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。     

硼烷结构规则的量子化学计算

利用EHMO方法,对n=5～12的完整多面体硼烷骨架、缺一个和两个顶点以及戴一个和两个帽原子的各种异构体进行了量子化学计算。直接对硼烷的价成键轨道数公式BMO=4n-[f+3(s+1)]进行了验证。在对计算结果讨论的基础上,进一步探讨了骨架几何结构与成键轨道数之间的关系。     

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。     

硼烷及杂硼烷簇合物的结构规则

硼烷及杂硼烷簇合物的结构规则张晓辉，陈利平，由业诚，王国栋（大连大学师范学院化学系大连１１６０３５）关键词原子簇化合物，稠合硼烷，杂硼烷，结构规则本文在研究前人工作的基础上［１－１２］，利用徐光宪提出的超额电子数概念，将硼烷分成多个分子片，以讨论它们...     

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.     

硼原子簇和碳原子簇

本文在一般性地讨论多面体硼烷和碳烷骨架几何性质的基础上,探讨了以已知封闭型硼烷(碳烷)骨架为基础,在保持对称性下依次进行截角-戴帽,交替地得到多面体碳烷(硼烷)-硼烷(碳烷)骨架系列的方法,并以构造I_h和O_h对称性系列作为例子。在此基础上,讨论了可能存在的多面体硼烷和碳烷以及高硼和高碳裸体原子簇的结构和性质。     

14顶点双取代碳硼烷和金属硼烷极化率和二阶超极化率的DFT研究

采用量子化学密度泛函理论(DFT) B3LYP/6-31G(d)方法对14顶点双取代碳硼烷和金属硼烷几何构型进行优化, 结合有限场(FF)方法计算了各体系的极化率和二阶超极化率. 同时金属硼烷中金属原子采用赝势基组进行计算, 讨论基组对计算结果的影响. 结果表明, 14顶点碳硼烷和金属硼烷中碳和金属元素的成键方式不同, 金属硼烷中各原子间距离比碳硼烷中大, 平面偏移角增大. 金属原子的引入有效增加分子的NLO系数, 同时金属硼烷的前线分子轨道能级差比碳硼烷小很多, 金属硼烷材料有可能表现出半导体甚至导体特性, 金属原子采用不同基组对计算结果影响不大.     

质子化硼烷正离子体系电子结构的理论研究

本文用a b initio计算法和近似a b initio计算法(PRDDO)研究了质子化硼烷正离子体系的电子结构,给出了一些正离子体系的优化几何构型并讨论了它们的成键情况。计算的硼烷分子质子亲和势与实验值相当吻合。     

碳硼烷和碳硼炔金属配合物中金属-碳键的化学性质

碳硼烷和碳硼炔金属配合物中的金属-碳键具有不同于经典金属-碳键的化学性质.一方面,二十面体碳硼烷独特的电子和空间效应使得碳硼烷金属配合物中的金属-碳键不参与和不饱和分子的反应 另一方面,在一定条件下具有大空间位阻的碳硼笼可以诱导某些碳-碳偶联反应.然而,碳硼炔金属配合物中的金属-碳键能与多种不饱和分子发生反应,其反应模式取决于中心金属离子的电子构型.本文简要总结了我们近期在这方面的研究进展.     

Studies on the structural rule of boranes

The authors discuss the structural rule of different kinds of polyhedral boranes and propose a general topological formula for calculating the number of bonding molecular orbitals. In the case of single polyhedral boranes, results obtained from the formula are the same as those from the famous Wade rule. Futhermore, the formula can also be used to calculate the number of bonding molecular orbitals of joined-type polyhedral boranes. We have also made some quantum chemistry calculations to verify the concept that the number of bonding molecular orbitals of boranes can be determined by considering only the corresponding boron polyhedral frameworks.     

The bonding in boron and transition-metal cluster compounds

A method is described for constructing qualitatively the molecular orbitals of an approximately spherical cluster of boron or transition-metal atoms. The method gives a way of understanding the electron-counting rules for such clusters, the preference for deltahedral structures, the relationship between closo boranes on the one hand and nido and arachno boranes on the other, and Mingos' capping and condensation principles for transition-metal clusters.     

A unifying electron-counting rule for macropolyhedral boranes, metallaboranes, and metallocenes.

