H_2CCC光谱性质的从头算研究

采用全活化空间自洽场方法(CASSCF)在C2v对称性和ANO-S基组水平下, 研究了H2CCC自由基及其阴阳离子的基态和低激发态性质. 为了进一步考虑动态电子相关效应, 采用多组态二级微扰理论(CASPT2)获得了更加精确的能量值. 计算得到X1A1 → 1A2, X1A1 → 1B1和X1A1 → 21A1在159.0, 216.5和476.4 kJ/mol处的激发可分别归因于π(b2)→π*(b1), n(a1)→π*(b1)和π(b1)→π*(b1)的跃迁, 理论波长与紫外吸收光谱得到的实验数据一致. 计算得到的电子亲和势与实验值也非常接近.     

多组态二级微扰理论计算CH3O2激发光谱以及CH3O2→CH3＋O2解离反应

在C_s对称性和aug-cc-pVTZ基组水平下, 采用全活化空间自洽场方法(CASSCF)研究了CH₃O₂自由基基态及其阴阳离子的12个低激发态. 为了进一步考虑动态电子相关效应, 采用二级多组态微扰理论(CASPT2)获得更加精确的能量值. 所有计算得到的电子态都是价电子态, 而且所得绝热激发能和电子亲和势与实验值非常接近.在CASPT2//CASSCF理论水平下计算了CH₃O₂从²A\"和²A'电子态的CH₃O₂→CH₃＋O₂的解离反应的势能曲线(PECs). 优化得到的裂解产物的几何结构和能量与分别优化CH₃和O₂得到的结果进行比较, 从而确定裂解产物的电子态. 结果表明, 从²A\"和²A'电子态的解离反应分别对应产物CH₃(²A\")＋O₂(³A\")和CH₃(²A\")＋O₂(¹A\").     

基于组态的多参考态二级微扰理论

考察了各种基于组态的多参考态二阶微扰理论方法, 提出了一个新的避免出现 Intruder 态的方法, 并完成了各种方案的程序化. 通过实例计算, 考察了这些方案的可行性及其效率,并通过BH分子的势能曲线的计算说明了多参考态方法的重要性.     

卤代氰基卡宾自由基XCCN(X=F,Cl,Br)的理论研究

在C_s对称性和ANO-S基组下, 使用全活化空间自洽场方法(CASSCF), 研究了卤代氰基卡宾自由基及其阴离子的低能电子激发态性质. 为了进一步考虑电子的动态相关效应,采用多组态二级微扰理论(CASPT2)获得更加精确的能量值. 计算结果表明, XCCN的基态是三重态. 单重态和三重态的能隙差ΔE_S-T(kJ/mol): 7.4(FCCN)<13.4(ClCCN)<16.6(BrCCN). 计算得到, XCCN(X=F, Cl, Br)最低垂直激发能分别为408.3, 385.4和 345.2 kJ/mol, 这归因于π(a′) →n_xy 的电子跃迁; XCCN的电子亲和势分别为235.7, 233.0和 237.2 kJ/mol, 与HCCN相比, 其电子亲和势变大.     

氰基铝(AlCN)及其阴阳离子低能激发态的理论研究

在C2v对称性下,采用全活化空间自洽场(CASSCF)和多组态二级微扰理论(CASPT2)方法研究氰基铝(AlCN)及其阴阳离子的基态和低能激发态.在ANO-L基组水平下,计算了AlCN及其阴阳离子低能电子态的几何,组态及其相互作用系数,谐振频率,绝热激发能,垂直激发能和振子强度.在CASSCF/CASPT2理论水平下,计算得到AlCN的11Π电子态的绝热激发能为352.4kJ·mol-1,与实验值344.0kJ·mol-1符合得很好.另外,预测AlCN的跃迁X1Σ+→21Π发生在673.1kJ·mol-1.激发能和振子强度的计算为研究AlCN的吸收光谱提供理论指导.     

