Topological Studies on the П…П Interactions between OCS, CO2, N2O and Hydrocarbon

采用MP2/aug-cc-pVDZ方法对氧硫化碳（OCS）、二氧化碳（CO2）、一氧化二氮（N2O）与乙烯（C2H4）、乙炔（C2H2）、2-丁炔（C4H6）之间形成的平行构型复合物中的分子间相互作用进行了理论研究.复合物的相互作用能按照B…C2H4〈B…C2H2〈B…C4H6（B=OCS,CO2,N2O）的顺序依次增大,相互作用距离按照B…C2H4〉B…C2H2〉B…C4H6（B=OCS,CO2,N2O）的顺序依次减小.采用电子密度拓扑分析理论方法,讨论了复合物中π…π作用的成键特性.电子密度拓扑分析表明复合物中形成了弱的分子间相互作用,且以静电作用为主;π电子密度分子图与全电子密度分子图中键径方向是一致的,说明π…π作用在本文所讨论的体系中起着很重要的作用.NBO分析表明净电荷迁移从电子给体C2H4,C2H2,C4H6到电子受体OCS,CO2,N2O,迁移数按照B…C2H4〈B…C2H2〈B…C4H6（B=OCS,CO2,N2O）的顺序依次增大,与相互作用能的顺序一致.     

OCS,CO2,N2O与烯、炔烃之间π…π作用的电子密度拓扑研究

采用MP2/aug-cc-pVDZ方法对氧硫化碳(OCS)、二氧化碳(CO2)、一氧化二氮(N2O)与乙烯(C2H4)、乙炔(C2H2)、2-丁炔(C4H6)之间形成的平行构型复合物中的分子间相互作用进行了理论研究.复合物的相互作用能按照B…C2H4B…C2H2>B…C4H6(B=OCS,CO2,N2O)的顺序依次减小.采用电子密度拓扑分析理论方法,讨论了复合物中π…π作用的成键特性.电子密度拓扑分析表明复合物中形成了弱的分子间相互作用,且以静电作用为主;π电子密度分子图与全电子密度分子图中键径方向是一致的,说明π…π作用在本文所讨论的体系中起着很重要的作用.NBO分析表明净电荷迁移从电子给体C2H4,C2H2,C4H6到电子受体OCS,CO2,N2O,迁移数按照B…C2H4相似文献   

(HAlNH)n(n=2～3)环状化合物的结构特征

用自洽场理论(HF)和密度泛函理论(DFT)的B3LYP方法,在6-31G*的水平上对化合物(HAlNH)2和(HAlNH)3的几何结构进行优化,并分别与环丁二烯C4H4和苯分子C6H6的结构和成键方式进行比较.以B3LYP/STO-3G方法讨论其分子轨道波函数(ψ).结果表明C4H4和(HAlNH)2均为D2h对称,前者为长方形结构,形成两个孤立的π键;而后者为菱形结构,形成一个π44键.C6H6和(HAlNH)3分子点群分别为D6h和D3h,并均形成一个π66键.成键原子对分子轨道的贡献不同,其中C原子是完全等价的,而Al和N原子各不相同,N原子比Al的贡献要大得多.     

(Cl_2AlNH_2)_n和(H_2AlNH_2)_n(n=1～ 5)簇结构及其热力学性质

用 HF自洽场理论和密度泛函理论 (DFT)的 B3LYP方法 ,在 6 31G水平上研究了低聚物 (Cl2AlNH2)n和 (H2AlNH2)n(n=1～ 5)簇的几何构型、电子结构和聚合反应热力学性质 ,比较了两个系列化合物中化学键的强度 .结果表明 ,Cl2AlNH2和 H2AlNH2分子为 C2υ (EC)平面型结构 ,其中 Al－ N为由一个σ键和一个π键组成的双键 .(Cl2AlNH2)n和 (H2AlNH2)n(n=1～ 5)分子为 Dnh对称 ,Al－ N是典型的σ单键 .低聚物 (Cl2AlNH2)n和 (H2AlNH2)n的稳定性顺序分别为 : 3 > 2 > 4> 5 > 1和 8 > 7 > 9 > 11 > 6.     