A generally applicable electron-counting rule-the mno rule-that integrates macropolyhedral boranes, metallaboranes, and metallocenes and any combination thereof is presented. According to this rule, m + n + o number of electron pairs are necessary for a macropolyhedral system to be stable. Here, m is the number of polyhedra, n is the number of vertices, and o is the number of single-vertex-sharing condensations. For nido and arachno arrangements, one and two additional pairs of electrons are required. Wade's n + 1 rule is a special case of the mno rule, where m = 1 and o = 0. B20H16, for example has m = 2 and n = 20, leading to 22 electron pairs. Ferrocene, with two nido polyhedral fragments, has m = 2, n = 11, and o = 1, making the total 2 + 11 + 1 + 2 = 16. The generality of the mno rule is demonstrated by applying it to a variety of known macropolyhedral boranes and heteroboranes. We also enumerate the various pathways for condensation by taking icosahedral B12 as the model. The origin of the mno rule is explored by using fragment molecular orbitals. This clearly shows that the number of skeletal bonding molecular orbitals of two polyhedral fragments remains unaltered during exohedral interactions. This is true even when a single vertex is shared, provided the common vertex is large enough to avoid nonbonding interactions of adjacent vertices on either side. But the presence of more than one common vertex results in the sharing of surface orbitals thereby, reducing the electronic requirements.     

Cluster increments for macropolyhedral boranes

Cluster increments derived for individual cluster fragments reproduce the DFT computed relative stabilities of macropolyhedral boranes usually within +/-6 kcal mol(-1). A simple summation procedure helps to select the best partner for a given cluster fragment in order to construct the thermodynamically most stable macropolyhedral borane. Cluster increments are considerably smaller for nido-cluster fragments with an even number of vertexes than for odd nido-cluster fragments pointing towards high thermodynamic stability of macropolyhedral boranes with even numbered nido-units.     

Bonding of the chain structure for novel boranes B_(3k+)H_(5k+p+3)~-

The molecular orbitals obtained from conventional quantum chemistry calculations, are expressed in terms of symmetrized valence bond functions of fragment, and a direct picture of chemical bonding can be drawn easily. This method is utilized, together with extended Huckel calculations, to interpret the bonding properties of a centipede-like chain structure for novel laser-producing boranes B3k+pH5k+p+3- which is constructed from the repeated unit B3H5 linked to each other by three B-H-B bonds.     

Reversal of stability on metalation of pentagonal-bipyramidal (1-MB6H7(2-) 1-M-2-CB5H7(1-) and 1-M-2,4-C2B4H7) and Icosahedral (1-MB11H12(2-) 1-M-2-CB10H12(1-) and 1-M-2,4-C2B9H12) boranes (M = Al, Ga, In, and Tl): energetics of condensation and relationship to binuclear metallocenes

The usual assumption of the extra stability of icosahedral boranes (2) over pentagonal-bipyramidal boranes (1) is reversed by substitution of a vertex by a group 13 metal. This preference is a result of the geometrical requirements for optimum overlap between the five-membered face of the ligand and the metal fragment. Isodesmic equations calculated at the B3LYP/LANL2DZ level indicate that the extra stability of 1-M-2,4-C(2)B(4)H(7) varies from 14.44 kcal/mol (M = Al) to 15.30 kcal/mol (M = Tl). Similarly, M(2,4-C(2)B(4)H(6))(2)(1-) is more stable than M(2,4-C(2)B(9)H(11))(2)(1-) by 9.26 kcal/mol (M = Al) and by 6.75 kcal/mol (M = Tl). The preference for (MC(2)B(4)H(6))(2) over (MC(2)B(9)H(11))(2) at the same level is 30.54 kcal/mol (M = Al), 33.16 kcal/ mol (M = Ga) and 37.77 kcal/mol (M = In). The metal-metal bonding here is comparable to those in CpZn-ZnCp and H(2)M-MH(2) (M= Al, Ga, and In).     

α-Keggin结构钼硅四电子杂多蓝的量子化学研究

采用半经验的INDO法,首次完成了α-Keggin 结构钼硅四电子杂多蓝K~ 3H~ 5[Simo^v~4-Mo^Ⅵ~8O~4~0].12H~2O量子化学计算,获得102个成键轨道和68 个反键轨道,轨道能级,键序及电荷等数据,证明了杂多酸盐还原产物杂多蓝,还原后Keggin结构阴离子中各原子上电子云密度重新分配,产生一定程度的结构畸变, 但仍保持α-Keggin结构,最高占据轨道由组成分子的各原子轨道组成,其中的桥氧(O~b'O~c)成分较多,表明O~b'O~c为分子中的主要化学活性点HOMO和LUMO为负值, 表明仍可进一步接受电子生成四电子以上的杂多蓝,Muliken分析进一步证明了还原钼原子的位置.     

Bonding of the chain structure for novel boranes B3k+pH−5k+p+3

The molecular orbitals obtained from conventional quantum chemistry calculations, are expressed in terms of symmetrized valence bond functions of fragment, and a direct picture of chemical bonding can be drawn easily. This method is utilized, together with extended Huckel calculations, to interpret the bonding properties of a centipede-like chain structure for novel laser-producing boranes B_3k+pH^?_5k+p+3 which is constructed from the repeated unit B₃H₅ halted to each other by three B—H—B bonds.