丙烯酰基正离子的红外光解离光谱研究

利用脉冲激光溅射-超声分子束载带离子源在气相中产生了[H_3C_3O]~+和[D_3C_3O]~+离子及贴附CO的[H_3C_3O?CO]~+和[D_3C_3O?CO]~+络合物离子.通过贴附CO的络合物离子的红外光解离光谱实验获得了[H_3C_3O]~+和[D_3C_3O]~+离子的红外光谱.通过比较实验光谱和理论模拟光谱,确定了[H_3C_3O]~+离子为丙烯酰基正离子,其电子基态为~1A′,具有C_s对称性.适应性自然密度划分分析方法(Ad NDP)成键分析表明,丙烯酰基正离子除了定域的CH,CC,COσ键和两个简并COπ键以外,还存在一个离域的三中心两电子CCCπ键.     

H_5~+的几何构型及电子激发态研究

本文使用组态相互作用(CI)与多组态自洽场(MCSCF)相结合的方法,对H_5~+进行了研究。得到H_5~+为H_3~+·H_2复合体的新构型,属C_2点群。且给出了H_5~+的电子激发态能量。     

分子离子NO+激发态的势能函数

100公里以上的大气分子离子主要为NO~+。它的辐射特点及它与电子、原子或分子的相互作用,对于理解大气的化学过程具有特别重要的意义。为了研究这些过程,确定NO~+分子离子基态及其各个激发态的分子势能函数是非常重要的。精确的X~1Σ~+,A~1Ⅱ和a~3∑~+势能曲线已发表;基于光电子谱的研究发现了NO~+的其它激发态,但对于这些激发态的研究尤其是势能函数的研究不多。本文研究并导出NO~+的基态和10个激发态的势能函数。     

H~3^+的精确量子化学计算

本文采用组态相互作用方法(CI), 对H~3^+的基态和三个低激发态3^A~1,1^A~1和3^Σ~u^+进行了计算研究。结果表明, 键函数方法不失为一个可供选择的精确量子化学计算方法。     

HeNa及HeNa~+光谱的理论研究

利用从头算Molecule-UHF程序计算得到HeNa分子的基态~2∑3s及激发态~2∏3p和HeNa~+的~1∑2p、~3∑3s及~t∑3s态的势能曲线,并在此基础上利用自编的程序计算了态-态间光谱跃迁的Franck-Condon因子.结果说明HeNa分子的基态是不稳定的,激发态2∏3p有一个较浅的势阱,HeNa~+的1∑2p有一个较浅的势阱,而~3∑3s态及~t∑3s态分别存在一个很深的势阱.     

HeLi^n^+(n=0, 1)簇合物的稳定性和垂直激发态光谱

本文用ab initio研究了簇合物HeLi^n^+(n=0, 1)的几何构型和成键性质。在MP2(FULL)/6-31G**, 水平优化所得LeLi^+的平衡键长为0.2062nm, 与实验值0.205nm十分吻合。比较了HeLi^+(X^1∑^+和a^3∑^+), HeLi(X^2∑^+和a^4II)以及HLi(X^1∑^+)的稳定性, 计算了HeLi^+基态的相关能, 势能曲线和垂直激发态光谱。计算采用了6-31G**, 6-311G**,6-311G(2df, 2pd), 6-311G(3df, 2pd)和6-311+G(3df, 2pd)基组; 采用的方法包括MP2(FULL), MP4, MCSCF, MRSDCI, CCD和ST4CCD。计算表明, 同价HeLi^n^+中激发态的离解能均远比基态的大, 其中HeLi^+(a^3∑^+)的离解能最高(60.49kj/mol),说明激发态是稳定束缚态。HeLi^+基态比等电子体HLi分子基态的稳定性小得多。HeLi^+由A^1∑^+到B^1II的垂直跃迁(3σ→1π)振子强度较大而垂直跃迁能较小。     

光驱动三氯化钒络合物溶液的氧化还原反应的电子吸收光谱考察

过渡金属络合物的电子吸收光谱是其基态分子的电子跃迁到激发态的重要表征方法,已经成为观测光化学过程中活性中间物及金属离子的氧化态变化的有效手段.中心金属离子与配位体之间的电荷转移(CT),是过渡金属络合物光驱动氧化还原反应的原因. VCl_3在乙醇中形成[VCl_2(C_2H_5OH)_4]~+Cl~-络合物(以下简写为VCl_3(C_2H_5OH)_4),在近紫外光辐照下,它发生氧化还原反应,C_2H_5OH氧化成CH_3CHO,而V~(3+)原为V~(2+),     

