过渡金属夹心化合物的电子结构

本文利用过渡金属杂硼烷的结构规则,一般性地讨论了过渡金属夹心化合物的电子结构。得到N+1层(N个金属原子)夹心化合物的价成键轨道数为:VBO=6N+3-6N+5,与金属原子和配位环的性质无关。进而,通过用EHMO量子化学方法,对二、三和四层夹心化合物进行模型骨架计算,并结合实际化合物的结构分析,验证和讨论了上述公式的可靠性。     

确定硼烷的杂硼烷价成键轨道对称性的拓扑方法

本文通过对硼烷的分子轨道的定域化分析, 建立了由硼烷或杂硼烷的骨架多面体的几何性质, 确定其价成键轨道对称性的拓扑方法。从以多面体骨架的三角面和缺顶点周围的边为基约化出的不同约表示中, 按建议的能量与节面数的对应规则,选定出分子的价成键轨道所属的不可约表示。     

确定硼烷的杂硼烷价成键轨道对称性的拓扑方法

本文通过对硼烷的分子轨道的定域化分析, 建立了由硼烷或杂硼烷的骨架多面体的几何性质, 确定其价成键轨道对称性的拓扑方法。从以多面体骨架的三角面和缺顶点周围的边为基约化出的不同约表示中, 按建议的能量与节面数的对应规则,选定出分子的价成键轨道所属的不可约表示。     

过渡金属杂硼烷结构规则的量子化学计算

用EHMO量子化学计算方法,计算了过渡金属杂硼烷骨架Fe_{nB6-n(n=0,1,…,6),验证和讨论了过渡金属杂硼烷的价成键和价非键轨道数BMO+NBMO=4n1+9n2-F。其中n1、n2和F都只与骨架的几何性质有关。}     

硼烷结构规则的Xα方法研究

本文对B6H6^2^-,B7H7^2^-,B5H9,B6H10,B4H10,B5H11及其相应的硼骨架作了Xα.计算.讨论了硼烷的结构规则,Watson球对能级的影响以及电子占有数对成键轨道的影响等.     

碳硼烷结构规则的量子化学计算

本文对一系列封闭型C_nB_5-n(n=0～5)和C_nB_6-n(n=0～6)碳硼烷骨架及巢型C₄B_5-n(n=0～5)碳硼烷骨架进行了EHMO量子化学计算,根据计算结果讨论了碳硼烷的结构规则.     

硼烷的结构规则

本文讨论了不同类型多面体硼烷的结构规则,建立了硼烷成键分子轨道数与其硼多面体骨架的顶点数和面数之间的关系,并表述为统一的拓扑公式。对于单多面体硼烷结构,该公式与Wade规则等价,但是它还可以用于讨论各种稠合型多面体硼烷的结构。按此公式,可以认为硼烷的成键分子轨道数由硼多面体骨架完全确定。量子化学计算结果对此给以很好的验证。     

Ih对称性硼,碳原子簇化合物的从头计算（I）：B32,C2B30B32H…

本文用从头计算方法研究了含３２个顶点的硼烷Ｂ３２Ｈ３２＾０＾．＾２＾－及裸原子簇Ｂ３２与Ｃ２Ｂ３０的构型，稳定性及反应活性，Ｂ３２的优化计算结果表明，１２个５配位与２０个６配位两类硼原子不在同一球面时最稳定，而且所含两种Ｂ－Ｂ核间距离（Ｒ５６，Ｒ６６）的优化值验证了Ｌｉｐｓｃｏｍｂ的经验数值，Ｂ３２，Ｂ３２３２＾２＾－电子结构及原子布居的计算表明骨架成键轨道满足Ｗａｄｅ规则。相应的计算还表明，中性     

BnXn^0,^2^—（X=H,Cl;n=4,6,8,9,10,12）稳定性的从头计算研究

用双ξ型收缩高斯基对全卤代硼烷ＢｎＣｌｎ＾０＾，＾２＾－（ｎ＝４，６，８，９，１０，１２）进行了从头计算。讨论中性卤代硼烷稳定存在的原因及ＢｎＣｌｎ与ＢｎＣｌｎ＾２＾－稳定性随ｎ变化的不同趋势，并通过对Ｂ４Ｈ４＾２＾－结构规则的计算与分析，提出骨架成键轨道未填满电子是Ｂ４Ｈ４＾２＾－不稳定及迄今尚未发现中性ＢｎＨｎ存在的重要原因。     