C6H5C2H4Co(salen)H2O的晶体结构和性质研究

合成了标题配合物Ｃ６Ｈ５Ｃ２Ｈ４ＣＯ（ｓａｌｅｎ）Ｈ２Ｏ,并经元素分析、红外、紫外－可见光谱、差热－热重分析和循环伏安法表征．测定了晶体结构,其中轴向的Ｃｏ—Ｃ和Ｃｏ－Ｏ键长分别为１．９６２（１４）和２．２０９（９）Ａ,其Ｃｏ—Ｃ键是目前ＲＣｏ（ｓａｌｅｎ）Ｈ２Ｏ中最短的,晶体属四方晶系,空间点群为Ｐ－４２（１）Ｃ,品胞参数如下：ａ＝２４．７８９（９）,ｂ＝２４．７８９（９）,ｃ＝７．０６０（７）Ａ,β＝９０．００°,Ｖ＝４３３８．９Ａ３,Ｚ＝８．     

二元体系C6H6-DMF在293.15 K下的体积性质

利用Anton Paar DMA4500振动管密度计, 测量了293.15 K时二元体系C6H6-DMF(苯-N,N-二甲基甲酰胺)溶液的密度, 利用最小二乘法确立了溶液密度与组成的函数关系. 利用密度数据分别计算了二元体系中C6H6和DMF的表观摩尔体积, 并利用非线性最小二乘拟合法, 分别拟合得到了优化的C6H6和DMF的表观摩尔体积和摩尔分数的函数关系, 以及C6H6和DMF的表观摩尔体积和质量分数的函数关系. 通过对函数关系的极限运算得到了C6H6和DMF的标准偏摩尔体积和摩尔体积. 此外, 还计算了不同组分下体系的超额摩尔体积, 数据可用四参数Redlich-Kister方程很好地关联拟合, 得到方程系数及体系的超额摩尔体积极值位置.     

基于完全活性空间自洽场的杂化多组态密度泛函方法λ-DFCAS

提出了一种杂化多组态密度泛函新方法——λ-DFCAS. 在λ-DFCAS方法中, 电子相关能被分为静态和动态相关能. 静态相关能由多组态波函数方法完全活性空间自洽场(CASSCF)得到, 而动态相关能由密度泛函理论方法描述. 两种相关能的杂化比例由一个可调节的参数λ控制. 参数λ的取值取决于分子体系的多组态特性, 在0~1之间变化, 从而使得λ-DFCAS可以应用于各种强相关分子体系. 该方法能够以与CASSCF相当的计算代价获得接近完全活性空间二阶微扰(CASPT2)的计算精度, 并具备了大小一致性.     

双核铜配合物[Cu2(C6H5COO)4(C9H7N)2]·2H2O

本文首次利用铜粉和过氧化苯甲酰的氧化加成反应,在喹啉存在下合成了新的双核铜配合物［Ｃｕ２（Ｃ６Ｈ５ＣＯＯ）４（Ｃ９Ｈ７Ｎ）２］·２Ｈ２Ｏ．配合物进行了元素分析、摩尔电导、热重分析、红外光谱、电化学等测试;并经Ｘ－射线单晶结构分析;确定了配合物的结构．配合物属正交晶系,空间群Ｐｂｃａ,ａ＝１９．８７９（２）Ａ,ｂ＝１６．９８２（５）Ａ,ｃ＝１１．６００（４）Ａ,α＝β＝γ＝９０°,Ｖ＝３９１６Ａ３,Ｚ＝４,Ｄ＝１．４７５ｇ·ｃｍ（－３）,Ｒ＝０．０２５９９,Ｒｗ＝０．０２８８５．     

MO_2分子基态的全活化空间多组态自洽场研究(英文)

近些年来，对过渡金属簇，特别是二聚物的电子结构及光谱性质的研究已成为化学家们非常关心的一个课题，因为这方面的研究能使人们对过渡金属多重键的本质及d轨道在成键中的作用有一个深入的了解和认识．这无论是对配位化学，还是对于材料科学，都有着十分重要的意义．采用全活化空间多组态自洽场方法，对Mo2分子基态的电子结构、光谱性质及势能曲线进行了相对论有效势从头算研究，得出了较为合理的结果,根据计算预测Mo─Mo多重键的键级为4．95．     