β-羟基丙醛基态与激发态氢迁移反应的从头算研究

本文用从头算RHF和UHF方法在3-21G基组上研究了β-羟基丙醛基态和激发态分解为甲醛和乙烯醇的反应机理。优化得到了各反应途径的过渡态和中间体, 其结果为: 基态β-羟基丙醛经过一个六元环过渡态和一个氢键中间体形成产物, 反应属于氢迁移和断键的协同过程; 激发三态β-羟基丙醛的分解途径首先经过一个氢迁移六元环过渡态形成双自由基中间体, 然后该中间体的分解包括两条相互竞争的途径, 它们各自经过一个断碳碳键的过渡态和一个氢键激-基态配合物中间体而形成两类产物, 一类为甲醛的基态和乙烯醇的激发态, 另一类为甲醛的激发态和乙烯醇的基态。激发态反应的两条通道均属于先氢迁移后断键分解的分步过程, 且反应的第二步为速控步骤。计算结果表明, 激发态反应活化位垒都比基态的低。     

N_2H体系的势能面及振动激发态的理论研究

本文采用含Davidson校正的多参考组态相互作用MRCI+Q方法以及aug-cc-pVQZ基组计算了N2H体系的基态与第一激发态近24000个从头算能量点,使用三次样条插值法构建了高精度的全域绝热势能面.基态势能面具有一个极小点以及高于极小点0.44 eV的鞍点.基于该势能面上发生的N(~4S)+NH(X~3∑~-)→H(~2S)+N_2(X~1∑_g~g)反应是一个无能垒的放热反应,放热量为6.172 eV,比过去的势能面更接近实验值(5.956 eV).基态与第一激发态势能面间存在明显的锥形交叉,说明两个态之间存在非绝热耦合.此外,采用Lanczos算法预测了基态N_2H分子的振动能级.     

碘乙烷激光裂解反应通道及产物的能量分布

用分子束和飞行时间技术测量了248 nm激光光解过程C_2H_5I→C_2H_5+I°(~2p_(1/2))和C_2H_5I→C_2H_5+I(~2p_(3/2))裂解碎片的平动能和内能分布。测得通道比I~*/I为2.37。根据实验结果, 对光解过程中电子激发态特性, 产生I(~2p_(3/2))通道的机理以及乙基自由基的振动激发作了讨论。     

Valence bond theoretical study for chemical reactivity

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He2+和He2++分子离子基态和激发态的特性研究

采用SAC/SAC-CI方法在CC-PV5Z基组下, 计算研究了He2+、He2++的基态及低激发态的分子特性, 给出了其基态和一些激发态的势能函数和光谱数据(Be、αe、ωe和ωeχe). 从群论出发推导了相应状态的离解极限；与已有实验结果的He2+(X2Σu+)相比, 计算结果令人满意. 还计算了激发态2Πu、4Σu+和4Πg的结构与光谱数据. 对于He2++, 计算的九个电子态中只有三个态(X1Σg+、1Σg+和1Σu+)属束缚态, 并得到了其光谱常数. 用价键理论模型的不相交规则对He2++基态的势能曲线极大点产生的原因做了较好的分析.     

MRD CI calculations of excited states of the SiH3 radical,including potential curves for the inversion mode and the dissociation SiH3 → SiH2 + H

Using the MRD CI method and large basis sets the vertical spectrum of silyl radical (SiH₃) has been calculated. The lowest excited state is the 4s Rydberg state, 41000 cm⁻¹ (5.2 eV) above the ground state. Only one excited valence state (2²E) was encountered, all other states are of Rydberg type. From potential curves for the inversion mode (symmetric bending motion) it was inferred that all Rydberg states are planar, whereas the valence excited state is highly pyramidalized. The investigation of the dissociation reaction SiH₃ → SiH₂ + H leads to the conclusion that the first excited state is dissociative.     

The low-lying electronic excited states of NiCO

Highly correlated coupled cluster methods with single and double excitations (CSSD) and CCSD with perturbative triple excitations were used to predict molecular structures and harmonic vibrational frequencies for the electronic ground state X 1Sigma+, and for the 3Delta, 3Sigma+, 3Phi, 1 3Pi, 2 3Pi, 1Sigma+, 1Delta, and 1Pi excited states of NiCO. The X 1Sigma+ ground state's geometry is for the first time compared with the recently determined experimental structure. The adiabatic excitation energies, vertical excitation energies, and dissociation energies of these excited states are predicted. The importance of pi and sigma bonding for the Ni-C bond is discussed based on the structures of excited states.     