Wade规则和唐敖庆拓扑规则间的关系

原于簇化合物的化学是当前活跃的研究领域之一。Lipscomb、wade、唐敖庆等对它们的结构做了许多工作。关于硼烷和碳硼烷的成键轨道总数——BMO,Wade提出了2n 1等规则,并把它推广到金属原子簇化合物;唐敖庆对硼烷和金属原子簇化合物,分别提出了4n—F和9n—l的拓扑规则。Wade从顶点数出发,唐敖庆则考虑面数和边数,我们根据多面体的拓扑性质,讨论二者间的关系。     

原子簇化合物的键价分析

根据原子簇化合物骨架的价电子结构及与配位体成键的性质,在确定原子簇骨架中存在的空轨道或孤对电子轨道数目后,按骨架价电子数目在骨架价成键轨道中的具体分配,推导了原子簇骨架的总键价数。再结合分子的几何构型,可以估计骨架中相邻原子间的成键情况。     

饱和烷烃分子C_nH_(2n+2)(n=4-6)的电子动量光谱(英文)

使用B3LYP/TZVP//B3LYP/aug-cc-pVTZ方法系统研究了饱和烷烃分子CnH2n+2(n=4-6)的轨道电子动量光谱,比较了同分异构体CnH2n+2(n=4-6)对轨道动量分布的影响.结合二维空间分析方法对电子在坐标空间中的密度分布进行了系统的研究.计算结果表明,最内价壳层电荷分布主要由s电子贡献,第二近邻芯价壳层则主要由p电子贡献,而其余的价壳层则为sp杂化.最内价轨道表现出最大的谱线强度并且远大于其它轨道的谱线强度,而且正烷烃的谱线强度要大于异烷烃等同分异构体的谱线强度,表现出了明显的与甲基移动的个数有关的性质.     

某些镧系化合物化学键特性的INDO研究

本文用INDO方法研究了不同价态镧系化合物的成键性质和4f轨道在成键中的作用,结果表明, 镧系化合物的成键受许多因素, 如价态、半径、配位数、空间构型等影响。不同配体与镧系元素成键的强度差别较大; 高价态的共价性大于低价态的; 配位数低的大于配位数高的。某些特殊构型的镧系化合物除σ键外, 还形成重叠较好的π配键,使Ln-L键共价性大大增强。4f轨道在成键中的作用比5d的少得多, 三价(二价态)的4f轨道基本定域(<0.1%), 四价态的4f轨道对成键的贡献明显增大, 可接近1%。     

ELECTRONIC CONFIGURATIONS OF TRANSITION METAL SANDWICH COMPLEXES

In this paper the electronic configurations of n+1-decker transition metal sandwich com-plexes have been generally discussed by means of the structural rule of transition metalheterocarborans and the numbers of their valence bonding orbitals have been obtained as fol-lows: VBO = 6n + 3-6n + 5,which are not dependent on the properties of transition metal atoms and coordination rings.Then the results of EHMO quantum chemistry calculations of the model skeletons and cor-responding analyses on electronic configurations of actual molecules for double-, triple- andtetra-decker sandwich complexes have been discussed to verify the above formula.     

Geometric and electronic structures of multiple-decker one-end open sandwich clusters: Eu(n)(C8H8)n- (n = 1-4)

We have measured the photoelectron spectra of the multiple-decker 1:1 sandwich clusters of Eu(n)(COT)n- (n = 1-4; COT = 1,3,5,7-cyclooctatetraene), synthesized in the gas phase, and studied theoretically the bonding scheme, charge distribution, valence orbital energies, and photodetachment energies. We calculated the ground electronic state X- and the first excited electronic state A-, both of which have strong ionic bonding and a characteristic charge distribution. Moreover, we found that the valence orbital energies of Eu (6s) and COT (L delta) depend strongly on cluster size and their positions in the clusters. With the calculated vertical detachment energies for these valence orbitals, we assigned the peaks in the experimental photoelectron spectra and analyzed the origin of their interesting behavior by employing simple point charge models. From these analyses, it became clear that the characteristic behavior of the spectra is due to the strong ionic bonding and the charge distribution. In addition, using the point charge models, we estimated the vertical detachment energies of the one-dimensional polymer [Eu(COT)]infinity-.     

