mechanisms.     

Relationship between the Auger parameter and the ground state valence charge at the core-ionized site

A simple semi-empirical model that correlates the Auger parameter to the ground state valence charge of the core-ionized atom with closed valence shell configuration, and which was previously applied to Cu(I) (3d¹⁰) compounds, is extended to Ba (II) (5d¹⁰), Pb (II) (5d¹⁰4s²), and Zn (II) (3d¹⁰) compounds (halides and chalcogenides). Until now, the Auger parameter was employed to separate initial and final state effects that influence the core electron binding energy. In agreement with our model, a linear relationship is found between the Auger parameter shift and the ground state Bader valence charge obtained by density functional theory (DFT) calculations.     

过渡金属羰基簇合物的键价计算和分析

本文运用原子簇化合物键价计算公式 ,对过渡金属羰基簇合物成键情况进行了分析 ,利用金属键轨道数 ,价非键轨道数和金属配体成键轨道数计算簇合物价轨道总数 .计算结果表明 :簇合物价轨道总数与金属键轨道数成线性关系 ,BT=9N -Bn.对于一般簇合物其价轨道总数与Lauher的EHMO计算结果 ,与唐敖庆的结构拓扑规则一致 ,对于反常的高核簇合物其价轨道总数与按化学式计算的 1/ 2VE相吻合     

电负性研究(Ⅱ)—氢的电负性

氢的电负性值是氢元素性质的重要参数，１９３２年Pauling犤１～３犦定量确定氢的相对电负性值等于２．１，１９６１年Allred犤４，５犦用更准确的实验数据对Paul－ing电负性标度进行了修正，氢的电负性值被确定为２．２，目前这两个数值都在采用。元素的电负性值是与元素的性质紧密相关的，一个合适的电负性标度应该至少反映所有重要元素的电负性值，氢的化合物比任何其它元素都多，理应有一个基本的准确电负性值，然而一些电负性标度中却缺乏这样的数据。在Murphy等四人犤６犦最近发表的论文中，对Pauling电负性标度又进行了深入考查与…     

Electronic structure,Compton profiles and cohesive properties of Cs-halides

We have reported energy bands, density of states, valence electron charge densities and Compton profiles of CsCl, CsBr and CsI using linear combination of atomic orbitals with Hartree–Fock and density functional theories. We have also computed these properties, except the momentum densities, using full potential linearized augmented plane wave method. The general features of the energy bands and the density of states in these halides are found to be almost similar. To interpret the theoretical data on Compton line shapes, we have also measured the Compton profiles using our 20 Ci ¹³⁷Cs spectrometer. It is seen that the Hartree–Fock calculations give relatively a better agreement with the experimental momentum densities. On the basis of equal-valence-electron-density profiles, a comparison of relative nature of bonding is made which is in agreement with the valence charge densities and atomic charges by means of Mulliken analysis. Using our experimental and theoretical Compton profiles, we have also computed the cohesive energy of the halides.     

Stereochemistry of post-transition metal oxides: revision of the classical lone pair model

The chemistry of post transition metals is dominated by the group oxidation state N and a lower N-2 oxidation state, which is associated with occupation of a metal s(2) lone pair, as found in compounds of Tl(I), Pb(II) and Bi(III). The preference of these cations for non-centrosymmetric coordination environments has previously been rationalised in terms of direct hybridisation of metal s and p valence orbitals, thus lowering the internal electronic energy of the N-2 ion. This explanation in terms of an on-site second-order Jahn-Teller effect remains the contemporary textbook explanation. In this tutorial review, we review recent progress in this area, based on quantum chemical calculations and X-ray spectroscopic measurements. This recent work has led to a revised model, which highlights the important role of covalent interaction with oxygen in mediating lone pair formation for metal oxides. The role of the anion p atomic orbital in chemical bonding is key to explaining why chalcogenides display a weaker preference for structural distortions in comparison to oxides and halides. The underlying chemical interactions are responsible for the unique physicochemical properties of oxides containing lone pairs and, in particular, to their application as photocatalysts (BiVO(4)), ferroelectrics (PbTiO(3)), multi-ferroics (BiFeO(3)) and p-type semiconductors (SnO). The exploration of lone pair systems remains a viable a venue for the design of functional multi-component oxide compounds.