(1,3,5-C3P3H3)M与(1,3,5-C3P3H3)2M (M=Ti,V, Cr)配合物的结构与芳香性

运用密度泛函理论研究了(1,3,5-C3P3H3)M和(1,3,5-C3P3H3)2M (M=Ti,V,Cr)的结构、键合能以及芳香性.结果表明:低自旋的(1,3,5-C3P3H3)M和(1,3,5-C3P3H3)2M基态结构分别具有C3v和D3h对称性.金属与配体间为共价作用,二者之间存在σ、π和σ三种成键方式.V的三明治配合物的解离方式与Ti和Cr的三明治配合物不同,前者为分步解离,后两者则为一步解离.其中(1,3,5-C3P3H3)2Cr(D3h)的第一解离能最大,配合物最稳定.这些三明治和半三明治配合物都具有中心芳香性、内芳香性和外芳香性,且中心芳香性均大于自由配体(1,3,5-C3P3H3)的中心芳香性,芳香性主要贡献来源于π键和金属原子的孤对电子.内芳香性按照Ti、V、Cr的顺序依次增大,且内芳香性明显要大于外芳香性.高自旋的半三明治(1,3,5-C3P3H3)Ti(C3,5A1)与单重态(1,3,5-C3P3H3)Ti (C3v,1A1)相比,配体的变形性增大,稳定性增加,且C平面中心芳香性和内芳香性均增大,但P平面的中心芳香性却降低.     

平面五配位硅、 锗XBe5H6(X=Si,Ge)团簇

采用密度泛函理论PBE0方法, 在aug-cc-pVTZ水平上理论预测了含平面五配位硅和锗原子的XBe₅H₆ (X=Si, Ge)团簇. 势能面系统搜索及高精度量化计算表明, 它们均为全局极小结构. XBe₅H₆(X=Si, Ge)团簇整体呈完美的扇形结构: Si/Ge原子被5个金属Be原子配位; 4个H原子以桥基方式与Be原子相键连, 剩余的2个 H原子以端基方式与两端的Be原子成键. 化学键分析表明, XBe₅H₆(X=Si, Ge) 团簇中XBe₅单元具有完全离域的1个π及3个σ键, 外围铍氢间形成4个Be—H—Be 三中心二电子(3c-2e)键及2个定域的Be—H键. XBe₅单元上离域的2π及6σ电子赋予体系π和σ双重芳香性, 并使Si/Ge原子满足八隅律（或八电子规则）. 能量分解-化学价自然轨道分析揭示, Si/Ge和Be₅H₆之间主要为电子共享键.     

Cp_4An和COT_2An(Cp~-=C_5H_5~-,COT~(2-)=C_8H_8~(2-),An=U(Ⅳ),Pu(Ⅳ))的结构和光谱性质的密度泛函理论研究

采用密度泛函理论研究气相和四氢呋喃(THF)溶剂中Cp4An和COT2An(Cp-=C5H5-,COT2-=C8H82-,An=U(Ⅳ),Pu(Ⅳ))配合物的性质。THF溶剂对配合物的溶剂化效应采用类导体极化连续模型(CPCM)近似计算。计算结果显示在THF溶液中各配合物结合能的大小顺序为COT2PuCOT2UCp4PuCp4U。溶剂化效应降低了该金属有机配合物的结合能。计算得到的化合物的结构参数和红外光谱数据与实验数据保持一致。通过对Cp4An和COT2An(An=U(Ⅳ),Pu(Ⅳ))的分子轨道能级图分析发现,采用最高的RSC ECP赝势计算COT2U和Cp4U的基态分别为三重fφ2和fσ2组态;而COT2Pu和Cp4Pu的基态分别为五重fσ1fπ1fφ2和fσ3fδ1组态。     

铍-铍金属链夹心配合物D4d [Ben(C4H4)2]2- 及[Ben(C4H4)2]Li2 (n=2–8)

