过渡金属和硅烯配体相互作用的理论研究(Ⅰ)——MSiH2+的从头算研究

以HF/6-311+G^*基组研究了过渡金属硅烯离子MSiH₂⁺(M从Sc至Cu)的构型、成键特征以及M-Si键解离能.具有共平面构型的MSiH₂⁺,其M=Si键带有明显的双键特征,M=Si键解离能从Sc至Cu呈现周期性变化,与M的金属离子激发能有近似的线性关系.     

CO2在α-U(001)表面的吸附和解离

采用广义梯度密度泛函理论研究了0.25ML覆盖度下CO₂在α-U（001）表面上的吸附和解离,得到了CO₂的稳定吸附构型和吸附能,确定了CO₂的解离过渡态和解离能垒,探讨了CO₂与表面U原子的相互作用本质.结果表明CO₂趋向以C（O）-U多键结合方式在α-U（001）面发生强化学吸附,吸附能为1.24-1.67 eV;C-O键的活化程度依赖于表面电子向CO₂发生转移的程度.CO₂与表面U原子的相互作用主要来自于U原子电子向CO₂最低空轨道（LUMO）2π_u转移,以及CO₂π_u/1π_g/3σ_u-U 6d轨道间杂化而生成新的化学键.以形成3个C-U键和6个O-U键模式在穴位1和穴位2上发生吸附的CO₂（H1-C₃O₆和H2-C₃O₆）的解离吸附能分别为3.15和3.13 eV,解离能垒分别为0.26和0.36 eV,预示着吸附CO₂分于易于解离形成CO分子和O原子.     

多硝基尿酸衍生物含能性质的理论研究

为了寻找兼具优异爆轰性能和良好热力学及动力学稳定性的高能材料, 本文设计了15个硝基尿酸化合物, 运用密度泛函理论, 对其性质进行了研究. 通过半经验的K-J方程和比冲量预测了其爆炸性能, 结果表明, 所设计分子的爆热、 分子密度、 爆炸速率和爆炸压强同硝基取代基数目之间存在较强的线性关系. 三硝基尿酸和四硝基尿酸衍生物的爆炸速率超过了8.0 km/s, 爆炸压强超过了30 GPa, 并且大多数衍生物的比冲量要高于目前经常使用的炸药黑索金. 通过计算N—NO₂键的解离能、 特征落高、 分子的自由空间预判了衍生物的稳定性和撞击感度, 结果显示, 绝大多数分子有大于80 kJ/mol的键解离能. 本文的理论结果可以为实验上设计合成新的高能材料提供一些有用的信息.     

密度泛函法计算C1-C14正构烃生成焓及C-C键裂解能

采用密度泛函理论(DFT)方法研究了费托石脑油裂解反应中涉及到C₁-C₁₄正构烃和自由基中间体的生成焓及其C-C键解离能(BDE)。 结果表明,在所有评价的密度泛函理论方法（B97-1、BB1K、B1B95、MPWB1K和MPW1B95）中,MPW1B95/6-311G(d,p)方法计算最精确。 以此方法为基准,进一步对高碳烃及其裂解产物的标准生成焓和C-C键解离能进行了预测。 与可得到的实验数据相比,MPW1B95/6-311G(d,p)方法预测的烃和自由基的平均生成焓分别为0.8和2.7 kJ/mol,C-C键解离能的平均绝对误差只有3.1 kJ/mol,表明此方法不仅可准确计算正构烃标准生成焓和C-C键解离能,而且还能正确预测C-C键解离能变化趋势。     

吲哚咪唑基钌(Ⅱ)联吡啶配合物与酵母RNA的相互作用

通过紫外-可见光谱和荧光光谱滴定、稳态荧光猝灭和溴化乙啶竞争键合实验研究了Ru(Ⅱ)配合物[Ru(bpy)(H₂iip)₂](ClO₄)₂{bpy=2,2′-联吡啶, H₂iip=2-(吲哚-3-基)-咪唑[4,5-f][1,10]-邻菲罗啉}的酵母RNA键合性质. 结果表明, 二者键合模式为嵌入键合, 其键合常数为7.09×10⁶ L/mol, 比小牛胸腺DNA的键合常数大, 且比同类配合物[Ru(bpy)₂(H₂iip)](ClO₄)₂的酵母RNA键合常数大.     