Construction and applications of symmetrized valence bond wave functions

A method constructing symmetry-adapted bonded Young tableau bases is proposed, based on the symmetry properties of bonded tableaus and the projection operator associated with a point group. Several examples including the ground states and π excited states of O₃⁻, O₃, O₃⁺, and C₃⁻ are shown for instruction to construct the symmetrized valence bond (VB) wave function. Excitation energies of transitions from the ground states to π excited states of O₃⁻, C₃H₅, and C₃⁻ are calculated with an optimized symmetrized valence bond wave function in the σ–π separation approximation. Good agreement between the VB and experimental excitation energies is observed. The bonding features of the ground state and the first π excited singlet and triplet states for S₃ are discussed according to bonding populations from VB calculations. Both the singlet-biradical and the dipole structures have significant contributions to the ground state X ¹A₁ of S₃, while the excited state 1 ¹B₂ is essentially composed of the dipole structures, and the 1 ³B₂ excited state is comprised from a triplet-biradical structure. © 1998 John Wiley & Sons, Inc. Int J Quant Chem 66 : 1–7, 1998     

A microwave spectroscopic and quantum chemical study of propa-1,2-dienyl selenocyanate (H(2)==C==CHSeC[triple bond]N) and cyclopropyl selenocyanate (C(3)H(5)SeC[triple bond]N)

The microwave spectra of propa-1,2-dienyl selenocyanate, H(2)C==C==CHSeC[triple bond]N, and cyclopropyl selenocyanate, C(3)H(5)SeC[triple bond]N, are reported. The spectra of the ground and two vibrationally excited states of the (80)Se isotopologue and the spectrum of the ground state of the (78)Se isotopologue were assigned for one rotameric form of H(2)C==C[double bond, length as m-dash]CHSeC[triple bond]N. This conformer is characterized by a C-C-Se-C dihedral angle of 129(5) degrees from synperiplanar (0 degrees ) and is shown to be the global minimum of H(2)C[double bond, length as m-dash]C[double bond, length as m-dash]CHSeC[triple bond]N. The spectra of the ground and of three vibrationally excited states of the (80)Se isotopologue, as well as of the ground state of the (78)Se isotopologue of one rotamer of C(3)H(5)SeC[triple bond]N were assigned. This conformer has a H-C-Se-C dihedral angle of 80(4) degrees from synperiplanar and is at least 3 kJ mol(-1) more stable than any other form of the molecule. The microwave study has been augmented by quantum chemical calculations at the B3LYP/6-311+ +G(3df,3pd) and MP2/6-311+ +G(3df,3pd) levels of theory.     

Coupled cluster investigation on the low-lying electronic states of CuCN and CuNC and the ground state barrier to isomerization

The observation of several metal cyanides and isocyanides in interstellar space has raised much interest these molecules. Optimum molecular structures, harmonic vibrational frequencies, and dipole moments of the ground electronic states (X1Sigma+), triplet excited states, and open shell singlet excited states of CuCN and CuNC were determined using different levels of nonrelativistic and scalar relativistic (Douglas-Kroll) [Ann. Phys. 82, 89 (1979)] coupled cluster theory in conjunction with atomic natural orbital basis sets and correlation consistent basis sets. For the relativistic computations the specially contracted correlation consistent Douglas-Kroll (DK) basis sets were used. Moreover, barriers to isomerization from CuCN to CuNC were computed. The predicted structures of the X1Sigma+ state for CuCN are re(Cu-C)=1.826 A and re(C-N)=1.167 A, at the most sophisticated level of theory, the scalar relativistic DK-CCSD(T)/cc-pVQZ(DK) method. These results are in excellent agreement with the experimentally determined Cu-C bond length of 1.829 A and C-N bond distance of 1.162 A. At the same level of theory, the zero-point corrected barrier to isomerization from CuCN to CuNC is estimated to be 14.7 kcal mol(-1), and the cyanide is more stable than the isocyanide by 11.5 kcal mol(-1). For both CuCN and CuNC the 3Sigma+ state is the lowest lying excited electronic state. At the DK-CCSD/cc-pVQZ(DK) level of theory, the energetic ordering of excited states of CuCN and CuNC is X1Sigma+相似文献