中文：采用密度泛函理论方法(B3LYP和BP86)在6-311+G(d,p)基组水平上系统研究了新颖的铍-铍金属链夹心配合物[Ben(C4H4)2]2- 及 [Ben(C4H4)2]Li2 (n=2–8) 的几何结构、电子结构、成键特征及热力学稳定性。结果表明,具有交错式D4d 对称性的[Ben(C4H4)2]2-及[Ben(C4H4)2]Li2 为体系势能面上的真正极小。自然键轨道(NBO)、分子中的原子(AIM)及分子轨道分析表明该系列夹心配合物中铍-铍间主要以共价键为主,而配体与铍-铍链之间则主要以离子键为主。核独立化学位移(NICS)分析表明配体在该系列配合物中具有π芳香性。稳定的夹心配合物锂盐[Ben(C4H4)2]Li2 (n=2–8)有望通过C4H4Li2/C5H5-配体交换反应进行制 备,该系列配合物将进一步丰富多核夹心配合物研究领域。     

配体稳定的二元过渡金属团簇[PdAu8(PR3)8]2+(R=Me,OMe,H,F,Cl,CN)的量子化学理论研究

采用从头计算MP2方法和密度泛函理论方法,对过渡金属团簇[PdAu8(PR3)8]2+(R=Me,OMe,H,F,Cl,CN)的几何结构、电子结构以及团簇各组成部分之间的结合能进行了研究.MP2方法和SVWN局域泛函能够对团簇的结构给予准确的描述,而离域泛函BP86,PBE,BLYP和杂化泛函B3LYP则过高地估计了团簇的几何结构参数.电子结构研究表明Pd,Au原子通过d电子的成键作用构成团簇内核[PdAu8]2+,[PdAu8]2+与PR3配体则通过"σ给予/π反馈"模式成键.PR3配体与[PdAu8]2+的结合能够加强Pd-Au之间的成键作用,增大前线轨道能级间隙,从而提高团簇的稳定性.PR3配体中 R 基团供、吸电能力的变化对[PdAu8(PR3)8]2+结构的影响较小,但对[PdAu8]2+ -pR3结合能的影响较大.能量分析显示不同PR3与[PdAu8]2+之间具有相近的轨道作用能,与R基团供、吸电能力相关的非轨道作用能成为影响两者连接牢同程度的决定因素.     

系列杂氮钛三环中的分子内弱相互作用的紫外光电子能谱和理论研究

首次报道了四种杂氮钛三环的紫外光电子能谱,结合量子化学从头算和和电子密度拓扑分析方法对这些化合物的电子结构和分子内存在的弱相互作用进行了分析研究。通过优化STO-6G(d)基组(C:1s=5.66,ζ2s=1.675,ζ2p=1.66;O:ζ1s=7.67,ζ2s=2.25,ζ2p=2.20;N:ζ1s=6.66,ζ2s=1.91,ζ2p=1.89;H:ζ1s=1.24)对所研究的化合物进行了分子轨道计算,结合计算结果对化合物的紫外光电子能谱进行了解析和指认。实验得到的体现分子内弱相互作用σN-Ti的轨道电子的电离能表明了N,Ti间相互作用的弱成键特性,电子密度拓扑分析显示N,Ti原子间存在体现成键作用的键鞍点,键鞍点处电子密度的拓扑性质也进一步支持了N,Ti间弱成键作用的特性。     

Double bonds in the second and third periods. Ab initio study of the conjugation in HnX  YHm?ZH2 (X,Y = C,N, SI,and P; Z = B and N; n = 1, 2; m = 0, 1)

Ab initio SCF calculations were performed to study the conjugation of C, N, Si, and P double bonds with BH₂ (π-acceptor) and NH₂ (π-donor). The variations of the energy, geometry, and electronic distribution on rotation ZH₂ groups connected to the double bonds depend greatly on the polarities and polarizabilities of the molecules under study. The repulsive (attractive) interactions of the lone pairs lying in the plane of the double bond with donor (acceptor) orbital can modify strongly the relative stabilities of the conformations and the parameters of the molecule and electronic structures.     