理论研究丁羟粘合剂化学键解离及其对力学性能的影响

端羟基聚丁烯(HTPB)是推进剂中的常用的粘合剂,老化是其贮存和使用中的重要问题。通过量子化学计算HTPB 与甲基二异腈酸酯(TDI)形成的网络模型简化结构中化学键的均裂解离能(BDE),分析了键能与老化分解的关系。键能计算结果证明可靠且可用于比较分析。与CH₂ 基团相连的C-O 键的BDE值最小,推测该键最弱并且在热老化过程会发生断裂分解,降解产物主要是CO₂。HTPB 中的烯丙基伯羟基与TDI 形成的聚氨酯中α-C-H 属于最弱的X-H(X=C, N)键,推测其容易受到自由基的进攻发生氢转移反应。对容易断裂分解的C-O 键,提出了可能的老化机理。计算的C-O 键断裂活化能与其解离能近似相等,热老化过程中断键生成自由基并通过无势垒过程释放出CO₂。整个过程的热老化半衰期是温度的指数衰减函数,表明随着温度的提高HTPB-TDI 聚氨酯老化加速。热力学计算证明老化形成的氨基自由基和烷基自由基能够重新结合。采用分子动力学动态分析方法,分析了HTPB-TDI 聚氨酯网络老化前后的结构变化及其对弹性力性质的影响,发现释放CO₂ 的过程伴随着体系密度降低。对假定的CO₂ 扩散聚集以及CO₂ 从体系中扩散消失的模型进行了模拟,发现拉伸模量和剪切模量在这两种情形下会增加。     

亚汞氢氧化物Hg2(OH)2结构的理论研究

采用从头计算HF, MP2方法和密度泛函方法,选择LanL2DZ和SDD基组,对Hg₂(OH)₂的几何构型、振动频率和稳定性进行了研究,并与Hg₂F₂和Hg₂Cl₂的稳定性进行了对比.研究表明Hg的5s, 5p准内层电子参与了Hg与Hg之间的成键作用,Hg-Hg键强烈的电子相关作用使得HF方法不适用于该体系的研究.Becke的离域校正给出较大的Hg-Hg键长,而局域的DFT方法和MP2方法则给出了合理的结构参数、振动频率和能量.相对论效应使Hg-Hg键缩短24 pm,增加Hg-Hg键的强度达20%左右.Hg₂(OH)₂的稳定性与Hg₂F₂和Hg₂Cl₂的稳定性相当.虽然在气相中Hg₂L₂(L=F, Cl, OH)比其分解物HgL₂和Hg要稳定,但相对论效应降低了这种趋势.     

266 nm激光光解C2H5SSC2H5产物的激光诱导荧光光谱

有机硫化物是大气主要污染物之一,其在大气中的光解产物还将造成二次污染,除了存在于有机硫化物中, S―S键还存在于胱氨酸等蛋白质中, S―S键的形成和断裂决定该类蛋白质的活性.本工作中,我们研究了用实验室常见的Nd:YAG激光器的四倍频266 nm激光光解C₂H₅SSC₂H₅过程,通过激光诱导荧光(LIF)光谱方法检测乙硫自由基C₂H₅S等光解产物.实验表明266 nm激光主要光解C₂H₅SSC₂H₅的S―S键产生C₂H₅S自由基.本文应用密度泛函理论的Becke3-Lee-Yang-Parr泛函(B3LYP方法)得到C₂H₅SSC₂H₅的S―S键、C―S键和C―C键的解离势能曲线,可知在266 nm光解条件下, C₂H₅SSC₂H₅在基态能够发生S―S键、C―S键解离, C―C键不发生解离.本文采用全活化空间自洽场(CASSCF)方法优化得到态和态的C₂H₅S自由基结构及其跃迁的绝热激发能,以辅助解析实验检测的C₂H₅S自由基的LIF光谱.实验结合理论计算最终得出,本实验266 nm光解条件下, C₂H₅SSC₂H₅主要发生S―S键解离,不排除少量分子发生C―S键解离的可能性.     