手性异构体的片断染色计数

将配体取代看作对骨架点的染色, 通过染色片断的对称性分类, 直接计数取代手性和非手性异构体. 列表示出典型结果. 将Polya定理推广于陪集, 与片断染色计数进行比较。     

Localized molecular orbital studies on B_4C1_4,1,5-C_2B_3H_5 and B_nH_n~(2-)(n = 6-10, 12)

The wave functions, level energies and Mulliken population analysis of localized molecular orbitals (LMO's) for B4Cl4, 1,5-C2B3H5 and the closo-BnHn2- (n = 6-10, 12) are calculated by using the Edmiston-Reudenberg energy localization scheme under the CNDO/2 approximation in order to reveal the nature of quasi-aromaticity of the closo-BnHn2- (n > 5). It has been found that all the B-H or B-Cl LMO's are highly localized between the B and H (or Cl) atoms, corresponding to B-H or B-Cl o-bond, while the Bn framework bonding is formed mainly by the three-centered two-electron B-B-B bonds on the polyhedral faces. In the cases of B4Cl4 and 1,5-C2B3H5, these three-centered B-B-B bonds just fill their polyhedral faces; however, for the framework bonding of the closo-BnHn2- (n > 5), the valence electron deficiency leads to the delocalization of their three-centered B-B-B bonds, and as delocalizability of this three-centered B-B-B bond increases, some three-centered B-B-B bonds are further delocalized to become a f     

New structural motif of 18 valence electron molecules with a planar tetracoordinate heavier group 14 center: Unique stabilization effect of a π‐type skeleton

Proposing new valence electron counting rules and new structural motifs are both very important in chemistry. In this work, we unexpectedly found that by introducing a π‐type skeleton YCCY (Y = Al/Ga/In/Tl), a total of sixteen novel planar tetracoordinate heavier group 14 species, that is, ptM (M = Si/Ge/Sn/Pb) in neutral, can be designed as global minima. The underlying bonding situation contrasts sharply both with the well‐known 18ve‐ptC and the limited 18ve‐ptM, for which there is little multiple bonding character within the skeleton. The fact that each YCCY (Y = Al/Ga/In/Tl) can stabilize all heavier group 14 atoms in a planar tetracoordinate fashion strongly demonstrates the universality of such a π‐type skeleton. The present work firmly demonstrates that introducing the π‐type ligand skeleton can effectively enrich the planar tetracoordinate chemistry with the heavier group atoms.     

Computational study of analogues of the uranyl ion containing the -N=U=N- unit: density functional theory calculations on UO2(2+), UON+, UN2, UO(NPH3)3+, U(NPH3)2(4+), [UCl4[NPR3]2] (R = H, Me), and [UOCl4[NP(C6H5)3]

The electronic and geometric structures of the title species have been studied computationally using quasi-relativistic gradient-corrected density functional theory. The valence molecular orbital ordering of UO2(2+) is found to be pi g < pi u < sigma g < sigma u (highest occupied orbital), in agreement with previous experimental conclusions. The significant energy gap between the sigma g and sigma u orbitals is traced to the "pushing from below" mechanism: a filled-filled interaction between the semi-core uranium 6p atomic orbitals and the sigma u valence level. The U-N bonding in UON+ and UN2 is significantly more covalent than the U-O bonding in UON+ and UO2(2+). UO(NPH3)3+ and U(NPH3)2(4+) are similar to UO2(2+), UON+, and UN2 in having two valence molecular orbitals of metal-ligand sigma character and two of pi character, although they have additional orbitals not present in the triatomic systems, and the U-N sigma levels are more stable than the U-N pi orbitals. The inversion of U-N sigma/pi orbital ordering is traced to significant N-P (and P-H) sigma character in the U-N sigma levels. The pushing from below mechanism is found to destabilize the U-N f sigma molecular orbital with respect to the U-N d sigma level in U(NPH3)2(4+). The uranium f atomic orbitals play a greater role in metal-ligand bonding in UO2(2+), UN2, and U(NPH3)2(4+) than do the d atomic orbitals, although, while the relative roles of the uranium d and f atomic orbitals are similar in UO2(2+) and U(NPH3)2(4+), the metal d atomic orbitals have a more important role in the bonding in UN2. The preferred UNP angle in [UCl4(NPR3)2] (R = H, Me) and [UOCl4(NP(C6H5)3)]- is found to be close to 180 degrees in all cases. This preference for linearity decreases in the order R = Ph > R = Me > R = H and is traced to steric effects which in all cases overcome an electronic preference for bending at the nitrogen atom. Comparison of the present iminato (UNPR3) calculations with previous extended Hückel work on d block imido (MNR) systems reveals that in all cases there is little or no preference for linearity over bending at the nitrogen when R is (a) only sigma-bound to the nitrogen and (b) sterically unhindered. The U/N bond order in iminato complexes is best described as 3.