膦配体对金团簇[Au@Au8(PR3)8]3+(R=Me,OMe,H,F,Cl,CN)稳定化作用的理论研究

采用ab initio HF, MP2方法和密度泛函理论方法, 对具有D2h和D4d构型的膦配体稳定的过渡金属团簇[Au@Au8(PR3)8]3+(R=Me, OMe, H, F, Cl, CN)进行了几何结构、 电子结构及团簇稳定性等方面的研究. 计算表明, 与D2h构型相比, D4d构型更稳定, 两者能量相差约5~10 kJ/mol. SVWN局域泛函能够对团簇的几何结构给予较准确的描述, MP2方法对团簇的结构参数有所低估, 而离域和杂化泛函则过高地估计了团簇的结构参数. 电子结构分析表明, 中心Au原子与外围的Au原子之间通过 d 电子的成键作用构成团簇内核[Au@Au8]3+, [Au@Au8]3+与PR3配体则通过"σ给予/π反馈"模式成键. PR3配体与[Au@Au8]3+的结合能够加强内核-外围Au原子间的成键作用, 缩小外围Au原子在成键上的差异, 增大前线轨道能级间隙, 从而提高团簇的稳定性. PR3配体中R基团供、 吸电子能力的变化对[Au@Au8(PR3)8]3+结构影响较小, 但对[Au@Au8]3+-PR3结合能影响较大. 能量分析显示, 不同PR3配体与[Au@Au8]3+之间具有相近的轨道作用能, 与R基团供、 吸电子能力相关的非轨道作用能成为影响两者连接牢固程度的决定因素.     

Diamagnetic group 6 tetrakis(di-tert-butylketimido)metal(IV) complexes

The addition of 4 equiv of LiN=C-t-Bu(2) to CrCl(3), MoCl(5), and WCl(6) in diethyl ether produced the complexes M(N=C-t-Bu(2))(4) (M = Cr, Mo, W). Single-crystal X-ray diffraction studies revealed that the molecules have flattened tetrahedral geometries with virtual D(2d) symmetry in the solid state. (1)H and (13)C NMR spectra indicated that the complexes are diamagnetic, and a qualitative MO analysis showed that the orthogonal π-donor and -acceptor orbitals of the ketimide ligand cooperatively split the d(xy) and d(z2) orbitals sufficiently to allow spin pairing in the d(xy) orbital. A more sophisticated quantum-mechanical analysis of Cr(N=C-t-Bu(2))(4) using density functional/molecular mechanics methods confirmed the qualitative analysis by showing that the singlet state is 27 kcal/mol more stable than the triplet state.     

Density functional study of the sigma and pi bond activation at the Pd=X (X = Sn, Si, C) bonds of the (H2PC2H4PH2)Pd=XH2 complexes. Is the bond cleavage homolytic or heterolytic?

The mechanism for the activation of the sigma bonds, the O-H of H2O, C-H of CH4, and the H-H of H2, and the pi bonds, the C[triple bond]C of C2H2, C=C of C2H4, and the C=O of HCHO, at the Pd=X (X = Sn, Si, C) bonds of the model complexes (H2PC2H4PH2)Pd=XH2 5 has been theoretically investigated using a density functional method (B3LYP). The reaction is significantly affected by the electronic nature of the Pd=X bond, and the mechanism is changed depending on the atom X. The activation of the O-H bond with the lone pair electron is heterolytic at the Pd=X (X = Sn, Si) bonds, while it is homolytic at the Pd=C bond. The C-H and H-H bonds without the lone pair electron are also heterolytically activated at the Pd=X bonds independent of the atom X, where the hydrogen is extracted as a proton by the Pd atom in the case of X = Sn, Si and by the C atom in the case of X=C because the nucleophile is switched between the Pd and X atoms depending on the atom X. In contrast, the pi bond activation of C[triple bond]C and C=C at the Pd=Sn bond proceeds homolytically, and is accompanied by the rotation of the (H2PC2H4PH2)Pd group around the Pd-Sn axis to successfully complete the reaction by both the electron donation from the pi orbital to Sn p orbital and the back-donation from the Pd dpi orbital to the pi orbital. On the other hand, the activation of the C=O pi bond with the lone pair electron at the Pd=Sn bond has two reaction pathways: one is homolytic with the rotation of the (H2PC2H4PH2)Pd group and the other is heterolytic without the rotation. The role of the ligands controlling the activation mechanism, which is heterolytic or homolytic, is discussed.     