硝酸碳酰肼合钴、镍、铜含能配合物结构和性质的理论研究

对硝酸三碳酰肼合钴([Co(CHZ)₃](NO₃)₂)、硝酸三碳酰肼合镍([Ni(CHZ)₃](NO₃)₂)和硝酸二碳酰肼合铜([Cu(CHZ)₂(NO₃)₂])进行密度泛函理论计算研究, 获得其稳定分子的几何构型、电子结构、红外光谱以及热化学性质. 研究结果表明, 这三种配合物均表现出六配位八面体结构, 而铜配合物中的硝酸根参与了配位. 自然键轨道分析表明, 配体和金属离子之间存在供体-受体相互作用, 致使配位氨基N—H键上的成键轨道电子发生离域, 进而导致氨基N—H键的电子占据数降低、键长增大、键级减小、伸缩振动频率红移, 这与实测红外光谱变化规律很好地吻合. 标题化合物的金属离子均为＋1氧化态, 金属-氮配位键都是共价键, 而Cu—O配位键是离子键. 通过计算求得理论反应热, 预测这些配合物的合成均为放热反应; 由生成热大小推测标题物的稳定性次序为[Ni(CHZ)₃](NO₃)₂＞[Co(CHZ)₃](NO₃)₂＞[Cu(CHZ)₂(NO₃)₂], 与实测热稳定性次序完全吻合.     

可见光催化二氧化碳参与多氟芳烃的选择性C-F键羧基化（英文）

二氧化碳(CO₂)具有廉价易得、无毒、可循环再生等优点,是合成化学中优良的碳一(C1)合成子,可用于多种大宗化学品及精细化学品的合成.然而,由于CO₂具有较高的热力学稳定性及动力学惰性,其在温和条件下选择性转化较为困难.多氟芳基羧酸是一种重要的含氟砌块,具有独特的物化性质及生理活性,在医药、农药和有机光电材料等领域中均有广泛应用.多氟化合物C-F键的选择性羧基化反应是构建含氟羧酸的重要手段之一.然而,由于C-F键具有较高的键解离能,实现其选择性断裂及官能团化反应较为困难,因此CO₂参与芳基C-F键的羧基化反应面临着极大的挑战.目前,该领域仅有少量关于电化学和过渡金属催化的报道,且存在需使用牺牲阳极、当量的金属还原剂、额外引入导向基以及反应条件苛刻等问题,因此,需要发展其他策略实现温和条件下CO₂参与的芳基C-F键羧基化反应.可见光是一种来源广泛、可再生的清洁能源.可见光催化反应具有条件温和、官能团兼容性高和绿色环保等优点,在近年来得到了较大的发展,并为多种惰性底物以及惰性化学键的活化提供了新的手段....     

Transition‐Metal Complexes [(PMe3)2Cl2M(E)] and [(PMe3)2(CO)2M(E)] with Naked Group 14 Atoms (E=C–Sn) as Ligands; Part 1: Parent Compounds

The equilibrium geometries and bond dissociation energies of 16‐valence‐electron(VE) complexes [(PMe₃)₂Cl₂M(E)] and 18‐VE complexes [(PMe₃)₂(CO)₂M(E)] with M=Fe, Ru, Os and E=C, Si, Ge, Sn were calculated by using density functional theory at the BP86/TZ2P level. The nature of the M? E bond was analyzed with the NBO charge decomposition analysis and the EDA energy‐decomposition analysis. The theoretical results predict that the heavier Group 14 complexes [(PMe₃)₂Cl₂M(E)] and [(PMe₃)₂(CO)₂M(E)] with E=Si, Ge, Sn have C_2v equilibrium geometries in which the PMe₃ ligands are in the axial positions. The complexes have strong M? E bonds which are slightly stronger in the 16‐VE species 1ME than in the 18‐VE complexes 2ME . The calculated bond dissociation energies show that the M? E bonds become weaker in both series in the order C>Si>Ge>Sn; the bond strength increases in the order Fe<Ru<Os for 1ME , whereas a U‐shaped trend Ru<Os<Fe is found for 2ME . The M? E bonding analysis suggests that the 16‐VE complexes 1ME have two electron‐sharing bonds with σ and π symmetry and one donor–acceptor π bond like the carbon complex. Thus, the bonding situation is intermediate between a typical Fischer complex and a Schrock complex. In contrast, the 18‐VE complexes 2ME have donor–acceptor bonds, as suggested by the Dewar–Chatt–Duncanson model, with one M←E σ donor bond and two M→E π‐acceptor bonds, which are not degenerate. The shape of the frontier orbitals reveals that the HOMO?2 σ MO and the LUMO and LUMO+1 π* MOs of 1ME are very similar to the frontier orbitals of CO.     