Relativistic atomic natural orbital type basis sets for the alkaline and alkaline-earth atoms applied to the ground-state potentials for the corresponding dimers

New basis sets of the atomic natural orbital (ANO) type have been developed for the atoms Li–Fr and Be–Ra. The ANOs have been obtained from the average density matrix of the ground states and the lowest excited states of the atom, the positive ion, and the dimer at its equilibirium geometry. Scalar realtivisitc effects are included through the use of a Douglas–Kroll Hamiltonian. Multiconfigurational wave functions have been used with dynamic correlation included using second-order perturbation theory (CASSCF/CASPT2). The basis sets are applied in calculations of the ground-state potentials for the dimers. Computed bond energies are accurate to within 0.05 eV for the alkaline dimers and 0.02 eV for the alkaline-earth dimers (except for Be₂).Acknowledgments.ensp;B.O.R. would like to express his gratitude to Prof. Jacopo Tomasi for all the inspiration that his scientific work has given him through the years and continues to do in particular through the work on solvent effects on molecular properties. This work has been supported by a grant from the Swedish Science Research Council, VR.Contribution to the Jacopo Tomasi Honorary Issue     

The electronic spectrum of VCr

The electronic spectrum of VCr has been studied using the complete-active-space self-consistent field complete-active-space second-order perturbation theory approach. Potential-energy curves for 12 electronic states have been computed. Transition energies, with respect to the X² ground state, for some of the calculated electronic states are (with possible experimental values within parentheses) 0.53 eV (0.56) for A²⁺, 1.03 eV (1.14) for A⁴, 1.20 eV (1.14) for B², 1.45 eV (1.51) for B⁴, 1.60 eV (1.51, 1.78) for C², and 1.61 eV (1.63) for A^4–. AcknowledgementsThe research reported in this communication was supported by a grant from the Swedish Natural Science Research Council (NFR). S. Alex and D.G. Leopold are acknowledged for providing results from their negative ion photoelectron spectroscopy on VCr.Contribution to Björn Roos Honorary Issue     

Theoretical characterization of the absorption spectra of phenanthrene and its radical cation

The vertical absorption spectra of phenanthrene and its radical cation have been studied theoretically by means of a multiconfigurational second-order perturbation approach. Singlet-singlet transition energies and oscillator strengths, and singlet-triplet excitation energies have been studied in the absorption spectrum of phenanthrene up to 6 eV. The absorption spectrum of the pehnanthrene radical cation has been computed up to 3.4 eV. The results obtained confirm previous assignments and also lead to new interpretations of the main features of the spectra of these systems.     

Semiclassical self-consistent field perturbation theory for the hydrogen atom in a magnetic field

A recently developed perturbation theory for solving self-consistent field equations is applied to the hydrogen atom in a strong magnetic field. This system has been extensively studied using other methods and is therefore a good test case for the new method. The perturbation theory yields summable large-order expansions. The accuracy of the self-consistent field approximation varies according to field strength and quantum state but is often higher than the accuracy from adiabatic approximations. A new derivation is presented for the asymptotic adiabatic approximation, the most useful of the adiabatic approaches. This derivation uses semiclassical perturbation theory without invoking an adiabatic hypothesis. © 1998 John Wiley & Sons, Inc. Int J Quant Chem 69: 183–192, 1998     

芳香酮、酚、胺、羧酸及含氮杂环的解离常数与其π电子分布的关系

本文用微扰分子轨道(PMO),Hackel分子轨道(HMO)和自洽场分子轨道(PPP)方法研究了芳香酮、芳香胺、酚和含氮杂环等化合物的解离常数(pK_α)和π-电子分布的关系。结果表明对交替烃,PMO,HMO和PPP在某些情况下,有类似的平行结果。pK_α与活性原子上的电荷密度q_w有着良好的线性关系。但对芳香甲酸和含氮杂环,pK_α与q_x有反比关系。对芳香甲酸pK_α主要由偶极矩决定。而含氮杂环主要由氮原子中的孤对电子与最高充满轨道中的电子间的排斥积分所控制。