Synthesis and structural features of α-acyloxy-(η-allyl)palladium complexes

α-Acetoxy (η³-allyl)palladium complexes were prepared from acyloxy functionalized allylsilanes under mild conditions and in good isolated yields. The substituent and ligand effects of the acetoxy group on the palladium-allyl bonding were studied by X-ray diffraction. These studies show that the acetoxy group generates a strongly deformed bonding between the metal atom and the allyl moiety. This unsymmetrical bonding is modulated by the σ-donor/π-acceptor properties of the ligands. The ¹³C NMR studies indicated that the shift values correlate with the carbon-palladium bond lengths and the inductive effects of the acetoxy group.     

M2(hpp)4Cl2 and M2(hpp)4, where M = Mo and W: preparations, structure and bonding, and comparisons with C2, C2H2, and C2Cl2 and the hypothetical molecules M2(hpp)4(H)2

The reaction between M(2)Cl(2)(NMe(2))(4), where M = Mo or W, and Hhpp (8 equiv) in a solid-state melt reaction at 150 degrees C yields the compounds M(2)(hpp)(4)Cl(2) 1a (M = Mo) and 1b (M = W), respectively, by the elimination of HNMe(2) [hpp is the anion derived from deprotonation of 1,3,4,6,7,8-hexahydro-2H-pyrimido[1,2-a]pyrimidine, Hhpp]. Purification of 1a and 1b is achieved by sublimation of the excess Hhpp and subsequent recrystallization from either CH(2)Cl(2) or CHCl(3) (or CDCl(3)). By single-crystal X-ray crystallography, the structures of 1a and 1b are shown to contain a central paddlewheel-like M(2)(hpp)(4) core with Mo-Mo = 2.1708(8) A (from CH(2)Cl(2)), 2.1574(5) A (from CDCl(3)), W-W = 2.2328(2) A (from CDCl(3)), and M-N = 2.09(1) (av) A. The Cl ligands are axially ligated (linear Cl-M-M-Cl) with abnormally long M-Cl bond distances that, in turn, depend on the presence or absence of hydrogen bonding to chloroform. The quadruply bonded compounds M(2)(hpp)(4), 2a (M = Mo), and 2b (M = W), can be prepared from the reactions between 1,2-M(2)R(2)(NMe(2))(4) compounds, where R = (i)()Bu or p-tolyl, and Hhpp (4 equiv) in benzene by ligand replacement and reductive elimination. The compounds 2a and 2b are readily oxidized, and in chloroform they react to form 1a and 1b, respectively. The electronic structure and bonding in the compounds 1a, 1b, 2a, and 2b have been investigated using gradient corrected density functional theory employing Gaussian 98. The bonding in the M-M quadruply bonded compounds, 2a and 2b, reveals M-M delta(2) HOMOs and extensive mixing of M-M pi and nitrogen ligand lone-pair orbitals in a manner qualitatively similar to that of the M(2)(formamidinates)(4). The calculations indicate that in the chloride compounds, 1a and 1b, the HOMO is strongly M-Cl sigma antibonding and weakly M-M sigma bonding in character. Formally there is a M-M triple bond of configuration pi(4)sigma(2), and the LUMO is the M-M delta orbital. An interesting mixing of M-M and M-Cl pi interactions occurs, and an enlightening analogy emerges between these d(4)-d(4) and d(3)-d(3) dinuclear compounds and the bonding in C(2), C(2)H(2), and C(2)Cl(2), which is interrogated herein by simple theoretical calculations together with the potential bonding in axially ligated compounds where strongly covalent M-X bonds are present. The latter were represented by the model compounds M(2)(hpp)(4)(H)(2). On the basis of calculations, we estimate the reactions M(2)(hpp)(4) + X(2) to give M(2)(hpp)(4)X(2) to be enthalpically favorable for X = Cl but not for X = H. These results are discussed in terms of the recent work of Cotton and Murillo and our attempts to prepare parallel-linked oligomers of the type [[bridge]-[M(2)]-](n)().     