Infrared spectroscopic and theoretical studies of the OTiF(2), OZrF(2) and OHfF(2) molecules with terminal oxo ligands

The isolated group 4 metal oxydifluoride molecules OMF(2) (M = Ti, Zr, Hf) with terminal oxo groups are produced specifically on the spontaneous reactions of metal atoms with OF(2) through annealing in solid argon. The product structures and vibrational spectra are characterized using matrix isolation infrared spectroscopy as well as B3LYP density functional and CCSD(T) frequency calculations. OTiF(2) is predicted to have a planar structure while both OZrF(2) and OHfF(2) possess pyramidal structures, all with singlet ground states. Three infrared absorptions are observed for each product molecule, one M-O and two M-F stretching modes, and assignments of these molecules are further supported by the corresponding (18)O shifts. The molecular orbitals of the group 4 OMF(2) molecules show triple bond character for the terminal oxo groups, which are also supported by an NBO analysis. These molecular orbitals include a σ bond (O(2p) + Ti(sd hybrid)), a normal electron pair π bond (O(2p) + Ti(d)), and a dative π bond arising from O lone pair donation to the overlapping Ti d orbital. The M-O bond dissociation energies for OMF(2) are comparable to those in the diatomic oxide molecules. The OTiF intermediate is also observed through two slightly lower frequency bond stretching modes, and its yield is increased in complementary TiO + F(2) experiments. Finally, the formation of group 4 OMF(2) molecules is highly exothermic due to the weak O-F bonds in OF(2) as well as the strong new MO and M-F bonds formed.     

As-5、[As5M]-、[As5MAs5]2- (M=Ti,Zr, Hf)的结构和芳香性

用密度泛函理论(DFT)研究了As-5、[As5M]-和[As5MAs5]2- (M=Ti, Zr, Hf)的结构、频率、能量以及芳香性, 详细讨论了体系中不同类型的键和电子如化学键、孤对电子、核电子等对总的核独立化学位移(NICS)的影响. 结果表明, As-5、[As5M]-和[As5MAs5]2-的基态结构分别具有D5h、C5v和D5h对称性, 而且都具有芳香性. As-5 (D5h)的芳香性主要来源于As—As π键和As—As σ键的作用. [As5M]-(C5v)中各种As—M键的NICS分割值占主要优势, 其次是As—As之间形成的σ键. [As5TiAs5]2-(D5h)中, As—As π键的作用占主要优势. [As5ZrAs5]2-(D5h)中, As—As π键对体系总的NICS贡献相对减小, 而As—Zr键的作用增强. [As5HfAs5]2-(D5h)的芳香性主要来自As—Hf键的作用.     

A comparison of the reactivity of Ni atoms toward CH4, SiH4, and SnH4: a combined matrix isolation and quantum-chemical study

Nickel atoms are shown to react spontaneously with SiH(4) and SnH(4) to give the insertion products HNiSiH(3) and HNiSnH(3). With CH(4), however, no spontaneous reaction occurs, in agreement with earlier reports; HNiCH(3) can be formed only on photolytic activation of the Ni atom. The reaction products were characterized experimentally by IR spectroscopy, including the effect of isotopic substitution (H/D), and by quantum-chemical calculations. They all have C(s) symmetry with a terminal Ni--H bond and three terminal E--H bonds (E=Si, Sn). Strikingly, the H-Ni-E bond angles are less than 90 degrees, and there is a weak interaction between the H atom bound to Ni and the E atom. The structures are compared with those of other molecules of general formula MSiH(4) that have been characterized recently in our group (M=Ti, Ni, Ga). While TiSiH(4) has three Ti-H-Si bridges, both NiSiH(4) and GaSiH(4) exhibit only terminal Ni--H and E--H bonds, but with the difference that there is no interaction between the H atom bound to Ga and the Si atom.     

Why are the Homoleptic Diyl Complexes M(InR)4 with M = Ni and Pt Stable Compounds while only Ni(CO)4 but not Pt(CO)4 can become Isolated? A Theoretical Study of M(EMe)44 and M(CO)4 (M = Ni,Pd, Pt; E = B,Al, Ga,In, Tl)

The equilibrium geometries and first bond dissociation energies of the homoleptic complexes M(EMe)₄ and M(CO)₄ with M = Ni, Pd, Pt and E = B, Al, Ga, In, Tl have been calculated at the gradient corrected DFT level using the BP86 functionals. The electronic structure of the metal‐ligand bonds has been examined with the topologial analysis of the electron density distribution. The nature of the bonding is revealed by partitioning the metal‐ligand interaction energies into contributions by electrostatic attraction, covalent bonding and Pauli repulsion. The calculated data show that the M‐CO and M‐EMe bonding is very similar. However, the M‐EMe bonds of the lighter elements E are much stronger than the M‐CO bonds. The bond energies of the latter are as low or even lower than the M‐TlMe bonds. The main reason why Pd(CO)₄ and Pt(CO)₄ are unstable at room temperature in a condensed phase can be traced back to the already rather weak bond energy of the Ni‐CO bond. The Pd‐L bond energies of the complexes with L = CO and L = EMe are always 10 — 20 kcal/mol lower than the Ni‐L bond energies. The calculated bond energy of Ni(CO)₄ is only D_o = 27 kcal/mol. Thus, the bond energy of Pd(CO)₄ is only D_o = 12 kcal/mol. The first bond dissociation energy of Pt(CO)₄ is low because the relaxation energy of the Pt(CO)₃ fragment is rather high. The low bond energies of the M‐CO bonds are mainly caused by the relatively weak electrostatic attraction and by the comparatively large Pauli repulsion. The σ and π contributions to the covalent M‐CO interactions have about the same strength. The π bonding in the M‐EMe bonds is less than in the M‐CO bonds but it remains an important part of the bond energy. The trends of the electrostatic and covalent contributions to the bond energies and the σ and π bonding in the metal‐ligand bonds are discussed.     

Ab initio study of the transition-metal carbene cations

The geometries and bonding characteristics of the first-row transition-metal carbene cations MCH_2~ were investigated by ab initio molecular orbital theory (HF/LANL2DZ). All of MCH_2~ are coplanar. In the closed shell structures the C bonds to M with double bonds; while in the open shell structures the partial double bonds are formed, because one of the σ and π orbitals is singly occupied. It is mainly the π-type overlap between the 2p_x orbital of C and 4p_x, 3d_(xz), orbitals of M~ that forms the π orbitals. The dissociation energies of C—M bond appear in periodic trend from Sc to Cu. Most of the calculated bond dissociation energies are close to the experimental ones.     

Electronic states and nature of bonding of the molecule NiSi by all electron ab initio HF-CI and CASSCF calculations

All electron ab initio Hartree-Fock (HF), configuration interaction (CI) and multiconfiguration self-consistent field (CASSCF) calculations have been applied to investigate the low-lying electronic states of the NiSi molecule. The ground state of the NiSi molecule is predicted to be¹Σ⁺. The chemical bond in the¹Σ⁺ ground state is a double bond composed of one σ and one π bond. The σ bond is due to a delocalized molecular orbital formed by combining the Ni 4s and the Si 3pσ orbitals. The π bond is a partly delocalized valence bond, originating from the coupling of the 3dπ hole on Ni with the 3pπ electron on Si. Withing the energy range 1 eV 18 electronic states have been identified. The lowest lying electronic states have been characterized as having a hole in either the 3dπ or the 3dδ orbital of Ni, and the respective final states are formed when either of these holes are coupled to the 3pπ valence electron of Si.     

Electronic states and nature of the chemical bond in the molecule CrC by all-electron ab initio calculations

All-electron ab initio Hartree–Fock (HF ), valence configuration interaction (CI ), and multiconfiguration self-consistent-field (CASSCF ) calculations have been applied to investigate the electronic states of the CrC molecule. The molecule is predicted as having four low-lying electronic states, ³∑^?, ⁵∑^?, ⁷∑^?, and ⁹∑^?, separated by an energy gap of 0.55 eV from the next higher-lying state, ¹∑^?, which is followed by the states ⁵Π and ⁷Π. The four lowest-lying electronic states are due to the coupling of the angular momenta of the ⁶S_g Cr⁺ ion with those of the ⁴S_u C^? anion. The chemical bond in the ³∑^? ground state can be viewed as a quadruple bond composed of two σ and two π bonds. One σ bond is due to the formation of a molecular orbital that is doubly occupied. The remaining bonds, i.e., one σ and two π bonds, arise from valence-bond couplings. The π bonds originate from the valence-bond couplings of the electrons in the C 2pπ orbitals with those in the Cr 3dπ orbitals. The σ bond originates from the valence-bond coupling of the C 2pσ electron with an electron in the Cr 4s, 4p hybrid that is polarized away from the C atom.     

过渡金属卡宾正离子的从头算研究

过渡金属卡宾正离子被认为是如烯烃的聚合和烷基金属的分解过程等许多反应的中间体．较为稳定的环丁烷金属离子和环戊烷金属离子已从相应酮的脱羰反应获得［１］．Ｊａｃｏｂｓｏｎ等［２］研究了ＦｅＣＨ＋２和ＣｏＣＨ＋２与烯烃和环烷烃的气相反应．Ｍｃｋｅｅ［３］在...