Structural and Electron Density Studies on a Chromium(IV)-Oxo Complex [CrIV(O)(TMP)]

The electron density distribution of a chromium(IV)-oxo complex, [Cr^IV(O)(TMP)] (TMP = 5,10,15,20-tetrakis-p-methoxyphenyl porphyrin), is investigated by molecular orbital calculation. The molecular and crystal structure of the compound is studied by x-ray diffraction. It belongs to the space group 1 2, Z = 2, a = 14.979(4) Å, b = 9.752(3), c = 15.605(3) Å, β = 100.97(2)°, V = 2238(1) ų, Mo Kα radiation λ = 0.7107 Å, R = 4.9%, Rw = 3.5% for 3575 observed reflections. Cr is five-coordinated in a square pyramidal fashion with the Cr atom located 0.42 Å toward the oxo-ligand. Deformation density maps are derived from the single point molecular orbital calculation on the basis of HF and DFT(density functional theory) calculations. The accumulation of deformation density along the C-H, C-C, C-N and C-O bonds in the porphyrin ligand is well represented. The asphericity in electron density around the Cr ion is clearly demonstrated. Natural bond orbital analysis (NBO) reveals that the Cr-O_oxo is actually a triple-bond character (σ²π⁴) and the four N of pyrrole serves as a σ-donor to Cr. The Cr-N_pyrrole bond is essentially a dative bond d-Orbital populations of Cr derived from both calculations are in good agreement with each other. Planar d_π-orbital is the most populated, which is in accord with the prediction from crystal field theory. Detail bond characterization of the Cr-L, multiple bond is discussed.     

Structure and dynamics of tetrakis(thiophosphinato)resorcinarene complexes of silver(I), gold(I), and palladium(II)

The coordination chemistry of the tetrakis(thiophosphinato)resorcinarene sulfur-donor ligands [(C6H2CH{CH2CH2Ph})4{OC(O)R}4{OP(=S)Ph2}4] (L), where R = OCH2Ph, 4-C6H4CH3, C6H11, C4H3S, or OCH2CCH, is reported. Both silver(I) and gold(I) form cationic complexes of the type [LM2]2+, in which the ligand acts as a bis(chelate) in forming complexes with linear S-M-S (M = Ag or Au) stereochemistry. Gold(I) also forms the unusual complex [L(AuCl)2][LAu2]2+, which forms a supramolecular polymer through intermolecular aurophilic attractions. Palladium(II) forms the complex [LPd2Cl2(mu-Cl)2], in which the dipalladium(II) unit extends the natural bowl structure of the resorcinarene. The solid-state and solution conformations of the complexes, as determined by X-ray structure determination and NMR spectroscopy, respectively, are similar, but several complexes were found to exhibit dynamic behavior in solution, involving either conformational mobility of the resorcinarene unit or intermolecular ligand exchange.     

Density functional theoretical study of a series of binary azides M(N3)n (n = 3, 4)

Geometrical structures of a series of binary azides M(N3)n (M = elements in groups 3 and 13 (n = 3) and in groups 4 and 14 (n = 4)) were investigated at the B3LYP/6-311+G level of theory. Our calculations found that binary group 3 triazides M(N3)3 (M = Sc, Y, La) and binary group 4 tetraazides M(N3)4 (M = Ti, Zr, Hf) turn out to be stable with all frequencies real having a similar linear M-N-NN structural feature, as previously reported for M(N3)4 (M = Ti, Zr, Hf). However, binary azides of group 13 M(N3)3 (M = B, Al, Ga, In, Tl) and group 14 elements M(N3)4 (C, Si, Ge, Sn, Pb) with bent M-N-NN bond angles differ obviously from binary group 3 and 4 azides in geometrical structure. These facts are mainly explained by the difference in electronic density overlap between the central atom and the alpha-N atoms of the azido groups. Two lone-pair electrons on the sp hybridization alpha-N atoms in the binary group 3 and 4 azides donate electron density into two empty d orbitals of the central transition metal atom and a pair of valence bonding electrons, resulting in the alpha-N atoms acting as a tridentate ligand. The sp2 hybridization alpha-N atoms of the binary group 13 and 14 azides only give one valence electron to form one valence bonding electron pair acting virtually as monodentate donors.